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--- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/physics/continuum_mechanics/__pycache__/beam.cpython-310.pyc @@ -0,0 +1,3 @@ +version https://git-lfs.github.com/spec/v1 +oid sha256:0edd50d6210aa3e13cb2258869ebbfafd4c02b119609793f8d98dca1dd19c598 +size 122349 diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/__init__.py b/mgm/lib/python3.10/site-packages/sympy/unify/__init__.py new file mode 100644 index 0000000000000000000000000000000000000000..5c166f9163785f4aa5744324eb817bef79b33525 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/unify/__init__.py @@ -0,0 +1,15 @@ +""" Unification in SymPy + +See sympy.unify.core docstring for algorithmic details + +See http://matthewrocklin.com/blog/work/2012/11/01/Unification/ for discussion +""" + +from .usympy import unify, rebuild +from .rewrite import rewriterule + +__all__ = [ + 'unify', 'rebuild', + + 'rewriterule', +] diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/__pycache__/__init__.cpython-310.pyc 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Approach by Stuart Russel and Peter Norvig +Second edition, section 9.2, page 276 + +It is modified in the following ways: + +1. We allow associative and commutative Compound expressions. This results in + combinatorial blowup. +2. We explore the tree lazily. +3. We provide generic interfaces to symbolic algebra libraries in Python. + +A more traditional version can be found here +http://aima.cs.berkeley.edu/python/logic.html +""" + +from sympy.utilities.iterables import kbins + +class Compound: + """ A little class to represent an interior node in the tree + + This is analogous to SymPy.Basic for non-Atoms + """ + def __init__(self, op, args): + self.op = op + self.args = args + + def __eq__(self, other): + return (type(self) is type(other) and self.op == other.op and + self.args == other.args) + + def __hash__(self): + return hash((type(self), self.op, self.args)) + + def __str__(self): + return "%s[%s]" % (str(self.op), ', '.join(map(str, self.args))) + +class Variable: + """ A Wild token """ + def __init__(self, arg): + self.arg = arg + + def __eq__(self, other): + return type(self) is type(other) and self.arg == other.arg + + def __hash__(self): + return hash((type(self), self.arg)) + + def __str__(self): + return "Variable(%s)" % str(self.arg) + +class CondVariable: + """ A wild token that matches conditionally. + + arg - a wild token. + valid - an additional constraining function on a match. + """ + def __init__(self, arg, valid): + self.arg = arg + self.valid = valid + + def __eq__(self, other): + return (type(self) is type(other) and + self.arg == other.arg and + self.valid == other.valid) + + def __hash__(self): + return hash((type(self), self.arg, self.valid)) + + def __str__(self): + return "CondVariable(%s)" % str(self.arg) + +def unify(x, y, s=None, **fns): + """ Unify two expressions. + + Parameters + ========== + + x, y - expression trees containing leaves, Compounds and Variables. + s - a mapping of variables to subtrees. + + Returns + ======= + + lazy sequence of mappings {Variable: subtree} + + Examples + ======== + + >>> from sympy.unify.core import unify, Compound, Variable + >>> expr = Compound("Add", ("x", "y")) + >>> pattern = Compound("Add", ("x", Variable("a"))) + >>> next(unify(expr, pattern, {})) + {Variable(a): 'y'} + """ + s = s or {} + + if x == y: + yield s + elif isinstance(x, (Variable, CondVariable)): + yield from unify_var(x, y, s, **fns) + elif isinstance(y, (Variable, CondVariable)): + yield from unify_var(y, x, s, **fns) + elif isinstance(x, Compound) and isinstance(y, Compound): + is_commutative = fns.get('is_commutative', lambda x: False) + is_associative = fns.get('is_associative', lambda x: False) + for sop in unify(x.op, y.op, s, **fns): + if is_associative(x) and is_associative(y): + a, b = (x, y) if len(x.args) < len(y.args) else (y, x) + if is_commutative(x) and is_commutative(y): + combs = allcombinations(a.args, b.args, 'commutative') + else: + combs = allcombinations(a.args, b.args, 'associative') + for aaargs, bbargs in combs: + aa = [unpack(Compound(a.op, arg)) for arg in aaargs] + bb = [unpack(Compound(b.op, arg)) for arg in bbargs] + yield from unify(aa, bb, sop, **fns) + elif len(x.args) == len(y.args): + yield from unify(x.args, y.args, sop, **fns) + + elif is_args(x) and is_args(y) and len(x) == len(y): + if len(x) == 0: + yield s + else: + for shead in unify(x[0], y[0], s, **fns): + yield from unify(x[1:], y[1:], shead, **fns) + +def unify_var(var, x, s, **fns): + if var in s: + yield from unify(s[var], x, s, **fns) + elif occur_check(var, x): + pass + elif isinstance(var, CondVariable) and var.valid(x): + yield assoc(s, var, x) + elif isinstance(var, Variable): + yield assoc(s, var, x) + +def occur_check(var, x): + """ var occurs in subtree owned by x? """ + if var == x: + return True + elif isinstance(x, Compound): + return occur_check(var, x.args) + elif is_args(x): + if any(occur_check(var, xi) for xi in x): return True + return False + +def assoc(d, key, val): + """ Return copy of d with key associated to val """ + d = d.copy() + d[key] = val + return d + +def is_args(x): + """ Is x a traditional iterable? """ + return type(x) in (tuple, list, set) + +def unpack(x): + if isinstance(x, Compound) and len(x.args) == 1: + return x.args[0] + else: + return x + +def allcombinations(A, B, ordered): + """ + Restructure A and B to have the same number of elements. + + Parameters + ========== + + ordered must be either 'commutative' or 'associative'. + + A and B can be rearranged so that the larger of the two lists is + reorganized into smaller sublists. + + Examples + ======== + + >>> from sympy.unify.core import allcombinations + >>> for x in allcombinations((1, 2, 3), (5, 6), 'associative'): print(x) + (((1,), (2, 3)), ((5,), (6,))) + (((1, 2), (3,)), ((5,), (6,))) + + >>> for x in allcombinations((1, 2, 3), (5, 6), 'commutative'): print(x) + (((1,), (2, 3)), ((5,), (6,))) + (((1, 2), (3,)), ((5,), (6,))) + (((1,), (3, 2)), ((5,), (6,))) + (((1, 3), (2,)), ((5,), (6,))) + (((2,), (1, 3)), ((5,), (6,))) + (((2, 1), (3,)), ((5,), (6,))) + (((2,), (3, 1)), ((5,), (6,))) + (((2, 3), (1,)), ((5,), (6,))) + (((3,), (1, 2)), ((5,), (6,))) + (((3, 1), (2,)), ((5,), (6,))) + (((3,), (2, 1)), ((5,), (6,))) + (((3, 2), (1,)), ((5,), (6,))) + """ + + if ordered == "commutative": + ordered = 11 + if ordered == "associative": + ordered = None + sm, bg = (A, B) if len(A) < len(B) else (B, A) + for part in kbins(list(range(len(bg))), len(sm), ordered=ordered): + if bg == B: + yield tuple((a,) for a in A), partition(B, part) + else: + yield partition(A, part), tuple((b,) for b in B) + +def partition(it, part): + """ Partition a tuple/list into pieces defined by indices. + + Examples + ======== + + >>> from sympy.unify.core import partition + >>> partition((10, 20, 30, 40), [[0, 1, 2], [3]]) + ((10, 20, 30), (40,)) + """ + return type(it)([index(it, ind) for ind in part]) + +def index(it, ind): + """ Fancy indexing into an indexable iterable (tuple, list). + + Examples + ======== + + >>> from sympy.unify.core import index + >>> index([10, 20, 30], (1, 2, 0)) + [20, 30, 10] + """ + return type(it)([it[i] for i in ind]) diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/rewrite.py b/mgm/lib/python3.10/site-packages/sympy/unify/rewrite.py new file mode 100644 index 0000000000000000000000000000000000000000..95a6fa5ffd6a3fde94d17ee845c03bb2b44cf009 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/unify/rewrite.py @@ -0,0 +1,55 @@ +""" Functions to support rewriting of SymPy expressions """ + +from sympy.core.expr import Expr +from sympy.assumptions import ask +from sympy.strategies.tools import subs +from sympy.unify.usympy import rebuild, unify + +def rewriterule(source, target, variables=(), condition=None, assume=None): + """ Rewrite rule. + + Transform expressions that match source into expressions that match target + treating all ``variables`` as wilds. + + Examples + ======== + + >>> from sympy.abc import w, x, y, z + >>> from sympy.unify.rewrite import rewriterule + >>> from sympy import default_sort_key + >>> rl = rewriterule(x + y, x**y, [x, y]) + >>> sorted(rl(z + 3), key=default_sort_key) + [3**z, z**3] + + Use ``condition`` to specify additional requirements. Inputs are taken in + the same order as is found in variables. + + >>> rl = rewriterule(x + y, x**y, [x, y], lambda x, y: x.is_integer) + >>> list(rl(z + 3)) + [3**z] + + Use ``assume`` to specify additional requirements using new assumptions. + + >>> from sympy.assumptions import Q + >>> rl = rewriterule(x + y, x**y, [x, y], assume=Q.integer(x)) + >>> list(rl(z + 3)) + [3**z] + + Assumptions for the local context are provided at rule runtime + + >>> list(rl(w + z, Q.integer(z))) + [z**w] + """ + + def rewrite_rl(expr, assumptions=True): + for match in unify(source, expr, {}, variables=variables): + if (condition and + not condition(*[match.get(var, var) for var in variables])): + continue + if (assume and not ask(assume.xreplace(match), assumptions)): + continue + expr2 = subs(match)(target) + if isinstance(expr2, Expr): + expr2 = rebuild(expr2) + yield expr2 + return rewrite_rl diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/tests/__init__.py 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a/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_rewrite.py b/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_rewrite.py new file mode 100644 index 0000000000000000000000000000000000000000..7b73e2856d5f6380c576220fa2780324df98091a --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_rewrite.py @@ -0,0 +1,74 @@ +from sympy.unify.rewrite import rewriterule +from sympy.core.basic import Basic +from sympy.core.singleton import S +from sympy.core.symbol import Symbol +from sympy.functions.elementary.trigonometric import sin +from sympy.abc import x, y +from sympy.strategies.rl import rebuild +from sympy.assumptions import Q + +p, q = Symbol('p'), Symbol('q') + +def test_simple(): + rl = rewriterule(Basic(p, S(1)), Basic(p, S(2)), variables=(p,)) + assert list(rl(Basic(S(3), S(1)))) == [Basic(S(3), S(2))] + + p1 = p**2 + p2 = p**3 + rl = rewriterule(p1, p2, variables=(p,)) + + expr = x**2 + assert list(rl(expr)) == [x**3] + +def test_simple_variables(): + rl = rewriterule(Basic(x, S(1)), Basic(x, S(2)), variables=(x,)) + assert list(rl(Basic(S(3), S(1)))) == [Basic(S(3), S(2))] + + rl = rewriterule(x**2, x**3, variables=(x,)) + assert list(rl(y**2)) == [y**3] + +def test_moderate(): + p1 = p**2 + q**3 + p2 = (p*q)**4 + rl = rewriterule(p1, p2, (p, q)) + + expr = x**2 + y**3 + assert list(rl(expr)) == [(x*y)**4] + +def test_sincos(): + p1 = sin(p)**2 + sin(p)**2 + p2 = 1 + rl = rewriterule(p1, p2, (p, q)) + + assert list(rl(sin(x)**2 + sin(x)**2)) == [1] + assert list(rl(sin(y)**2 + sin(y)**2)) == [1] + +def test_Exprs_ok(): + rl = rewriterule(p+q, q+p, (p, q)) + next(rl(x+y)).is_commutative + str(next(rl(x+y))) + +def test_condition_simple(): + rl = rewriterule(x, x+1, [x], lambda x: x < 10) + assert not list(rl(S(15))) + assert rebuild(next(rl(S(5)))) == 6 + + +def test_condition_multiple(): + rl = rewriterule(x + y, x**y, [x,y], lambda x, y: x.is_integer) + + a = Symbol('a') + b = Symbol('b', integer=True) + expr = a + b + assert list(rl(expr)) == [b**a] + + c = Symbol('c', integer=True) + d = Symbol('d', integer=True) + assert set(rl(c + d)) == {c**d, d**c} + +def test_assumptions(): + rl = rewriterule(x + y, x**y, [x, y], assume=Q.integer(x)) + + a, b = map(Symbol, 'ab') + expr = a + b + assert list(rl(expr, Q.integer(b))) == [b**a] diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_sympy.py b/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_sympy.py new file mode 100644 index 0000000000000000000000000000000000000000..eca3933a91abfabdbad96f626e4da761a41b3fd2 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_sympy.py @@ -0,0 +1,162 @@ +from sympy.core.add import Add +from sympy.core.basic import Basic +from sympy.core.containers import Tuple +from sympy.core.singleton import S +from sympy.core.symbol import (Symbol, symbols) +from sympy.logic.boolalg import And +from sympy.core.symbol import Str +from sympy.unify.core import Compound, Variable +from sympy.unify.usympy import (deconstruct, construct, unify, is_associative, + is_commutative) +from sympy.abc import x, y, z, n + +def test_deconstruct(): + expr = Basic(S(1), S(2), S(3)) + expected = Compound(Basic, (1, 2, 3)) + assert deconstruct(expr) == expected + + assert deconstruct(1) == 1 + assert deconstruct(x) == x + assert deconstruct(x, variables=(x,)) == Variable(x) + assert deconstruct(Add(1, x, evaluate=False)) == Compound(Add, (1, x)) + assert deconstruct(Add(1, x, evaluate=False), variables=(x,)) == \ + Compound(Add, (1, Variable(x))) + +def test_construct(): + expr = Compound(Basic, (S(1), S(2), S(3))) + expected = Basic(S(1), S(2), S(3)) + assert construct(expr) == expected + +def test_nested(): + expr = Basic(S(1), Basic(S(2)), S(3)) + cmpd = Compound(Basic, (S(1), Compound(Basic, Tuple(2)), S(3))) + assert deconstruct(expr) == cmpd + assert construct(cmpd) == expr + +def test_unify(): + expr = Basic(S(1), S(2), S(3)) + a, b, c = map(Symbol, 'abc') + pattern = Basic(a, b, c) + assert list(unify(expr, pattern, {}, (a, b, c))) == [{a: 1, b: 2, c: 3}] + assert list(unify(expr, pattern, variables=(a, b, c))) == \ + [{a: 1, b: 2, c: 3}] + +def test_unify_variables(): + assert list(unify(Basic(S(1), S(2)), Basic(S(1), x), {}, variables=(x,))) == [{x: 2}] + +def test_s_input(): + expr = Basic(S(1), S(2)) + a, b = map(Symbol, 'ab') + pattern = Basic(a, b) + assert list(unify(expr, pattern, {}, (a, b))) == [{a: 1, b: 2}] + assert list(unify(expr, pattern, {a: 5}, (a, b))) == [] + +def iterdicteq(a, b): + a = tuple(a) + b = tuple(b) + return len(a) == len(b) and all(x in b for x in a) + +def test_unify_commutative(): + expr = Add(1, 2, 3, evaluate=False) + a, b, c = map(Symbol, 'abc') + pattern = Add(a, b, c, evaluate=False) + + result = tuple(unify(expr, pattern, {}, (a, b, c))) + expected = ({a: 1, b: 2, c: 3}, + {a: 1, b: 3, c: 2}, + {a: 2, b: 1, c: 3}, + {a: 2, b: 3, c: 1}, + {a: 3, b: 1, c: 2}, + {a: 3, b: 2, c: 1}) + + assert iterdicteq(result, expected) + +def test_unify_iter(): + expr = Add(1, 2, 3, evaluate=False) + a, b, c = map(Symbol, 'abc') + pattern = Add(a, c, evaluate=False) + assert is_associative(deconstruct(pattern)) + assert is_commutative(deconstruct(pattern)) + + result = list(unify(expr, pattern, {}, (a, c))) + expected = [{a: 1, c: Add(2, 3, evaluate=False)}, + {a: 1, c: Add(3, 2, evaluate=False)}, + {a: 2, c: Add(1, 3, evaluate=False)}, + {a: 2, c: Add(3, 1, evaluate=False)}, + {a: 3, c: Add(1, 2, evaluate=False)}, + {a: 3, c: Add(2, 1, evaluate=False)}, + {a: Add(1, 2, evaluate=False), c: 3}, + {a: Add(2, 1, evaluate=False), c: 3}, + {a: Add(1, 3, evaluate=False), c: 2}, + {a: Add(3, 1, evaluate=False), c: 2}, + {a: Add(2, 3, evaluate=False), c: 1}, + {a: Add(3, 2, evaluate=False), c: 1}] + + assert iterdicteq(result, expected) + +def test_hard_match(): + from sympy.functions.elementary.trigonometric import (cos, sin) + expr = sin(x) + cos(x)**2 + p, q = map(Symbol, 'pq') + pattern = sin(p) + cos(p)**2 + assert list(unify(expr, pattern, {}, (p, q))) == [{p: x}] + +def test_matrix(): + from sympy.matrices.expressions.matexpr import MatrixSymbol + X = MatrixSymbol('X', n, n) + Y = MatrixSymbol('Y', 2, 2) + Z = MatrixSymbol('Z', 2, 3) + assert list(unify(X, Y, {}, variables=[n, Str('X')])) == [{Str('X'): Str('Y'), n: 2}] + assert list(unify(X, Z, {}, variables=[n, Str('X')])) == [] + +def test_non_frankenAdds(): + # the is_commutative property used to fail because of Basic.__new__ + # This caused is_commutative and str calls to fail + expr = x+y*2 + rebuilt = construct(deconstruct(expr)) + # Ensure that we can run these commands without causing an error + str(rebuilt) + rebuilt.is_commutative + +def test_FiniteSet_commutivity(): + from sympy.sets.sets import FiniteSet + a, b, c, x, y = symbols('a,b,c,x,y') + s = FiniteSet(a, b, c) + t = FiniteSet(x, y) + variables = (x, y) + assert {x: FiniteSet(a, c), y: b} in tuple(unify(s, t, variables=variables)) + +def test_FiniteSet_complex(): + from sympy.sets.sets import FiniteSet + a, b, c, x, y, z = symbols('a,b,c,x,y,z') + expr = FiniteSet(Basic(S(1), x), y, Basic(x, z)) + pattern = FiniteSet(a, Basic(x, b)) + variables = a, b + expected = ({b: 1, a: FiniteSet(y, Basic(x, z))}, + {b: z, a: FiniteSet(y, Basic(S(1), x))}) + assert iterdicteq(unify(expr, pattern, variables=variables), expected) + + +def test_and(): + variables = x, y + expected = ({x: z > 0, y: n < 3},) + assert iterdicteq(unify((z>0) & (n<3), And(x, y), variables=variables), + expected) + +def test_Union(): + from sympy.sets.sets import Interval + assert list(unify(Interval(0, 1) + Interval(10, 11), + Interval(0, 1) + Interval(12, 13), + variables=(Interval(12, 13),))) + +def test_is_commutative(): + assert is_commutative(deconstruct(x+y)) + assert is_commutative(deconstruct(x*y)) + assert not is_commutative(deconstruct(x**y)) + +def test_commutative_in_commutative(): + from sympy.abc import a,b,c,d + from sympy.functions.elementary.trigonometric import (cos, sin) + eq = sin(3)*sin(4)*sin(5) + 4*cos(3)*cos(4) + pat = a*cos(b)*cos(c) + d*sin(b)*sin(c) + assert next(unify(eq, pat, variables=(a,b,c,d))) diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_unify.py b/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_unify.py new file mode 100644 index 0000000000000000000000000000000000000000..31153242576e1ff55dd3097efbc985aced5d574a --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/unify/tests/test_unify.py @@ -0,0 +1,88 @@ +from sympy.unify.core import Compound, Variable, CondVariable, allcombinations +from sympy.unify import core + +a,b,c = 'a', 'b', 'c' +w,x,y,z = map(Variable, 'wxyz') + +C = Compound + +def is_associative(x): + return isinstance(x, Compound) and (x.op in ('Add', 'Mul', 'CAdd', 'CMul')) +def is_commutative(x): + return isinstance(x, Compound) and (x.op in ('CAdd', 'CMul')) + + +def unify(a, b, s={}): + return core.unify(a, b, s=s, is_associative=is_associative, + is_commutative=is_commutative) + +def test_basic(): + assert list(unify(a, x, {})) == [{x: a}] + assert list(unify(a, x, {x: 10})) == [] + assert list(unify(1, x, {})) == [{x: 1}] + assert list(unify(a, a, {})) == [{}] + assert list(unify((w, x), (y, z), {})) == [{w: y, x: z}] + assert list(unify(x, (a, b), {})) == [{x: (a, b)}] + + assert list(unify((a, b), (x, x), {})) == [] + assert list(unify((y, z), (x, x), {}))!= [] + assert list(unify((a, (b, c)), (a, (x, y)), {})) == [{x: b, y: c}] + +def test_ops(): + assert list(unify(C('Add', (a,b,c)), C('Add', (a,x,y)), {})) == \ + [{x:b, y:c}] + assert list(unify(C('Add', (C('Mul', (1,2)), b,c)), C('Add', (x,y,c)), {})) == \ + [{x: C('Mul', (1,2)), y:b}] + +def test_associative(): + c1 = C('Add', (1,2,3)) + c2 = C('Add', (x,y)) + assert tuple(unify(c1, c2, {})) == ({x: 1, y: C('Add', (2, 3))}, + {x: C('Add', (1, 2)), y: 3}) + +def test_commutative(): + c1 = C('CAdd', (1,2,3)) + c2 = C('CAdd', (x,y)) + result = list(unify(c1, c2, {})) + assert {x: 1, y: C('CAdd', (2, 3))} in result + assert ({x: 2, y: C('CAdd', (1, 3))} in result or + {x: 2, y: C('CAdd', (3, 1))} in result) + +def _test_combinations_assoc(): + assert set(allcombinations((1,2,3), (a,b), True)) == \ + {(((1, 2), (3,)), (a, b)), (((1,), (2, 3)), (a, b))} + +def _test_combinations_comm(): + assert set(allcombinations((1,2,3), (a,b), None)) == \ + {(((1,), (2, 3)), ('a', 'b')), (((2,), (3, 1)), ('a', 'b')), + (((3,), (1, 2)), ('a', 'b')), (((1, 2), (3,)), ('a', 'b')), + (((2, 3), (1,)), ('a', 'b')), (((3, 1), (2,)), ('a', 'b'))} + +def test_allcombinations(): + assert set(allcombinations((1,2), (1,2), 'commutative')) ==\ + {(((1,),(2,)), ((1,),(2,))), (((1,),(2,)), ((2,),(1,)))} + + +def test_commutativity(): + c1 = Compound('CAdd', (a, b)) + c2 = Compound('CAdd', (x, y)) + assert is_commutative(c1) and is_commutative(c2) + assert len(list(unify(c1, c2, {}))) == 2 + + +def test_CondVariable(): + expr = C('CAdd', (1, 2)) + x = Variable('x') + y = CondVariable('y', lambda a: a % 2 == 0) + z = CondVariable('z', lambda a: a > 3) + pattern = C('CAdd', (x, y)) + assert list(unify(expr, pattern, {})) == \ + [{x: 1, y: 2}] + + z = CondVariable('z', lambda a: a > 3) + pattern = C('CAdd', (z, y)) + + assert list(unify(expr, pattern, {})) == [] + +def test_defaultdict(): + assert next(unify(Variable('x'), 'foo')) == {Variable('x'): 'foo'} diff --git a/mgm/lib/python3.10/site-packages/sympy/unify/usympy.py b/mgm/lib/python3.10/site-packages/sympy/unify/usympy.py new file mode 100644 index 0000000000000000000000000000000000000000..3942b35ec549e5dbd08a3cf1cad2b2ecea733c7a --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/unify/usympy.py @@ -0,0 +1,124 @@ +""" SymPy interface to Unification engine + +See sympy.unify for module level docstring +See sympy.unify.core for algorithmic docstring """ + +from sympy.core import Basic, Add, Mul, Pow +from sympy.core.operations import AssocOp, LatticeOp +from sympy.matrices import MatAdd, MatMul, MatrixExpr +from sympy.sets.sets import Union, Intersection, FiniteSet +from sympy.unify.core import Compound, Variable, CondVariable +from sympy.unify import core + +basic_new_legal = [MatrixExpr] +eval_false_legal = [AssocOp, Pow, FiniteSet] +illegal = [LatticeOp] + +def sympy_associative(op): + assoc_ops = (AssocOp, MatAdd, MatMul, Union, Intersection, FiniteSet) + return any(issubclass(op, aop) for aop in assoc_ops) + +def sympy_commutative(op): + comm_ops = (Add, MatAdd, Union, Intersection, FiniteSet) + return any(issubclass(op, cop) for cop in comm_ops) + +def is_associative(x): + return isinstance(x, Compound) and sympy_associative(x.op) + +def is_commutative(x): + if not isinstance(x, Compound): + return False + if sympy_commutative(x.op): + return True + if issubclass(x.op, Mul): + return all(construct(arg).is_commutative for arg in x.args) + +def mk_matchtype(typ): + def matchtype(x): + return (isinstance(x, typ) or + isinstance(x, Compound) and issubclass(x.op, typ)) + return matchtype + +def deconstruct(s, variables=()): + """ Turn a SymPy object into a Compound """ + if s in variables: + return Variable(s) + if isinstance(s, (Variable, CondVariable)): + return s + if not isinstance(s, Basic) or s.is_Atom: + return s + return Compound(s.__class__, + tuple(deconstruct(arg, variables) for arg in s.args)) + +def construct(t): + """ Turn a Compound into a SymPy object """ + if isinstance(t, (Variable, CondVariable)): + return t.arg + if not isinstance(t, Compound): + return t + if any(issubclass(t.op, cls) for cls in eval_false_legal): + return t.op(*map(construct, t.args), evaluate=False) + elif any(issubclass(t.op, cls) for cls in basic_new_legal): + return Basic.__new__(t.op, *map(construct, t.args)) + else: + return t.op(*map(construct, t.args)) + +def rebuild(s): + """ Rebuild a SymPy expression. + + This removes harm caused by Expr-Rules interactions. + """ + return construct(deconstruct(s)) + +def unify(x, y, s=None, variables=(), **kwargs): + """ Structural unification of two expressions/patterns. + + Examples + ======== + + >>> from sympy.unify.usympy import unify + >>> from sympy import Basic, S + >>> from sympy.abc import x, y, z, p, q + + >>> next(unify(Basic(S(1), S(2)), Basic(S(1), x), variables=[x])) + {x: 2} + + >>> expr = 2*x + y + z + >>> pattern = 2*p + q + >>> next(unify(expr, pattern, {}, variables=(p, q))) + {p: x, q: y + z} + + Unification supports commutative and associative matching + + >>> expr = x + y + z + >>> pattern = p + q + >>> len(list(unify(expr, pattern, {}, variables=(p, q)))) + 12 + + Symbols not indicated to be variables are treated as literal, + else they are wild-like and match anything in a sub-expression. + + >>> expr = x*y*z + 3 + >>> pattern = x*y + 3 + >>> next(unify(expr, pattern, {}, variables=[x, y])) + {x: y, y: x*z} + + The x and y of the pattern above were in a Mul and matched factors + in the Mul of expr. Here, a single symbol matches an entire term: + + >>> expr = x*y + 3 + >>> pattern = p + 3 + >>> next(unify(expr, pattern, {}, variables=[p])) + {p: x*y} + + """ + decons = lambda x: deconstruct(x, variables) + s = s or {} + s = {decons(k): decons(v) for k, v in s.items()} + + ds = core.unify(decons(x), decons(y), s, + is_associative=is_associative, + is_commutative=is_commutative, + **kwargs) + for d in ds: + yield {construct(k): construct(v) for k, v in d.items()} diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/__init__.py b/mgm/lib/python3.10/site-packages/sympy/vector/__init__.py new file mode 100644 index 0000000000000000000000000000000000000000..9228befbdb4bd5c940cc59983c331627eab7475c --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/__init__.py @@ -0,0 +1,47 @@ +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.vector import (Vector, VectorAdd, VectorMul, + BaseVector, VectorZero, Cross, Dot, cross, dot) +from sympy.vector.dyadic import (Dyadic, DyadicAdd, DyadicMul, + BaseDyadic, DyadicZero) +from sympy.vector.scalar import BaseScalar +from sympy.vector.deloperator import Del +from sympy.vector.functions import (express, matrix_to_vector, + laplacian, is_conservative, + is_solenoidal, scalar_potential, + directional_derivative, + scalar_potential_difference) +from sympy.vector.point import Point +from sympy.vector.orienters import (AxisOrienter, BodyOrienter, + SpaceOrienter, QuaternionOrienter) +from sympy.vector.operators import Gradient, Divergence, Curl, Laplacian, gradient, curl, divergence +from sympy.vector.implicitregion import ImplicitRegion +from sympy.vector.parametricregion import (ParametricRegion, parametric_region_list) +from sympy.vector.integrals import (ParametricIntegral, vector_integrate) + +__all__ = [ + 'Vector', 'VectorAdd', 'VectorMul', 'BaseVector', 'VectorZero', 'Cross', + 'Dot', 'cross', 'dot', + + 'Dyadic', 'DyadicAdd', 'DyadicMul', 'BaseDyadic', 'DyadicZero', + + 'BaseScalar', + + 'Del', + + 'CoordSys3D', + + 'express', 'matrix_to_vector', 'laplacian', 'is_conservative', + 'is_solenoidal', 'scalar_potential', 'directional_derivative', + 'scalar_potential_difference', + + 'Point', + + 'AxisOrienter', 'BodyOrienter', 'SpaceOrienter', 'QuaternionOrienter', + + 'Gradient', 'Divergence', 'Curl', 'Laplacian', 'gradient', 'curl', + 'divergence', + + 'ParametricRegion', 'parametric_region_list', 'ImplicitRegion', + + 'ParametricIntegral', 'vector_integrate', +] diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/basisdependent.py b/mgm/lib/python3.10/site-packages/sympy/vector/basisdependent.py new file mode 100644 index 0000000000000000000000000000000000000000..656bcd37212b468ebceb7561a03db45c593b6323 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/basisdependent.py @@ -0,0 +1,365 @@ +from __future__ import annotations +from typing import TYPE_CHECKING + +from sympy.simplify import simplify as simp, trigsimp as tsimp # type: ignore +from sympy.core.decorators import call_highest_priority, _sympifyit +from sympy.core.assumptions import StdFactKB +from sympy.core.function import diff as df +from sympy.integrals.integrals import Integral +from sympy.polys.polytools import factor as fctr +from sympy.core import S, Add, Mul +from sympy.core.expr import Expr + +if TYPE_CHECKING: + from sympy.vector.vector import BaseVector + + +class BasisDependent(Expr): + """ + Super class containing functionality common to vectors and + dyadics. + Named so because the representation of these quantities in + sympy.vector is dependent on the basis they are expressed in. + """ + + zero: BasisDependentZero + + @call_highest_priority('__radd__') + def __add__(self, other): + return self._add_func(self, other) + + @call_highest_priority('__add__') + def __radd__(self, other): + return self._add_func(other, self) + + @call_highest_priority('__rsub__') + def __sub__(self, other): + return self._add_func(self, -other) + + @call_highest_priority('__sub__') + def __rsub__(self, other): + return self._add_func(other, -self) + + @_sympifyit('other', NotImplemented) + @call_highest_priority('__rmul__') + def __mul__(self, other): + return self._mul_func(self, other) + + @_sympifyit('other', NotImplemented) + @call_highest_priority('__mul__') + def __rmul__(self, other): + return self._mul_func(other, self) + + def __neg__(self): + return self._mul_func(S.NegativeOne, self) + + @_sympifyit('other', NotImplemented) + @call_highest_priority('__rtruediv__') + def __truediv__(self, other): + return self._div_helper(other) + + @call_highest_priority('__truediv__') + def __rtruediv__(self, other): + return TypeError("Invalid divisor for division") + + def evalf(self, n=15, subs=None, maxn=100, chop=False, strict=False, quad=None, verbose=False): + """ + Implements the SymPy evalf routine for this quantity. + + evalf's documentation + ===================== + + """ + options = {'subs':subs, 'maxn':maxn, 'chop':chop, 'strict':strict, + 'quad':quad, 'verbose':verbose} + vec = self.zero + for k, v in self.components.items(): + vec += v.evalf(n, **options) * k + return vec + + evalf.__doc__ += Expr.evalf.__doc__ # type: ignore + + n = evalf + + def simplify(self, **kwargs): + """ + Implements the SymPy simplify routine for this quantity. + + simplify's documentation + ======================== + + """ + simp_components = [simp(v, **kwargs) * k for + k, v in self.components.items()] + return self._add_func(*simp_components) + + simplify.__doc__ += simp.__doc__ # type: ignore + + def trigsimp(self, **opts): + """ + Implements the SymPy trigsimp routine, for this quantity. + + trigsimp's documentation + ======================== + + """ + trig_components = [tsimp(v, **opts) * k for + k, v in self.components.items()] + return self._add_func(*trig_components) + + trigsimp.__doc__ += tsimp.__doc__ # type: ignore + + def _eval_simplify(self, **kwargs): + return self.simplify(**kwargs) + + def _eval_trigsimp(self, **opts): + return self.trigsimp(**opts) + + def _eval_derivative(self, wrt): + return self.diff(wrt) + + def _eval_Integral(self, *symbols, **assumptions): + integral_components = [Integral(v, *symbols, **assumptions) * k + for k, v in self.components.items()] + return self._add_func(*integral_components) + + def as_numer_denom(self): + """ + Returns the expression as a tuple wrt the following + transformation - + + expression -> a/b -> a, b + + """ + return self, S.One + + def factor(self, *args, **kwargs): + """ + Implements the SymPy factor routine, on the scalar parts + of a basis-dependent expression. + + factor's documentation + ======================== + + """ + fctr_components = [fctr(v, *args, **kwargs) * k for + k, v in self.components.items()] + return self._add_func(*fctr_components) + + factor.__doc__ += fctr.__doc__ # type: ignore + + def as_coeff_Mul(self, rational=False): + """Efficiently extract the coefficient of a product.""" + return (S.One, self) + + def as_coeff_add(self, *deps): + """Efficiently extract the coefficient of a summation.""" + l = [x * self.components[x] for x in self.components] + return 0, tuple(l) + + def diff(self, *args, **kwargs): + """ + Implements the SymPy diff routine, for vectors. + + diff's documentation + ======================== + + """ + for x in args: + if isinstance(x, BasisDependent): + raise TypeError("Invalid arg for differentiation") + diff_components = [df(v, *args, **kwargs) * k for + k, v in self.components.items()] + return self._add_func(*diff_components) + + diff.__doc__ += df.__doc__ # type: ignore + + def doit(self, **hints): + """Calls .doit() on each term in the Dyadic""" + doit_components = [self.components[x].doit(**hints) * x + for x in self.components] + return self._add_func(*doit_components) + + +class BasisDependentAdd(BasisDependent, Add): + """ + Denotes sum of basis dependent quantities such that they cannot + be expressed as base or Mul instances. + """ + + def __new__(cls, *args, **options): + components = {} + + # Check each arg and simultaneously learn the components + for arg in args: + if not isinstance(arg, cls._expr_type): + if isinstance(arg, Mul): + arg = cls._mul_func(*(arg.args)) + elif isinstance(arg, Add): + arg = cls._add_func(*(arg.args)) + else: + raise TypeError(str(arg) + + " cannot be interpreted correctly") + # If argument is zero, ignore + if arg == cls.zero: + continue + # Else, update components accordingly + if hasattr(arg, "components"): + for x in arg.components: + components[x] = components.get(x, 0) + arg.components[x] + + temp = list(components.keys()) + for x in temp: + if components[x] == 0: + del components[x] + + # Handle case of zero vector + if len(components) == 0: + return cls.zero + + # Build object + newargs = [x * components[x] for x in components] + obj = super().__new__(cls, *newargs, **options) + if isinstance(obj, Mul): + return cls._mul_func(*obj.args) + assumptions = {'commutative': True} + obj._assumptions = StdFactKB(assumptions) + obj._components = components + obj._sys = (list(components.keys()))[0]._sys + + return obj + + +class BasisDependentMul(BasisDependent, Mul): + """ + Denotes product of base- basis dependent quantity with a scalar. + """ + + def __new__(cls, *args, **options): + from sympy.vector import Cross, Dot, Curl, Gradient + count = 0 + measure_number = S.One + zeroflag = False + extra_args = [] + + # Determine the component and check arguments + # Also keep a count to ensure two vectors aren't + # being multiplied + for arg in args: + if isinstance(arg, cls._zero_func): + count += 1 + zeroflag = True + elif arg == S.Zero: + zeroflag = True + elif isinstance(arg, (cls._base_func, cls._mul_func)): + count += 1 + expr = arg._base_instance + measure_number *= arg._measure_number + elif isinstance(arg, cls._add_func): + count += 1 + expr = arg + elif isinstance(arg, (Cross, Dot, Curl, Gradient)): + extra_args.append(arg) + else: + measure_number *= arg + # Make sure incompatible types weren't multiplied + if count > 1: + raise ValueError("Invalid multiplication") + elif count == 0: + return Mul(*args, **options) + # Handle zero vector case + if zeroflag: + return cls.zero + + # If one of the args was a VectorAdd, return an + # appropriate VectorAdd instance + if isinstance(expr, cls._add_func): + newargs = [cls._mul_func(measure_number, x) for + x in expr.args] + return cls._add_func(*newargs) + + obj = super().__new__(cls, measure_number, + expr._base_instance, + *extra_args, + **options) + if isinstance(obj, Add): + return cls._add_func(*obj.args) + obj._base_instance = expr._base_instance + obj._measure_number = measure_number + assumptions = {'commutative': True} + obj._assumptions = StdFactKB(assumptions) + obj._components = {expr._base_instance: measure_number} + obj._sys = expr._base_instance._sys + + return obj + + def _sympystr(self, printer): + measure_str = printer._print(self._measure_number) + if ('(' in measure_str or '-' in measure_str or + '+' in measure_str): + measure_str = '(' + measure_str + ')' + return measure_str + '*' + printer._print(self._base_instance) + + +class BasisDependentZero(BasisDependent): + """ + Class to denote a zero basis dependent instance. + """ + components: dict['BaseVector', Expr] = {} + _latex_form: str + + def __new__(cls): + obj = super().__new__(cls) + # Pre-compute a specific hash value for the zero vector + # Use the same one always + obj._hash = (S.Zero, cls).__hash__() + return obj + + def __hash__(self): + return self._hash + + @call_highest_priority('__req__') + def __eq__(self, other): + return isinstance(other, self._zero_func) + + __req__ = __eq__ + + @call_highest_priority('__radd__') + def __add__(self, other): + if isinstance(other, self._expr_type): + return other + else: + raise TypeError("Invalid argument types for addition") + + @call_highest_priority('__add__') + def __radd__(self, other): + if isinstance(other, self._expr_type): + return other + else: + raise TypeError("Invalid argument types for addition") + + @call_highest_priority('__rsub__') + def __sub__(self, other): + if isinstance(other, self._expr_type): + return -other + else: + raise TypeError("Invalid argument types for subtraction") + + @call_highest_priority('__sub__') + def __rsub__(self, other): + if isinstance(other, self._expr_type): + return other + else: + raise TypeError("Invalid argument types for subtraction") + + def __neg__(self): + return self + + def normalize(self): + """ + Returns the normalized version of this vector. + """ + return self + + def _sympystr(self, printer): + return '0' diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/coordsysrect.py b/mgm/lib/python3.10/site-packages/sympy/vector/coordsysrect.py new file mode 100644 index 0000000000000000000000000000000000000000..7c6cf372f1143897a847f607abb729c997c91e8c --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/coordsysrect.py @@ -0,0 +1,1034 @@ +from collections.abc import Callable + +from sympy.core.basic import Basic +from sympy.core.cache import cacheit +from sympy.core import S, Dummy, Lambda +from sympy.core.symbol import Str +from sympy.core.symbol import symbols +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.matrices.matrixbase import MatrixBase +from sympy.solvers import solve +from sympy.vector.scalar import BaseScalar +from sympy.core.containers import Tuple +from sympy.core.function import diff +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.functions.elementary.trigonometric import (acos, atan2, cos, sin) +from sympy.matrices.dense import eye +from sympy.matrices.immutable import ImmutableDenseMatrix +from sympy.simplify.simplify import simplify +from sympy.simplify.trigsimp import trigsimp +import sympy.vector +from sympy.vector.orienters import (Orienter, AxisOrienter, BodyOrienter, + SpaceOrienter, QuaternionOrienter) + + +class CoordSys3D(Basic): + """ + Represents a coordinate system in 3-D space. + """ + + def __new__(cls, name, transformation=None, parent=None, location=None, + rotation_matrix=None, vector_names=None, variable_names=None): + """ + The orientation/location parameters are necessary if this system + is being defined at a certain orientation or location wrt another. + + Parameters + ========== + + name : str + The name of the new CoordSys3D instance. + + transformation : Lambda, Tuple, str + Transformation defined by transformation equations or chosen + from predefined ones. + + location : Vector + The position vector of the new system's origin wrt the parent + instance. + + rotation_matrix : SymPy ImmutableMatrix + The rotation matrix of the new coordinate system with respect + to the parent. In other words, the output of + new_system.rotation_matrix(parent). + + parent : CoordSys3D + The coordinate system wrt which the orientation/location + (or both) is being defined. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + """ + + name = str(name) + Vector = sympy.vector.Vector + Point = sympy.vector.Point + + if not isinstance(name, str): + raise TypeError("name should be a string") + + if transformation is not None: + if (location is not None) or (rotation_matrix is not None): + raise ValueError("specify either `transformation` or " + "`location`/`rotation_matrix`") + if isinstance(transformation, (Tuple, tuple, list)): + if isinstance(transformation[0], MatrixBase): + rotation_matrix = transformation[0] + location = transformation[1] + else: + transformation = Lambda(transformation[0], + transformation[1]) + elif isinstance(transformation, Callable): + x1, x2, x3 = symbols('x1 x2 x3', cls=Dummy) + transformation = Lambda((x1, x2, x3), + transformation(x1, x2, x3)) + elif isinstance(transformation, str): + transformation = Str(transformation) + elif isinstance(transformation, (Str, Lambda)): + pass + else: + raise TypeError("transformation: " + "wrong type {}".format(type(transformation))) + + # If orientation information has been provided, store + # the rotation matrix accordingly + if rotation_matrix is None: + rotation_matrix = ImmutableDenseMatrix(eye(3)) + else: + if not isinstance(rotation_matrix, MatrixBase): + raise TypeError("rotation_matrix should be an Immutable" + + "Matrix instance") + rotation_matrix = rotation_matrix.as_immutable() + + # If location information is not given, adjust the default + # location as Vector.zero + if parent is not None: + if not isinstance(parent, CoordSys3D): + raise TypeError("parent should be a " + + "CoordSys3D/None") + if location is None: + location = Vector.zero + else: + if not isinstance(location, Vector): + raise TypeError("location should be a Vector") + # Check that location does not contain base + # scalars + for x in location.free_symbols: + if isinstance(x, BaseScalar): + raise ValueError("location should not contain" + + " BaseScalars") + origin = parent.origin.locate_new(name + '.origin', + location) + else: + location = Vector.zero + origin = Point(name + '.origin') + + if transformation is None: + transformation = Tuple(rotation_matrix, location) + + if isinstance(transformation, Tuple): + lambda_transformation = CoordSys3D._compose_rotation_and_translation( + transformation[0], + transformation[1], + parent + ) + r, l = transformation + l = l._projections + lambda_lame = CoordSys3D._get_lame_coeff('cartesian') + lambda_inverse = lambda x, y, z: r.inv()*Matrix( + [x-l[0], y-l[1], z-l[2]]) + elif isinstance(transformation, Str): + trname = transformation.name + lambda_transformation = CoordSys3D._get_transformation_lambdas(trname) + if parent is not None: + if parent.lame_coefficients() != (S.One, S.One, S.One): + raise ValueError('Parent for pre-defined coordinate ' + 'system should be Cartesian.') + lambda_lame = CoordSys3D._get_lame_coeff(trname) + lambda_inverse = CoordSys3D._set_inv_trans_equations(trname) + elif isinstance(transformation, Lambda): + if not CoordSys3D._check_orthogonality(transformation): + raise ValueError("The transformation equation does not " + "create orthogonal coordinate system") + lambda_transformation = transformation + lambda_lame = CoordSys3D._calculate_lame_coeff(lambda_transformation) + lambda_inverse = None + else: + lambda_transformation = lambda x, y, z: transformation(x, y, z) + lambda_lame = CoordSys3D._get_lame_coeff(transformation) + lambda_inverse = None + + if variable_names is None: + if isinstance(transformation, Lambda): + variable_names = ["x1", "x2", "x3"] + elif isinstance(transformation, Str): + if transformation.name == 'spherical': + variable_names = ["r", "theta", "phi"] + elif transformation.name == 'cylindrical': + variable_names = ["r", "theta", "z"] + else: + variable_names = ["x", "y", "z"] + else: + variable_names = ["x", "y", "z"] + if vector_names is None: + vector_names = ["i", "j", "k"] + + # All systems that are defined as 'roots' are unequal, unless + # they have the same name. + # Systems defined at same orientation/position wrt the same + # 'parent' are equal, irrespective of the name. + # This is true even if the same orientation is provided via + # different methods like Axis/Body/Space/Quaternion. + # However, coincident systems may be seen as unequal if + # positioned/oriented wrt different parents, even though + # they may actually be 'coincident' wrt the root system. + if parent is not None: + obj = super().__new__( + cls, Str(name), transformation, parent) + else: + obj = super().__new__( + cls, Str(name), transformation) + obj._name = name + # Initialize the base vectors + + _check_strings('vector_names', vector_names) + vector_names = list(vector_names) + latex_vects = [(r'\mathbf{\hat{%s}_{%s}}' % (x, name)) for + x in vector_names] + pretty_vects = ['%s_%s' % (x, name) for x in vector_names] + + obj._vector_names = vector_names + + v1 = BaseVector(0, obj, pretty_vects[0], latex_vects[0]) + v2 = BaseVector(1, obj, pretty_vects[1], latex_vects[1]) + v3 = BaseVector(2, obj, pretty_vects[2], latex_vects[2]) + + obj._base_vectors = (v1, v2, v3) + + # Initialize the base scalars + + _check_strings('variable_names', vector_names) + variable_names = list(variable_names) + latex_scalars = [(r"\mathbf{{%s}_{%s}}" % (x, name)) for + x in variable_names] + pretty_scalars = ['%s_%s' % (x, name) for x in variable_names] + + obj._variable_names = variable_names + obj._vector_names = vector_names + + x1 = BaseScalar(0, obj, pretty_scalars[0], latex_scalars[0]) + x2 = BaseScalar(1, obj, pretty_scalars[1], latex_scalars[1]) + x3 = BaseScalar(2, obj, pretty_scalars[2], latex_scalars[2]) + + obj._base_scalars = (x1, x2, x3) + + obj._transformation = transformation + obj._transformation_lambda = lambda_transformation + obj._lame_coefficients = lambda_lame(x1, x2, x3) + obj._transformation_from_parent_lambda = lambda_inverse + + setattr(obj, variable_names[0], x1) + setattr(obj, variable_names[1], x2) + setattr(obj, variable_names[2], x3) + + setattr(obj, vector_names[0], v1) + setattr(obj, vector_names[1], v2) + setattr(obj, vector_names[2], v3) + + # Assign params + obj._parent = parent + if obj._parent is not None: + obj._root = obj._parent._root + else: + obj._root = obj + + obj._parent_rotation_matrix = rotation_matrix + obj._origin = origin + + # Return the instance + return obj + + def _sympystr(self, printer): + return self._name + + def __iter__(self): + return iter(self.base_vectors()) + + @staticmethod + def _check_orthogonality(equations): + """ + Helper method for _connect_to_cartesian. It checks if + set of transformation equations create orthogonal curvilinear + coordinate system + + Parameters + ========== + + equations : Lambda + Lambda of transformation equations + + """ + + x1, x2, x3 = symbols("x1, x2, x3", cls=Dummy) + equations = equations(x1, x2, x3) + v1 = Matrix([diff(equations[0], x1), + diff(equations[1], x1), diff(equations[2], x1)]) + + v2 = Matrix([diff(equations[0], x2), + diff(equations[1], x2), diff(equations[2], x2)]) + + v3 = Matrix([diff(equations[0], x3), + diff(equations[1], x3), diff(equations[2], x3)]) + + if any(simplify(i[0] + i[1] + i[2]) == 0 for i in (v1, v2, v3)): + return False + else: + if simplify(v1.dot(v2)) == 0 and simplify(v2.dot(v3)) == 0 \ + and simplify(v3.dot(v1)) == 0: + return True + else: + return False + + @staticmethod + def _set_inv_trans_equations(curv_coord_name): + """ + Store information about inverse transformation equations for + pre-defined coordinate systems. + + Parameters + ========== + + curv_coord_name : str + Name of coordinate system + + """ + if curv_coord_name == 'cartesian': + return lambda x, y, z: (x, y, z) + + if curv_coord_name == 'spherical': + return lambda x, y, z: ( + sqrt(x**2 + y**2 + z**2), + acos(z/sqrt(x**2 + y**2 + z**2)), + atan2(y, x) + ) + if curv_coord_name == 'cylindrical': + return lambda x, y, z: ( + sqrt(x**2 + y**2), + atan2(y, x), + z + ) + raise ValueError('Wrong set of parameters.' + 'Type of coordinate system is defined') + + def _calculate_inv_trans_equations(self): + """ + Helper method for set_coordinate_type. It calculates inverse + transformation equations for given transformations equations. + + """ + x1, x2, x3 = symbols("x1, x2, x3", cls=Dummy, reals=True) + x, y, z = symbols("x, y, z", cls=Dummy) + + equations = self._transformation(x1, x2, x3) + + solved = solve([equations[0] - x, + equations[1] - y, + equations[2] - z], (x1, x2, x3), dict=True)[0] + solved = solved[x1], solved[x2], solved[x3] + self._transformation_from_parent_lambda = \ + lambda x1, x2, x3: tuple(i.subs(list(zip((x, y, z), (x1, x2, x3)))) for i in solved) + + @staticmethod + def _get_lame_coeff(curv_coord_name): + """ + Store information about Lame coefficients for pre-defined + coordinate systems. + + Parameters + ========== + + curv_coord_name : str + Name of coordinate system + + """ + if isinstance(curv_coord_name, str): + if curv_coord_name == 'cartesian': + return lambda x, y, z: (S.One, S.One, S.One) + if curv_coord_name == 'spherical': + return lambda r, theta, phi: (S.One, r, r*sin(theta)) + if curv_coord_name == 'cylindrical': + return lambda r, theta, h: (S.One, r, S.One) + raise ValueError('Wrong set of parameters.' + ' Type of coordinate system is not defined') + return CoordSys3D._calculate_lame_coefficients(curv_coord_name) + + @staticmethod + def _calculate_lame_coeff(equations): + """ + It calculates Lame coefficients + for given transformations equations. + + Parameters + ========== + + equations : Lambda + Lambda of transformation equations. + + """ + return lambda x1, x2, x3: ( + sqrt(diff(equations(x1, x2, x3)[0], x1)**2 + + diff(equations(x1, x2, x3)[1], x1)**2 + + diff(equations(x1, x2, x3)[2], x1)**2), + sqrt(diff(equations(x1, x2, x3)[0], x2)**2 + + diff(equations(x1, x2, x3)[1], x2)**2 + + diff(equations(x1, x2, x3)[2], x2)**2), + sqrt(diff(equations(x1, x2, x3)[0], x3)**2 + + diff(equations(x1, x2, x3)[1], x3)**2 + + diff(equations(x1, x2, x3)[2], x3)**2) + ) + + def _inverse_rotation_matrix(self): + """ + Returns inverse rotation matrix. + """ + return simplify(self._parent_rotation_matrix**-1) + + @staticmethod + def _get_transformation_lambdas(curv_coord_name): + """ + Store information about transformation equations for pre-defined + coordinate systems. + + Parameters + ========== + + curv_coord_name : str + Name of coordinate system + + """ + if isinstance(curv_coord_name, str): + if curv_coord_name == 'cartesian': + return lambda x, y, z: (x, y, z) + if curv_coord_name == 'spherical': + return lambda r, theta, phi: ( + r*sin(theta)*cos(phi), + r*sin(theta)*sin(phi), + r*cos(theta) + ) + if curv_coord_name == 'cylindrical': + return lambda r, theta, h: ( + r*cos(theta), + r*sin(theta), + h + ) + raise ValueError('Wrong set of parameters.' + 'Type of coordinate system is defined') + + @classmethod + def _rotation_trans_equations(cls, matrix, equations): + """ + Returns the transformation equations obtained from rotation matrix. + + Parameters + ========== + + matrix : Matrix + Rotation matrix + + equations : tuple + Transformation equations + + """ + return tuple(matrix * Matrix(equations)) + + @property + def origin(self): + return self._origin + + def base_vectors(self): + return self._base_vectors + + def base_scalars(self): + return self._base_scalars + + def lame_coefficients(self): + return self._lame_coefficients + + def transformation_to_parent(self): + return self._transformation_lambda(*self.base_scalars()) + + def transformation_from_parent(self): + if self._parent is None: + raise ValueError("no parent coordinate system, use " + "`transformation_from_parent_function()`") + return self._transformation_from_parent_lambda( + *self._parent.base_scalars()) + + def transformation_from_parent_function(self): + return self._transformation_from_parent_lambda + + def rotation_matrix(self, other): + """ + Returns the direction cosine matrix(DCM), also known as the + 'rotation matrix' of this coordinate system with respect to + another system. + + If v_a is a vector defined in system 'A' (in matrix format) + and v_b is the same vector defined in system 'B', then + v_a = A.rotation_matrix(B) * v_b. + + A SymPy Matrix is returned. + + Parameters + ========== + + other : CoordSys3D + The system which the DCM is generated to. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q1 = symbols('q1') + >>> N = CoordSys3D('N') + >>> A = N.orient_new_axis('A', q1, N.i) + >>> N.rotation_matrix(A) + Matrix([ + [1, 0, 0], + [0, cos(q1), -sin(q1)], + [0, sin(q1), cos(q1)]]) + + """ + from sympy.vector.functions import _path + if not isinstance(other, CoordSys3D): + raise TypeError(str(other) + + " is not a CoordSys3D") + # Handle special cases + if other == self: + return eye(3) + elif other == self._parent: + return self._parent_rotation_matrix + elif other._parent == self: + return other._parent_rotation_matrix.T + # Else, use tree to calculate position + rootindex, path = _path(self, other) + result = eye(3) + i = -1 + for i in range(rootindex): + result *= path[i]._parent_rotation_matrix + i += 2 + while i < len(path): + result *= path[i]._parent_rotation_matrix.T + i += 1 + return result + + @cacheit + def position_wrt(self, other): + """ + Returns the position vector of the origin of this coordinate + system with respect to another Point/CoordSys3D. + + Parameters + ========== + + other : Point/CoordSys3D + If other is a Point, the position of this system's origin + wrt it is returned. If its an instance of CoordSyRect, + the position wrt its origin is returned. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> N1 = N.locate_new('N1', 10 * N.i) + >>> N.position_wrt(N1) + (-10)*N.i + + """ + return self.origin.position_wrt(other) + + def scalar_map(self, other): + """ + Returns a dictionary which expresses the coordinate variables + (base scalars) of this frame in terms of the variables of + otherframe. + + Parameters + ========== + + otherframe : CoordSys3D + The other system to map the variables to. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import Symbol + >>> A = CoordSys3D('A') + >>> q = Symbol('q') + >>> B = A.orient_new_axis('B', q, A.k) + >>> A.scalar_map(B) + {A.x: B.x*cos(q) - B.y*sin(q), A.y: B.x*sin(q) + B.y*cos(q), A.z: B.z} + + """ + + origin_coords = tuple(self.position_wrt(other).to_matrix(other)) + relocated_scalars = [x - origin_coords[i] + for i, x in enumerate(other.base_scalars())] + + vars_matrix = (self.rotation_matrix(other) * + Matrix(relocated_scalars)) + return {x: trigsimp(vars_matrix[i]) + for i, x in enumerate(self.base_scalars())} + + def locate_new(self, name, position, vector_names=None, + variable_names=None): + """ + Returns a CoordSys3D with its origin located at the given + position wrt this coordinate system's origin. + + Parameters + ========== + + name : str + The name of the new CoordSys3D instance. + + position : Vector + The position vector of the new system's origin wrt this + one. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> A = CoordSys3D('A') + >>> B = A.locate_new('B', 10 * A.i) + >>> B.origin.position_wrt(A.origin) + 10*A.i + + """ + if variable_names is None: + variable_names = self._variable_names + if vector_names is None: + vector_names = self._vector_names + + return CoordSys3D(name, location=position, + vector_names=vector_names, + variable_names=variable_names, + parent=self) + + def orient_new(self, name, orienters, location=None, + vector_names=None, variable_names=None): + """ + Creates a new CoordSys3D oriented in the user-specified way + with respect to this system. + + Please refer to the documentation of the orienter classes + for more information about the orientation procedure. + + Parameters + ========== + + name : str + The name of the new CoordSys3D instance. + + orienters : iterable/Orienter + An Orienter or an iterable of Orienters for orienting the + new coordinate system. + If an Orienter is provided, it is applied to get the new + system. + If an iterable is provided, the orienters will be applied + in the order in which they appear in the iterable. + + location : Vector(optional) + The location of the new coordinate system's origin wrt this + system's origin. If not specified, the origins are taken to + be coincident. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q0, q1, q2, q3 = symbols('q0 q1 q2 q3') + >>> N = CoordSys3D('N') + + Using an AxisOrienter + + >>> from sympy.vector import AxisOrienter + >>> axis_orienter = AxisOrienter(q1, N.i + 2 * N.j) + >>> A = N.orient_new('A', (axis_orienter, )) + + Using a BodyOrienter + + >>> from sympy.vector import BodyOrienter + >>> body_orienter = BodyOrienter(q1, q2, q3, '123') + >>> B = N.orient_new('B', (body_orienter, )) + + Using a SpaceOrienter + + >>> from sympy.vector import SpaceOrienter + >>> space_orienter = SpaceOrienter(q1, q2, q3, '312') + >>> C = N.orient_new('C', (space_orienter, )) + + Using a QuaternionOrienter + + >>> from sympy.vector import QuaternionOrienter + >>> q_orienter = QuaternionOrienter(q0, q1, q2, q3) + >>> D = N.orient_new('D', (q_orienter, )) + """ + if variable_names is None: + variable_names = self._variable_names + if vector_names is None: + vector_names = self._vector_names + + if isinstance(orienters, Orienter): + if isinstance(orienters, AxisOrienter): + final_matrix = orienters.rotation_matrix(self) + else: + final_matrix = orienters.rotation_matrix() + # TODO: trigsimp is needed here so that the matrix becomes + # canonical (scalar_map also calls trigsimp; without this, you can + # end up with the same CoordinateSystem that compares differently + # due to a differently formatted matrix). However, this is + # probably not so good for performance. + final_matrix = trigsimp(final_matrix) + else: + final_matrix = Matrix(eye(3)) + for orienter in orienters: + if isinstance(orienter, AxisOrienter): + final_matrix *= orienter.rotation_matrix(self) + else: + final_matrix *= orienter.rotation_matrix() + + return CoordSys3D(name, rotation_matrix=final_matrix, + vector_names=vector_names, + variable_names=variable_names, + location=location, + parent=self) + + def orient_new_axis(self, name, angle, axis, location=None, + vector_names=None, variable_names=None): + """ + Axis rotation is a rotation about an arbitrary axis by + some angle. The angle is supplied as a SymPy expr scalar, and + the axis is supplied as a Vector. + + Parameters + ========== + + name : string + The name of the new coordinate system + + angle : Expr + The angle by which the new system is to be rotated + + axis : Vector + The axis around which the rotation has to be performed + + location : Vector(optional) + The location of the new coordinate system's origin wrt this + system's origin. If not specified, the origins are taken to + be coincident. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q1 = symbols('q1') + >>> N = CoordSys3D('N') + >>> B = N.orient_new_axis('B', q1, N.i + 2 * N.j) + + """ + if variable_names is None: + variable_names = self._variable_names + if vector_names is None: + vector_names = self._vector_names + + orienter = AxisOrienter(angle, axis) + return self.orient_new(name, orienter, + location=location, + vector_names=vector_names, + variable_names=variable_names) + + def orient_new_body(self, name, angle1, angle2, angle3, + rotation_order, location=None, + vector_names=None, variable_names=None): + """ + Body orientation takes this coordinate system through three + successive simple rotations. + + Body fixed rotations include both Euler Angles and + Tait-Bryan Angles, see https://en.wikipedia.org/wiki/Euler_angles. + + Parameters + ========== + + name : string + The name of the new coordinate system + + angle1, angle2, angle3 : Expr + Three successive angles to rotate the coordinate system by + + rotation_order : string + String defining the order of axes for rotation + + location : Vector(optional) + The location of the new coordinate system's origin wrt this + system's origin. If not specified, the origins are taken to + be coincident. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q1, q2, q3 = symbols('q1 q2 q3') + >>> N = CoordSys3D('N') + + A 'Body' fixed rotation is described by three angles and + three body-fixed rotation axes. To orient a coordinate system D + with respect to N, each sequential rotation is always about + the orthogonal unit vectors fixed to D. For example, a '123' + rotation will specify rotations about N.i, then D.j, then + D.k. (Initially, D.i is same as N.i) + Therefore, + + >>> D = N.orient_new_body('D', q1, q2, q3, '123') + + is same as + + >>> D = N.orient_new_axis('D', q1, N.i) + >>> D = D.orient_new_axis('D', q2, D.j) + >>> D = D.orient_new_axis('D', q3, D.k) + + Acceptable rotation orders are of length 3, expressed in XYZ or + 123, and cannot have a rotation about about an axis twice in a row. + + >>> B = N.orient_new_body('B', q1, q2, q3, '123') + >>> B = N.orient_new_body('B', q1, q2, 0, 'ZXZ') + >>> B = N.orient_new_body('B', 0, 0, 0, 'XYX') + + """ + + orienter = BodyOrienter(angle1, angle2, angle3, rotation_order) + return self.orient_new(name, orienter, + location=location, + vector_names=vector_names, + variable_names=variable_names) + + def orient_new_space(self, name, angle1, angle2, angle3, + rotation_order, location=None, + vector_names=None, variable_names=None): + """ + Space rotation is similar to Body rotation, but the rotations + are applied in the opposite order. + + Parameters + ========== + + name : string + The name of the new coordinate system + + angle1, angle2, angle3 : Expr + Three successive angles to rotate the coordinate system by + + rotation_order : string + String defining the order of axes for rotation + + location : Vector(optional) + The location of the new coordinate system's origin wrt this + system's origin. If not specified, the origins are taken to + be coincident. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + See Also + ======== + + CoordSys3D.orient_new_body : method to orient via Euler + angles + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q1, q2, q3 = symbols('q1 q2 q3') + >>> N = CoordSys3D('N') + + To orient a coordinate system D with respect to N, each + sequential rotation is always about N's orthogonal unit vectors. + For example, a '123' rotation will specify rotations about + N.i, then N.j, then N.k. + Therefore, + + >>> D = N.orient_new_space('D', q1, q2, q3, '312') + + is same as + + >>> B = N.orient_new_axis('B', q1, N.i) + >>> C = B.orient_new_axis('C', q2, N.j) + >>> D = C.orient_new_axis('D', q3, N.k) + + """ + + orienter = SpaceOrienter(angle1, angle2, angle3, rotation_order) + return self.orient_new(name, orienter, + location=location, + vector_names=vector_names, + variable_names=variable_names) + + def orient_new_quaternion(self, name, q0, q1, q2, q3, location=None, + vector_names=None, variable_names=None): + """ + Quaternion orientation orients the new CoordSys3D with + Quaternions, defined as a finite rotation about lambda, a unit + vector, by some amount theta. + + This orientation is described by four parameters: + + q0 = cos(theta/2) + + q1 = lambda_x sin(theta/2) + + q2 = lambda_y sin(theta/2) + + q3 = lambda_z sin(theta/2) + + Quaternion does not take in a rotation order. + + Parameters + ========== + + name : string + The name of the new coordinate system + + q0, q1, q2, q3 : Expr + The quaternions to rotate the coordinate system by + + location : Vector(optional) + The location of the new coordinate system's origin wrt this + system's origin. If not specified, the origins are taken to + be coincident. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q0, q1, q2, q3 = symbols('q0 q1 q2 q3') + >>> N = CoordSys3D('N') + >>> B = N.orient_new_quaternion('B', q0, q1, q2, q3) + + """ + + orienter = QuaternionOrienter(q0, q1, q2, q3) + return self.orient_new(name, orienter, + location=location, + vector_names=vector_names, + variable_names=variable_names) + + def create_new(self, name, transformation, variable_names=None, vector_names=None): + """ + Returns a CoordSys3D which is connected to self by transformation. + + Parameters + ========== + + name : str + The name of the new CoordSys3D instance. + + transformation : Lambda, Tuple, str + Transformation defined by transformation equations or chosen + from predefined ones. + + vector_names, variable_names : iterable(optional) + Iterables of 3 strings each, with custom names for base + vectors and base scalars of the new system respectively. + Used for simple str printing. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> a = CoordSys3D('a') + >>> b = a.create_new('b', transformation='spherical') + >>> b.transformation_to_parent() + (b.r*sin(b.theta)*cos(b.phi), b.r*sin(b.phi)*sin(b.theta), b.r*cos(b.theta)) + >>> b.transformation_from_parent() + (sqrt(a.x**2 + a.y**2 + a.z**2), acos(a.z/sqrt(a.x**2 + a.y**2 + a.z**2)), atan2(a.y, a.x)) + + """ + return CoordSys3D(name, parent=self, transformation=transformation, + variable_names=variable_names, vector_names=vector_names) + + def __init__(self, name, location=None, rotation_matrix=None, + parent=None, vector_names=None, variable_names=None, + latex_vects=None, pretty_vects=None, latex_scalars=None, + pretty_scalars=None, transformation=None): + # Dummy initializer for setting docstring + pass + + __init__.__doc__ = __new__.__doc__ + + @staticmethod + def _compose_rotation_and_translation(rot, translation, parent): + r = lambda x, y, z: CoordSys3D._rotation_trans_equations(rot, (x, y, z)) + if parent is None: + return r + + dx, dy, dz = [translation.dot(i) for i in parent.base_vectors()] + t = lambda x, y, z: ( + x + dx, + y + dy, + z + dz, + ) + return lambda x, y, z: t(*r(x, y, z)) + + +def _check_strings(arg_name, arg): + errorstr = arg_name + " must be an iterable of 3 string-types" + if len(arg) != 3: + raise ValueError(errorstr) + for s in arg: + if not isinstance(s, str): + raise TypeError(errorstr) + + +# Delayed import to avoid cyclic import problems: +from sympy.vector.vector import BaseVector diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/deloperator.py b/mgm/lib/python3.10/site-packages/sympy/vector/deloperator.py new file mode 100644 index 0000000000000000000000000000000000000000..51c3c0caf42b5e5d372bd65907d8bae2bd563562 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/deloperator.py @@ -0,0 +1,121 @@ +from sympy.core import Basic +from sympy.vector.operators import gradient, divergence, curl + + +class Del(Basic): + """ + Represents the vector differential operator, usually represented in + mathematical expressions as the 'nabla' symbol. + """ + + def __new__(cls): + obj = super().__new__(cls) + obj._name = "delop" + return obj + + def gradient(self, scalar_field, doit=False): + """ + Returns the gradient of the given scalar field, as a + Vector instance. + + Parameters + ========== + + scalar_field : SymPy expression + The scalar field to calculate the gradient of. + + doit : bool + If True, the result is returned after calling .doit() on + each component. Else, the returned expression contains + Derivative instances + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Del + >>> C = CoordSys3D('C') + >>> delop = Del() + >>> delop.gradient(9) + 0 + >>> delop(C.x*C.y*C.z).doit() + C.y*C.z*C.i + C.x*C.z*C.j + C.x*C.y*C.k + + """ + + return gradient(scalar_field, doit=doit) + + __call__ = gradient + __call__.__doc__ = gradient.__doc__ + + def dot(self, vect, doit=False): + """ + Represents the dot product between this operator and a given + vector - equal to the divergence of the vector field. + + Parameters + ========== + + vect : Vector + The vector whose divergence is to be calculated. + + doit : bool + If True, the result is returned after calling .doit() on + each component. Else, the returned expression contains + Derivative instances + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Del + >>> delop = Del() + >>> C = CoordSys3D('C') + >>> delop.dot(C.x*C.i) + Derivative(C.x, C.x) + >>> v = C.x*C.y*C.z * (C.i + C.j + C.k) + >>> (delop & v).doit() + C.x*C.y + C.x*C.z + C.y*C.z + + """ + return divergence(vect, doit=doit) + + __and__ = dot + __and__.__doc__ = dot.__doc__ + + def cross(self, vect, doit=False): + """ + Represents the cross product between this operator and a given + vector - equal to the curl of the vector field. + + Parameters + ========== + + vect : Vector + The vector whose curl is to be calculated. + + doit : bool + If True, the result is returned after calling .doit() on + each component. Else, the returned expression contains + Derivative instances + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Del + >>> C = CoordSys3D('C') + >>> delop = Del() + >>> v = C.x*C.y*C.z * (C.i + C.j + C.k) + >>> delop.cross(v, doit = True) + (-C.x*C.y + C.x*C.z)*C.i + (C.x*C.y - C.y*C.z)*C.j + + (-C.x*C.z + C.y*C.z)*C.k + >>> (delop ^ C.i).doit() + 0 + + """ + + return curl(vect, doit=doit) + + __xor__ = cross + __xor__.__doc__ = cross.__doc__ + + def _sympystr(self, printer): + return self._name diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/dyadic.py b/mgm/lib/python3.10/site-packages/sympy/vector/dyadic.py new file mode 100644 index 0000000000000000000000000000000000000000..980c6e6dad90ac095b7bd6d4228f507a7831b39f --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/dyadic.py @@ -0,0 +1,285 @@ +from __future__ import annotations + +from sympy.vector.basisdependent import (BasisDependent, BasisDependentAdd, + BasisDependentMul, BasisDependentZero) +from sympy.core import S, Pow +from sympy.core.expr import AtomicExpr +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +import sympy.vector + + +class Dyadic(BasisDependent): + """ + Super class for all Dyadic-classes. + + References + ========== + + .. [1] https://en.wikipedia.org/wiki/Dyadic_tensor + .. [2] Kane, T., Levinson, D. Dynamics Theory and Applications. 1985 + McGraw-Hill + + """ + + _op_priority = 13.0 + + _expr_type: type[Dyadic] + _mul_func: type[Dyadic] + _add_func: type[Dyadic] + _zero_func: type[Dyadic] + _base_func: type[Dyadic] + zero: DyadicZero + + @property + def components(self): + """ + Returns the components of this dyadic in the form of a + Python dictionary mapping BaseDyadic instances to the + corresponding measure numbers. + + """ + # The '_components' attribute is defined according to the + # subclass of Dyadic the instance belongs to. + return self._components + + def dot(self, other): + """ + Returns the dot product(also called inner product) of this + Dyadic, with another Dyadic or Vector. + If 'other' is a Dyadic, this returns a Dyadic. Else, it returns + a Vector (unless an error is encountered). + + Parameters + ========== + + other : Dyadic/Vector + The other Dyadic or Vector to take the inner product with + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> D1 = N.i.outer(N.j) + >>> D2 = N.j.outer(N.j) + >>> D1.dot(D2) + (N.i|N.j) + >>> D1.dot(N.j) + N.i + + """ + + Vector = sympy.vector.Vector + if isinstance(other, BasisDependentZero): + return Vector.zero + elif isinstance(other, Vector): + outvec = Vector.zero + for k, v in self.components.items(): + vect_dot = k.args[1].dot(other) + outvec += vect_dot * v * k.args[0] + return outvec + elif isinstance(other, Dyadic): + outdyad = Dyadic.zero + for k1, v1 in self.components.items(): + for k2, v2 in other.components.items(): + vect_dot = k1.args[1].dot(k2.args[0]) + outer_product = k1.args[0].outer(k2.args[1]) + outdyad += vect_dot * v1 * v2 * outer_product + return outdyad + else: + raise TypeError("Inner product is not defined for " + + str(type(other)) + " and Dyadics.") + + def __and__(self, other): + return self.dot(other) + + __and__.__doc__ = dot.__doc__ + + def cross(self, other): + """ + Returns the cross product between this Dyadic, and a Vector, as a + Vector instance. + + Parameters + ========== + + other : Vector + The Vector that we are crossing this Dyadic with + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> d = N.i.outer(N.i) + >>> d.cross(N.j) + (N.i|N.k) + + """ + + Vector = sympy.vector.Vector + if other == Vector.zero: + return Dyadic.zero + elif isinstance(other, Vector): + outdyad = Dyadic.zero + for k, v in self.components.items(): + cross_product = k.args[1].cross(other) + outer = k.args[0].outer(cross_product) + outdyad += v * outer + return outdyad + else: + raise TypeError(str(type(other)) + " not supported for " + + "cross with dyadics") + + def __xor__(self, other): + return self.cross(other) + + __xor__.__doc__ = cross.__doc__ + + def to_matrix(self, system, second_system=None): + """ + Returns the matrix form of the dyadic with respect to one or two + coordinate systems. + + Parameters + ========== + + system : CoordSys3D + The coordinate system that the rows and columns of the matrix + correspond to. If a second system is provided, this + only corresponds to the rows of the matrix. + second_system : CoordSys3D, optional, default=None + The coordinate system that the columns of the matrix correspond + to. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> v = N.i + 2*N.j + >>> d = v.outer(N.i) + >>> d.to_matrix(N) + Matrix([ + [1, 0, 0], + [2, 0, 0], + [0, 0, 0]]) + >>> from sympy import Symbol + >>> q = Symbol('q') + >>> P = N.orient_new_axis('P', q, N.k) + >>> d.to_matrix(N, P) + Matrix([ + [ cos(q), -sin(q), 0], + [2*cos(q), -2*sin(q), 0], + [ 0, 0, 0]]) + + """ + + if second_system is None: + second_system = system + + return Matrix([i.dot(self).dot(j) for i in system for j in + second_system]).reshape(3, 3) + + def _div_helper(one, other): + """ Helper for division involving dyadics """ + if isinstance(one, Dyadic) and isinstance(other, Dyadic): + raise TypeError("Cannot divide two dyadics") + elif isinstance(one, Dyadic): + return DyadicMul(one, Pow(other, S.NegativeOne)) + else: + raise TypeError("Cannot divide by a dyadic") + + +class BaseDyadic(Dyadic, AtomicExpr): + """ + Class to denote a base dyadic tensor component. + """ + + def __new__(cls, vector1, vector2): + Vector = sympy.vector.Vector + BaseVector = sympy.vector.BaseVector + VectorZero = sympy.vector.VectorZero + # Verify arguments + if not isinstance(vector1, (BaseVector, VectorZero)) or \ + not isinstance(vector2, (BaseVector, VectorZero)): + raise TypeError("BaseDyadic cannot be composed of non-base " + + "vectors") + # Handle special case of zero vector + elif vector1 == Vector.zero or vector2 == Vector.zero: + return Dyadic.zero + # Initialize instance + obj = super().__new__(cls, vector1, vector2) + obj._base_instance = obj + obj._measure_number = 1 + obj._components = {obj: S.One} + obj._sys = vector1._sys + obj._pretty_form = ('(' + vector1._pretty_form + '|' + + vector2._pretty_form + ')') + obj._latex_form = (r'\left(' + vector1._latex_form + r"{\middle|}" + + vector2._latex_form + r'\right)') + + return obj + + def _sympystr(self, printer): + return "({}|{})".format( + printer._print(self.args[0]), printer._print(self.args[1])) + + def _sympyrepr(self, printer): + return "BaseDyadic({}, {})".format( + printer._print(self.args[0]), printer._print(self.args[1])) + + +class DyadicMul(BasisDependentMul, Dyadic): + """ Products of scalars and BaseDyadics """ + + def __new__(cls, *args, **options): + obj = BasisDependentMul.__new__(cls, *args, **options) + return obj + + @property + def base_dyadic(self): + """ The BaseDyadic involved in the product. """ + return self._base_instance + + @property + def measure_number(self): + """ The scalar expression involved in the definition of + this DyadicMul. + """ + return self._measure_number + + +class DyadicAdd(BasisDependentAdd, Dyadic): + """ Class to hold dyadic sums """ + + def __new__(cls, *args, **options): + obj = BasisDependentAdd.__new__(cls, *args, **options) + return obj + + def _sympystr(self, printer): + items = list(self.components.items()) + items.sort(key=lambda x: x[0].__str__()) + return " + ".join(printer._print(k * v) for k, v in items) + + +class DyadicZero(BasisDependentZero, Dyadic): + """ + Class to denote a zero dyadic + """ + + _op_priority = 13.1 + _pretty_form = '(0|0)' + _latex_form = r'(\mathbf{\hat{0}}|\mathbf{\hat{0}})' + + def __new__(cls): + obj = BasisDependentZero.__new__(cls) + return obj + + +Dyadic._expr_type = Dyadic +Dyadic._mul_func = DyadicMul +Dyadic._add_func = DyadicAdd +Dyadic._zero_func = DyadicZero +Dyadic._base_func = BaseDyadic +Dyadic.zero = DyadicZero() diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/functions.py b/mgm/lib/python3.10/site-packages/sympy/vector/functions.py new file mode 100644 index 0000000000000000000000000000000000000000..ca3e5e52c6c9ef96f98cf6e20a32ae0ec1d78068 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/functions.py @@ -0,0 +1,517 @@ +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.deloperator import Del +from sympy.vector.scalar import BaseScalar +from sympy.vector.vector import Vector, BaseVector +from sympy.vector.operators import gradient, curl, divergence +from sympy.core.function import diff +from sympy.core.singleton import S +from sympy.integrals.integrals import integrate +from sympy.simplify.simplify import simplify +from sympy.core import sympify +from sympy.vector.dyadic import Dyadic + + +def express(expr, system, system2=None, variables=False): + """ + Global function for 'express' functionality. + + Re-expresses a Vector, Dyadic or scalar(sympyfiable) in the given + coordinate system. + + If 'variables' is True, then the coordinate variables (base scalars) + of other coordinate systems present in the vector/scalar field or + dyadic are also substituted in terms of the base scalars of the + given system. + + Parameters + ========== + + expr : Vector/Dyadic/scalar(sympyfiable) + The expression to re-express in CoordSys3D 'system' + + system: CoordSys3D + The coordinate system the expr is to be expressed in + + system2: CoordSys3D + The other coordinate system required for re-expression + (only for a Dyadic Expr) + + variables : boolean + Specifies whether to substitute the coordinate variables present + in expr, in terms of those of parameter system + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import Symbol, cos, sin + >>> N = CoordSys3D('N') + >>> q = Symbol('q') + >>> B = N.orient_new_axis('B', q, N.k) + >>> from sympy.vector import express + >>> express(B.i, N) + (cos(q))*N.i + (sin(q))*N.j + >>> express(N.x, B, variables=True) + B.x*cos(q) - B.y*sin(q) + >>> d = N.i.outer(N.i) + >>> express(d, B, N) == (cos(q))*(B.i|N.i) + (-sin(q))*(B.j|N.i) + True + + """ + + if expr in (0, Vector.zero): + return expr + + if not isinstance(system, CoordSys3D): + raise TypeError("system should be a CoordSys3D \ + instance") + + if isinstance(expr, Vector): + if system2 is not None: + raise ValueError("system2 should not be provided for \ + Vectors") + # Given expr is a Vector + if variables: + # If variables attribute is True, substitute + # the coordinate variables in the Vector + system_list = {x.system for x in expr.atoms(BaseScalar, BaseVector)} - {system} + subs_dict = {} + for f in system_list: + subs_dict.update(f.scalar_map(system)) + expr = expr.subs(subs_dict) + # Re-express in this coordinate system + outvec = Vector.zero + parts = expr.separate() + for x in parts: + if x != system: + temp = system.rotation_matrix(x) * parts[x].to_matrix(x) + outvec += matrix_to_vector(temp, system) + else: + outvec += parts[x] + return outvec + + elif isinstance(expr, Dyadic): + if system2 is None: + system2 = system + if not isinstance(system2, CoordSys3D): + raise TypeError("system2 should be a CoordSys3D \ + instance") + outdyad = Dyadic.zero + var = variables + for k, v in expr.components.items(): + outdyad += (express(v, system, variables=var) * + (express(k.args[0], system, variables=var) | + express(k.args[1], system2, variables=var))) + + return outdyad + + else: + if system2 is not None: + raise ValueError("system2 should not be provided for \ + Vectors") + if variables: + # Given expr is a scalar field + system_set = set() + expr = sympify(expr) + # Substitute all the coordinate variables + for x in expr.atoms(BaseScalar): + if x.system != system: + system_set.add(x.system) + subs_dict = {} + for f in system_set: + subs_dict.update(f.scalar_map(system)) + return expr.subs(subs_dict) + return expr + + +def directional_derivative(field, direction_vector): + """ + Returns the directional derivative of a scalar or vector field computed + along a given vector in coordinate system which parameters are expressed. + + Parameters + ========== + + field : Vector or Scalar + The scalar or vector field to compute the directional derivative of + + direction_vector : Vector + The vector to calculated directional derivative along them. + + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, directional_derivative + >>> R = CoordSys3D('R') + >>> f1 = R.x*R.y*R.z + >>> v1 = 3*R.i + 4*R.j + R.k + >>> directional_derivative(f1, v1) + R.x*R.y + 4*R.x*R.z + 3*R.y*R.z + >>> f2 = 5*R.x**2*R.z + >>> directional_derivative(f2, v1) + 5*R.x**2 + 30*R.x*R.z + + """ + from sympy.vector.operators import _get_coord_systems + coord_sys = _get_coord_systems(field) + if len(coord_sys) > 0: + # TODO: This gets a random coordinate system in case of multiple ones: + coord_sys = next(iter(coord_sys)) + field = express(field, coord_sys, variables=True) + i, j, k = coord_sys.base_vectors() + x, y, z = coord_sys.base_scalars() + out = Vector.dot(direction_vector, i) * diff(field, x) + out += Vector.dot(direction_vector, j) * diff(field, y) + out += Vector.dot(direction_vector, k) * diff(field, z) + if out == 0 and isinstance(field, Vector): + out = Vector.zero + return out + elif isinstance(field, Vector): + return Vector.zero + else: + return S.Zero + + +def laplacian(expr): + """ + Return the laplacian of the given field computed in terms of + the base scalars of the given coordinate system. + + Parameters + ========== + + expr : SymPy Expr or Vector + expr denotes a scalar or vector field. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, laplacian + >>> R = CoordSys3D('R') + >>> f = R.x**2*R.y**5*R.z + >>> laplacian(f) + 20*R.x**2*R.y**3*R.z + 2*R.y**5*R.z + >>> f = R.x**2*R.i + R.y**3*R.j + R.z**4*R.k + >>> laplacian(f) + 2*R.i + 6*R.y*R.j + 12*R.z**2*R.k + + """ + + delop = Del() + if expr.is_Vector: + return (gradient(divergence(expr)) - curl(curl(expr))).doit() + return delop.dot(delop(expr)).doit() + + +def is_conservative(field): + """ + Checks if a field is conservative. + + Parameters + ========== + + field : Vector + The field to check for conservative property + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy.vector import is_conservative + >>> R = CoordSys3D('R') + >>> is_conservative(R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k) + True + >>> is_conservative(R.z*R.j) + False + + """ + + # Field is conservative irrespective of system + # Take the first coordinate system in the result of the + # separate method of Vector + if not isinstance(field, Vector): + raise TypeError("field should be a Vector") + if field == Vector.zero: + return True + return curl(field).simplify() == Vector.zero + + +def is_solenoidal(field): + """ + Checks if a field is solenoidal. + + Parameters + ========== + + field : Vector + The field to check for solenoidal property + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy.vector import is_solenoidal + >>> R = CoordSys3D('R') + >>> is_solenoidal(R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k) + True + >>> is_solenoidal(R.y * R.j) + False + + """ + + # Field is solenoidal irrespective of system + # Take the first coordinate system in the result of the + # separate method in Vector + if not isinstance(field, Vector): + raise TypeError("field should be a Vector") + if field == Vector.zero: + return True + return divergence(field).simplify() is S.Zero + + +def scalar_potential(field, coord_sys): + """ + Returns the scalar potential function of a field in a given + coordinate system (without the added integration constant). + + Parameters + ========== + + field : Vector + The vector field whose scalar potential function is to be + calculated + + coord_sys : CoordSys3D + The coordinate system to do the calculation in + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy.vector import scalar_potential, gradient + >>> R = CoordSys3D('R') + >>> scalar_potential(R.k, R) == R.z + True + >>> scalar_field = 2*R.x**2*R.y*R.z + >>> grad_field = gradient(scalar_field) + >>> scalar_potential(grad_field, R) + 2*R.x**2*R.y*R.z + + """ + + # Check whether field is conservative + if not is_conservative(field): + raise ValueError("Field is not conservative") + if field == Vector.zero: + return S.Zero + # Express the field exntirely in coord_sys + # Substitute coordinate variables also + if not isinstance(coord_sys, CoordSys3D): + raise TypeError("coord_sys must be a CoordSys3D") + field = express(field, coord_sys, variables=True) + dimensions = coord_sys.base_vectors() + scalars = coord_sys.base_scalars() + # Calculate scalar potential function + temp_function = integrate(field.dot(dimensions[0]), scalars[0]) + for i, dim in enumerate(dimensions[1:]): + partial_diff = diff(temp_function, scalars[i + 1]) + partial_diff = field.dot(dim) - partial_diff + temp_function += integrate(partial_diff, scalars[i + 1]) + return temp_function + + +def scalar_potential_difference(field, coord_sys, point1, point2): + """ + Returns the scalar potential difference between two points in a + certain coordinate system, wrt a given field. + + If a scalar field is provided, its values at the two points are + considered. If a conservative vector field is provided, the values + of its scalar potential function at the two points are used. + + Returns (potential at point2) - (potential at point1) + + The position vectors of the two Points are calculated wrt the + origin of the coordinate system provided. + + Parameters + ========== + + field : Vector/Expr + The field to calculate wrt + + coord_sys : CoordSys3D + The coordinate system to do the calculations in + + point1 : Point + The initial Point in given coordinate system + + position2 : Point + The second Point in the given coordinate system + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy.vector import scalar_potential_difference + >>> R = CoordSys3D('R') + >>> P = R.origin.locate_new('P', R.x*R.i + R.y*R.j + R.z*R.k) + >>> vectfield = 4*R.x*R.y*R.i + 2*R.x**2*R.j + >>> scalar_potential_difference(vectfield, R, R.origin, P) + 2*R.x**2*R.y + >>> Q = R.origin.locate_new('O', 3*R.i + R.j + 2*R.k) + >>> scalar_potential_difference(vectfield, R, P, Q) + -2*R.x**2*R.y + 18 + + """ + + if not isinstance(coord_sys, CoordSys3D): + raise TypeError("coord_sys must be a CoordSys3D") + if isinstance(field, Vector): + # Get the scalar potential function + scalar_fn = scalar_potential(field, coord_sys) + else: + # Field is a scalar + scalar_fn = field + # Express positions in required coordinate system + origin = coord_sys.origin + position1 = express(point1.position_wrt(origin), coord_sys, + variables=True) + position2 = express(point2.position_wrt(origin), coord_sys, + variables=True) + # Get the two positions as substitution dicts for coordinate variables + subs_dict1 = {} + subs_dict2 = {} + scalars = coord_sys.base_scalars() + for i, x in enumerate(coord_sys.base_vectors()): + subs_dict1[scalars[i]] = x.dot(position1) + subs_dict2[scalars[i]] = x.dot(position2) + return scalar_fn.subs(subs_dict2) - scalar_fn.subs(subs_dict1) + + +def matrix_to_vector(matrix, system): + """ + Converts a vector in matrix form to a Vector instance. + + It is assumed that the elements of the Matrix represent the + measure numbers of the components of the vector along basis + vectors of 'system'. + + Parameters + ========== + + matrix : SymPy Matrix, Dimensions: (3, 1) + The matrix to be converted to a vector + + system : CoordSys3D + The coordinate system the vector is to be defined in + + Examples + ======== + + >>> from sympy import ImmutableMatrix as Matrix + >>> m = Matrix([1, 2, 3]) + >>> from sympy.vector import CoordSys3D, matrix_to_vector + >>> C = CoordSys3D('C') + >>> v = matrix_to_vector(m, C) + >>> v + C.i + 2*C.j + 3*C.k + >>> v.to_matrix(C) == m + True + + """ + + outvec = Vector.zero + vects = system.base_vectors() + for i, x in enumerate(matrix): + outvec += x * vects[i] + return outvec + + +def _path(from_object, to_object): + """ + Calculates the 'path' of objects starting from 'from_object' + to 'to_object', along with the index of the first common + ancestor in the tree. + + Returns (index, list) tuple. + """ + + if from_object._root != to_object._root: + raise ValueError("No connecting path found between " + + str(from_object) + " and " + str(to_object)) + + other_path = [] + obj = to_object + while obj._parent is not None: + other_path.append(obj) + obj = obj._parent + other_path.append(obj) + object_set = set(other_path) + from_path = [] + obj = from_object + while obj not in object_set: + from_path.append(obj) + obj = obj._parent + index = len(from_path) + i = other_path.index(obj) + while i >= 0: + from_path.append(other_path[i]) + i -= 1 + return index, from_path + + +def orthogonalize(*vlist, orthonormal=False): + """ + Takes a sequence of independent vectors and orthogonalizes them + using the Gram - Schmidt process. Returns a list of + orthogonal or orthonormal vectors. + + Parameters + ========== + + vlist : sequence of independent vectors to be made orthogonal. + + orthonormal : Optional parameter + Set to True if the vectors returned should be + orthonormal. + Default: False + + Examples + ======== + + >>> from sympy.vector.coordsysrect import CoordSys3D + >>> from sympy.vector.functions import orthogonalize + >>> C = CoordSys3D('C') + >>> i, j, k = C.base_vectors() + >>> v1 = i + 2*j + >>> v2 = 2*i + 3*j + >>> orthogonalize(v1, v2) + [C.i + 2*C.j, 2/5*C.i + (-1/5)*C.j] + + References + ========== + + .. [1] https://en.wikipedia.org/wiki/Gram-Schmidt_process + + """ + + if not all(isinstance(vec, Vector) for vec in vlist): + raise TypeError('Each element must be of Type Vector') + + ortho_vlist = [] + for i, term in enumerate(vlist): + for j in range(i): + term -= ortho_vlist[j].projection(vlist[i]) + # TODO : The following line introduces a performance issue + # and needs to be changed once a good solution for issue #10279 is + # found. + if simplify(term).equals(Vector.zero): + raise ValueError("Vector set not linearly independent") + ortho_vlist.append(term) + + if orthonormal: + ortho_vlist = [vec.normalize() for vec in ortho_vlist] + + return ortho_vlist diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/implicitregion.py b/mgm/lib/python3.10/site-packages/sympy/vector/implicitregion.py new file mode 100644 index 0000000000000000000000000000000000000000..fedc45315c9209b736b8fcd898080d6c8e48c3a8 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/implicitregion.py @@ -0,0 +1,506 @@ +from sympy.core.numbers import Rational +from sympy.core.singleton import S +from sympy.core.symbol import symbols +from sympy.functions.elementary.complexes import sign +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.polys.polytools import gcd +from sympy.sets.sets import Complement +from sympy.core import Basic, Tuple, diff, expand, Eq, Integer +from sympy.core.sorting import ordered +from sympy.core.symbol import _symbol +from sympy.solvers import solveset, nonlinsolve, diophantine +from sympy.polys import total_degree +from sympy.geometry import Point +from sympy.ntheory.factor_ import core + + +class ImplicitRegion(Basic): + """ + Represents an implicit region in space. + + Examples + ======== + + >>> from sympy import Eq + >>> from sympy.abc import x, y, z, t + >>> from sympy.vector import ImplicitRegion + + >>> ImplicitRegion((x, y), x**2 + y**2 - 4) + ImplicitRegion((x, y), x**2 + y**2 - 4) + >>> ImplicitRegion((x, y), Eq(y*x, 1)) + ImplicitRegion((x, y), x*y - 1) + + >>> parabola = ImplicitRegion((x, y), y**2 - 4*x) + >>> parabola.degree + 2 + >>> parabola.equation + -4*x + y**2 + >>> parabola.rational_parametrization(t) + (4/t**2, 4/t) + + >>> r = ImplicitRegion((x, y, z), Eq(z, x**2 + y**2)) + >>> r.variables + (x, y, z) + >>> r.singular_points() + EmptySet + >>> r.regular_point() + (-10, -10, 200) + + Parameters + ========== + + variables : tuple to map variables in implicit equation to base scalars. + + equation : An expression or Eq denoting the implicit equation of the region. + + """ + def __new__(cls, variables, equation): + if not isinstance(variables, Tuple): + variables = Tuple(*variables) + + if isinstance(equation, Eq): + equation = equation.lhs - equation.rhs + + return super().__new__(cls, variables, equation) + + @property + def variables(self): + return self.args[0] + + @property + def equation(self): + return self.args[1] + + @property + def degree(self): + return total_degree(self.equation) + + def regular_point(self): + """ + Returns a point on the implicit region. + + Examples + ======== + + >>> from sympy.abc import x, y, z + >>> from sympy.vector import ImplicitRegion + >>> circle = ImplicitRegion((x, y), (x + 2)**2 + (y - 3)**2 - 16) + >>> circle.regular_point() + (-2, -1) + >>> parabola = ImplicitRegion((x, y), x**2 - 4*y) + >>> parabola.regular_point() + (0, 0) + >>> r = ImplicitRegion((x, y, z), (x + y + z)**4) + >>> r.regular_point() + (-10, -10, 20) + + References + ========== + + - Erik Hillgarter, "Rational Points on Conics", Diploma Thesis, RISC-Linz, + J. Kepler Universitat Linz, 1996. Available: + https://www3.risc.jku.at/publications/download/risc_1355/Rational%20Points%20on%20Conics.pdf + + """ + equation = self.equation + + if len(self.variables) == 1: + return (list(solveset(equation, self.variables[0], domain=S.Reals))[0],) + elif len(self.variables) == 2: + + if self.degree == 2: + coeffs = a, b, c, d, e, f = conic_coeff(self.variables, equation) + + if b**2 == 4*a*c: + x_reg, y_reg = self._regular_point_parabola(*coeffs) + else: + x_reg, y_reg = self._regular_point_ellipse(*coeffs) + return x_reg, y_reg + + if len(self.variables) == 3: + x, y, z = self.variables + + for x_reg in range(-10, 10): + for y_reg in range(-10, 10): + if not solveset(equation.subs({x: x_reg, y: y_reg}), self.variables[2], domain=S.Reals).is_empty: + return (x_reg, y_reg, list(solveset(equation.subs({x: x_reg, y: y_reg})))[0]) + + if len(self.singular_points()) != 0: + return list[self.singular_points()][0] + + raise NotImplementedError() + + def _regular_point_parabola(self, a, b, c, d, e, f): + ok = (a, d) != (0, 0) and (c, e) != (0, 0) and b**2 == 4*a*c and (a, c) != (0, 0) + + if not ok: + raise ValueError("Rational Point on the conic does not exist") + + if a != 0: + d_dash, f_dash = (4*a*e - 2*b*d, 4*a*f - d**2) + if d_dash != 0: + y_reg = -f_dash/d_dash + x_reg = -(d + b*y_reg)/(2*a) + else: + ok = False + elif c != 0: + d_dash, f_dash = (4*c*d - 2*b*e, 4*c*f - e**2) + if d_dash != 0: + x_reg = -f_dash/d_dash + y_reg = -(e + b*x_reg)/(2*c) + else: + ok = False + + if ok: + return x_reg, y_reg + else: + raise ValueError("Rational Point on the conic does not exist") + + def _regular_point_ellipse(self, a, b, c, d, e, f): + D = 4*a*c - b**2 + ok = D + + if not ok: + raise ValueError("Rational Point on the conic does not exist") + + if a == 0 and c == 0: + K = -1 + L = 4*(d*e - b*f) + elif c != 0: + K = D + L = 4*c**2*d**2 - 4*b*c*d*e + 4*a*c*e**2 + 4*b**2*c*f - 16*a*c**2*f + else: + K = D + L = 4*a**2*e**2 - 4*b*a*d*e + 4*b**2*a*f + + ok = L != 0 and not(K > 0 and L < 0) + if not ok: + raise ValueError("Rational Point on the conic does not exist") + + K = Rational(K).limit_denominator(10**12) + L = Rational(L).limit_denominator(10**12) + + k1, k2 = K.p, K.q + l1, l2 = L.p, L.q + g = gcd(k2, l2) + + a1 = (l2*k2)/g + b1 = (k1*l2)/g + c1 = -(l1*k2)/g + a2 = sign(a1)*core(abs(a1), 2) + r1 = sqrt(a1/a2) + b2 = sign(b1)*core(abs(b1), 2) + r2 = sqrt(b1/b2) + c2 = sign(c1)*core(abs(c1), 2) + r3 = sqrt(c1/c2) + + g = gcd(gcd(a2, b2), c2) + a2 = a2/g + b2 = b2/g + c2 = c2/g + + g1 = gcd(a2, b2) + a2 = a2/g1 + b2 = b2/g1 + c2 = c2*g1 + + g2 = gcd(a2,c2) + a2 = a2/g2 + b2 = b2*g2 + c2 = c2/g2 + + g3 = gcd(b2, c2) + a2 = a2*g3 + b2 = b2/g3 + c2 = c2/g3 + + x, y, z = symbols("x y z") + eq = a2*x**2 + b2*y**2 + c2*z**2 + + solutions = diophantine(eq) + + if len(solutions) == 0: + raise ValueError("Rational Point on the conic does not exist") + + flag = False + for sol in solutions: + syms = Tuple(*sol).free_symbols + rep = dict.fromkeys(syms, 3) + sol_z = sol[2] + + if sol_z == 0: + flag = True + continue + + if not isinstance(sol_z, (int, Integer)): + syms_z = sol_z.free_symbols + + if len(syms_z) == 1: + p = next(iter(syms_z)) + p_values = Complement(S.Integers, solveset(Eq(sol_z, 0), p, S.Integers)) + rep[p] = next(iter(p_values)) + + if len(syms_z) == 2: + p, q = list(ordered(syms_z)) + + for i in S.Integers: + subs_sol_z = sol_z.subs(p, i) + q_values = Complement(S.Integers, solveset(Eq(subs_sol_z, 0), q, S.Integers)) + + if not q_values.is_empty: + rep[p] = i + rep[q] = next(iter(q_values)) + break + + if len(syms) != 0: + x, y, z = tuple(s.subs(rep) for s in sol) + else: + x, y, z = sol + flag = False + break + + if flag: + raise ValueError("Rational Point on the conic does not exist") + + x = (x*g3)/r1 + y = (y*g2)/r2 + z = (z*g1)/r3 + x = x/z + y = y/z + + if a == 0 and c == 0: + x_reg = (x + y - 2*e)/(2*b) + y_reg = (x - y - 2*d)/(2*b) + elif c != 0: + x_reg = (x - 2*d*c + b*e)/K + y_reg = (y - b*x_reg - e)/(2*c) + else: + y_reg = (x - 2*e*a + b*d)/K + x_reg = (y - b*y_reg - d)/(2*a) + + return x_reg, y_reg + + def singular_points(self): + """ + Returns a set of singular points of the region. + + The singular points are those points on the region + where all partial derivatives vanish. + + Examples + ======== + + >>> from sympy.abc import x, y + >>> from sympy.vector import ImplicitRegion + >>> I = ImplicitRegion((x, y), (y-1)**2 -x**3 + 2*x**2 -x) + >>> I.singular_points() + {(1, 1)} + + """ + eq_list = [self.equation] + for var in self.variables: + eq_list += [diff(self.equation, var)] + + return nonlinsolve(eq_list, list(self.variables)) + + def multiplicity(self, point): + """ + Returns the multiplicity of a singular point on the region. + + A singular point (x,y) of region is said to be of multiplicity m + if all the partial derivatives off to order m - 1 vanish there. + + Examples + ======== + + >>> from sympy.abc import x, y, z + >>> from sympy.vector import ImplicitRegion + >>> I = ImplicitRegion((x, y, z), x**2 + y**3 - z**4) + >>> I.singular_points() + {(0, 0, 0)} + >>> I.multiplicity((0, 0, 0)) + 2 + + """ + if isinstance(point, Point): + point = point.args + + modified_eq = self.equation + + for i, var in enumerate(self.variables): + modified_eq = modified_eq.subs(var, var + point[i]) + modified_eq = expand(modified_eq) + + if len(modified_eq.args) != 0: + terms = modified_eq.args + m = min(total_degree(term) for term in terms) + else: + terms = modified_eq + m = total_degree(terms) + + return m + + def rational_parametrization(self, parameters=('t', 's'), reg_point=None): + """ + Returns the rational parametrization of implicit region. + + Examples + ======== + + >>> from sympy import Eq + >>> from sympy.abc import x, y, z, s, t + >>> from sympy.vector import ImplicitRegion + + >>> parabola = ImplicitRegion((x, y), y**2 - 4*x) + >>> parabola.rational_parametrization() + (4/t**2, 4/t) + + >>> circle = ImplicitRegion((x, y), Eq(x**2 + y**2, 4)) + >>> circle.rational_parametrization() + (4*t/(t**2 + 1), 4*t**2/(t**2 + 1) - 2) + + >>> I = ImplicitRegion((x, y), x**3 + x**2 - y**2) + >>> I.rational_parametrization() + (t**2 - 1, t*(t**2 - 1)) + + >>> cubic_curve = ImplicitRegion((x, y), x**3 + x**2 - y**2) + >>> cubic_curve.rational_parametrization(parameters=(t)) + (t**2 - 1, t*(t**2 - 1)) + + >>> sphere = ImplicitRegion((x, y, z), x**2 + y**2 + z**2 - 4) + >>> sphere.rational_parametrization(parameters=(t, s)) + (-2 + 4/(s**2 + t**2 + 1), 4*s/(s**2 + t**2 + 1), 4*t/(s**2 + t**2 + 1)) + + For some conics, regular_points() is unable to find a point on curve. + To calulcate the parametric representation in such cases, user need + to determine a point on the region and pass it using reg_point. + + >>> c = ImplicitRegion((x, y), (x - 1/2)**2 + (y)**2 - (1/4)**2) + >>> c.rational_parametrization(reg_point=(3/4, 0)) + (0.75 - 0.5/(t**2 + 1), -0.5*t/(t**2 + 1)) + + References + ========== + + - Christoph M. Hoffmann, "Conversion Methods between Parametric and + Implicit Curves and Surfaces", Purdue e-Pubs, 1990. Available: + https://docs.lib.purdue.edu/cgi/viewcontent.cgi?article=1827&context=cstech + + """ + equation = self.equation + degree = self.degree + + if degree == 1: + if len(self.variables) == 1: + return (equation,) + elif len(self.variables) == 2: + x, y = self.variables + y_par = list(solveset(equation, y))[0] + return x, y_par + else: + raise NotImplementedError() + + point = () + + # Finding the (n - 1) fold point of the monoid of degree + if degree == 2: + # For degree 2 curves, either a regular point or a singular point can be used. + if reg_point is not None: + # Using point provided by the user as regular point + point = reg_point + else: + if len(self.singular_points()) != 0: + point = list(self.singular_points())[0] + else: + point = self.regular_point() + + if len(self.singular_points()) != 0: + singular_points = self.singular_points() + for spoint in singular_points: + syms = Tuple(*spoint).free_symbols + rep = dict.fromkeys(syms, 2) + + if len(syms) != 0: + spoint = tuple(s.subs(rep) for s in spoint) + + if self.multiplicity(spoint) == degree - 1: + point = spoint + break + + if len(point) == 0: + # The region in not a monoid + raise NotImplementedError() + + modified_eq = equation + + # Shifting the region such that fold point moves to origin + for i, var in enumerate(self.variables): + modified_eq = modified_eq.subs(var, var + point[i]) + modified_eq = expand(modified_eq) + + hn = hn_1 = 0 + for term in modified_eq.args: + if total_degree(term) == degree: + hn += term + else: + hn_1 += term + + hn_1 = -1*hn_1 + + if not isinstance(parameters, tuple): + parameters = (parameters,) + + if len(self.variables) == 2: + + parameter1 = parameters[0] + if parameter1 == 's': + # To avoid name conflict between parameters + s = _symbol('s_', real=True) + else: + s = _symbol('s', real=True) + t = _symbol(parameter1, real=True) + + hn = hn.subs({self.variables[0]: s, self.variables[1]: t}) + hn_1 = hn_1.subs({self.variables[0]: s, self.variables[1]: t}) + + x_par = (s*(hn_1/hn)).subs(s, 1) + point[0] + y_par = (t*(hn_1/hn)).subs(s, 1) + point[1] + + return x_par, y_par + + elif len(self.variables) == 3: + + parameter1, parameter2 = parameters + if 'r' in parameters: + # To avoid name conflict between parameters + r = _symbol('r_', real=True) + else: + r = _symbol('r', real=True) + s = _symbol(parameter2, real=True) + t = _symbol(parameter1, real=True) + + hn = hn.subs({self.variables[0]: r, self.variables[1]: s, self.variables[2]: t}) + hn_1 = hn_1.subs({self.variables[0]: r, self.variables[1]: s, self.variables[2]: t}) + + x_par = (r*(hn_1/hn)).subs(r, 1) + point[0] + y_par = (s*(hn_1/hn)).subs(r, 1) + point[1] + z_par = (t*(hn_1/hn)).subs(r, 1) + point[2] + + return x_par, y_par, z_par + + raise NotImplementedError() + +def conic_coeff(variables, equation): + if total_degree(equation) != 2: + raise ValueError() + x = variables[0] + y = variables[1] + + equation = expand(equation) + a = equation.coeff(x**2) + b = equation.coeff(x*y) + c = equation.coeff(y**2) + d = equation.coeff(x, 1).coeff(y, 0) + e = equation.coeff(y, 1).coeff(x, 0) + f = equation.coeff(x, 0).coeff(y, 0) + return a, b, c, d, e, f diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/integrals.py b/mgm/lib/python3.10/site-packages/sympy/vector/integrals.py new file mode 100644 index 0000000000000000000000000000000000000000..a6451c182f214b20b1105eb0a4dc243455c9d126 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/integrals.py @@ -0,0 +1,206 @@ +from sympy.core import Basic, diff +from sympy.core.singleton import S +from sympy.core.sorting import default_sort_key +from sympy.matrices import Matrix +from sympy.integrals import Integral, integrate +from sympy.geometry.entity import GeometryEntity +from sympy.simplify.simplify import simplify +from sympy.utilities.iterables import topological_sort +from sympy.vector import (CoordSys3D, Vector, ParametricRegion, + parametric_region_list, ImplicitRegion) +from sympy.vector.operators import _get_coord_systems + + +class ParametricIntegral(Basic): + """ + Represents integral of a scalar or vector field + over a Parametric Region + + Examples + ======== + + >>> from sympy import cos, sin, pi + >>> from sympy.vector import CoordSys3D, ParametricRegion, ParametricIntegral + >>> from sympy.abc import r, t, theta, phi + + >>> C = CoordSys3D('C') + >>> curve = ParametricRegion((3*t - 2, t + 1), (t, 1, 2)) + >>> ParametricIntegral(C.x, curve) + 5*sqrt(10)/2 + >>> length = ParametricIntegral(1, curve) + >>> length + sqrt(10) + >>> semisphere = ParametricRegion((2*sin(phi)*cos(theta), 2*sin(phi)*sin(theta), 2*cos(phi)),\ + (theta, 0, 2*pi), (phi, 0, pi/2)) + >>> ParametricIntegral(C.z, semisphere) + 8*pi + + >>> ParametricIntegral(C.j + C.k, ParametricRegion((r*cos(theta), r*sin(theta)), r, theta)) + 0 + + """ + + def __new__(cls, field, parametricregion): + + coord_set = _get_coord_systems(field) + + if len(coord_set) == 0: + coord_sys = CoordSys3D('C') + elif len(coord_set) > 1: + raise ValueError + else: + coord_sys = next(iter(coord_set)) + + if parametricregion.dimensions == 0: + return S.Zero + + base_vectors = coord_sys.base_vectors() + base_scalars = coord_sys.base_scalars() + + parametricfield = field + + r = Vector.zero + for i in range(len(parametricregion.definition)): + r += base_vectors[i]*parametricregion.definition[i] + + if len(coord_set) != 0: + for i in range(len(parametricregion.definition)): + parametricfield = parametricfield.subs(base_scalars[i], parametricregion.definition[i]) + + if parametricregion.dimensions == 1: + parameter = parametricregion.parameters[0] + + r_diff = diff(r, parameter) + lower, upper = parametricregion.limits[parameter][0], parametricregion.limits[parameter][1] + + if isinstance(parametricfield, Vector): + integrand = simplify(r_diff.dot(parametricfield)) + else: + integrand = simplify(r_diff.magnitude()*parametricfield) + + result = integrate(integrand, (parameter, lower, upper)) + + elif parametricregion.dimensions == 2: + u, v = cls._bounds_case(parametricregion.parameters, parametricregion.limits) + + r_u = diff(r, u) + r_v = diff(r, v) + normal_vector = simplify(r_u.cross(r_v)) + + if isinstance(parametricfield, Vector): + integrand = parametricfield.dot(normal_vector) + else: + integrand = parametricfield*normal_vector.magnitude() + + integrand = simplify(integrand) + + lower_u, upper_u = parametricregion.limits[u][0], parametricregion.limits[u][1] + lower_v, upper_v = parametricregion.limits[v][0], parametricregion.limits[v][1] + + result = integrate(integrand, (u, lower_u, upper_u), (v, lower_v, upper_v)) + + else: + variables = cls._bounds_case(parametricregion.parameters, parametricregion.limits) + coeff = Matrix(parametricregion.definition).jacobian(variables).det() + integrand = simplify(parametricfield*coeff) + + l = [(var, parametricregion.limits[var][0], parametricregion.limits[var][1]) for var in variables] + result = integrate(integrand, *l) + + if not isinstance(result, Integral): + return result + else: + return super().__new__(cls, field, parametricregion) + + @classmethod + def _bounds_case(cls, parameters, limits): + + V = list(limits.keys()) + E = [] + + for p in V: + lower_p = limits[p][0] + upper_p = limits[p][1] + + lower_p = lower_p.atoms() + upper_p = upper_p.atoms() + E.extend((p, q) for q in V if p != q and + (lower_p.issuperset({q}) or upper_p.issuperset({q}))) + + if not E: + return parameters + else: + return topological_sort((V, E), key=default_sort_key) + + @property + def field(self): + return self.args[0] + + @property + def parametricregion(self): + return self.args[1] + + +def vector_integrate(field, *region): + """ + Compute the integral of a vector/scalar field + over a a region or a set of parameters. + + Examples + ======== + >>> from sympy.vector import CoordSys3D, ParametricRegion, vector_integrate + >>> from sympy.abc import x, y, t + >>> C = CoordSys3D('C') + + >>> region = ParametricRegion((t, t**2), (t, 1, 5)) + >>> vector_integrate(C.x*C.i, region) + 12 + + Integrals over some objects of geometry module can also be calculated. + + >>> from sympy.geometry import Point, Circle, Triangle + >>> c = Circle(Point(0, 2), 5) + >>> vector_integrate(C.x**2 + C.y**2, c) + 290*pi + >>> triangle = Triangle(Point(-2, 3), Point(2, 3), Point(0, 5)) + >>> vector_integrate(3*C.x**2*C.y*C.i + C.j, triangle) + -8 + + Integrals over some simple implicit regions can be computed. But in most cases, + it takes too long to compute over them. This is due to the expressions of parametric + representation becoming large. + + >>> from sympy.vector import ImplicitRegion + >>> c2 = ImplicitRegion((x, y), (x - 2)**2 + (y - 1)**2 - 9) + >>> vector_integrate(1, c2) + 6*pi + + Integral of fields with respect to base scalars: + + >>> vector_integrate(12*C.y**3, (C.y, 1, 3)) + 240 + >>> vector_integrate(C.x**2*C.z, C.x) + C.x**3*C.z/3 + >>> vector_integrate(C.x*C.i - C.y*C.k, C.x) + (Integral(C.x, C.x))*C.i + (Integral(-C.y, C.x))*C.k + >>> _.doit() + C.x**2/2*C.i + (-C.x*C.y)*C.k + + """ + if len(region) == 1: + if isinstance(region[0], ParametricRegion): + return ParametricIntegral(field, region[0]) + + if isinstance(region[0], ImplicitRegion): + region = parametric_region_list(region[0])[0] + return vector_integrate(field, region) + + if isinstance(region[0], GeometryEntity): + regions_list = parametric_region_list(region[0]) + + result = 0 + for reg in regions_list: + result += vector_integrate(field, reg) + return result + + return integrate(field, *region) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/operators.py b/mgm/lib/python3.10/site-packages/sympy/vector/operators.py new file mode 100644 index 0000000000000000000000000000000000000000..270c3425034c747982e26a13107bcc94da1b1eb1 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/operators.py @@ -0,0 +1,335 @@ +import collections +from sympy.core.expr import Expr +from sympy.core import sympify, S, preorder_traversal +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.vector import Vector, VectorMul, VectorAdd, Cross, Dot +from sympy.core.function import Derivative +from sympy.core.add import Add +from sympy.core.mul import Mul + + +def _get_coord_systems(expr): + g = preorder_traversal(expr) + ret = set() + for i in g: + if isinstance(i, CoordSys3D): + ret.add(i) + g.skip() + return frozenset(ret) + + +def _split_mul_args_wrt_coordsys(expr): + d = collections.defaultdict(lambda: S.One) + for i in expr.args: + d[_get_coord_systems(i)] *= i + return list(d.values()) + + +class Gradient(Expr): + """ + Represents unevaluated Gradient. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Gradient + >>> R = CoordSys3D('R') + >>> s = R.x*R.y*R.z + >>> Gradient(s) + Gradient(R.x*R.y*R.z) + + """ + + def __new__(cls, expr): + expr = sympify(expr) + obj = Expr.__new__(cls, expr) + obj._expr = expr + return obj + + def doit(self, **hints): + return gradient(self._expr, doit=True) + + +class Divergence(Expr): + """ + Represents unevaluated Divergence. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Divergence + >>> R = CoordSys3D('R') + >>> v = R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k + >>> Divergence(v) + Divergence(R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k) + + """ + + def __new__(cls, expr): + expr = sympify(expr) + obj = Expr.__new__(cls, expr) + obj._expr = expr + return obj + + def doit(self, **hints): + return divergence(self._expr, doit=True) + + +class Curl(Expr): + """ + Represents unevaluated Curl. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Curl + >>> R = CoordSys3D('R') + >>> v = R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k + >>> Curl(v) + Curl(R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k) + + """ + + def __new__(cls, expr): + expr = sympify(expr) + obj = Expr.__new__(cls, expr) + obj._expr = expr + return obj + + def doit(self, **hints): + return curl(self._expr, doit=True) + + +def curl(vect, doit=True): + """ + Returns the curl of a vector field computed wrt the base scalars + of the given coordinate system. + + Parameters + ========== + + vect : Vector + The vector operand + + doit : bool + If True, the result is returned after calling .doit() on + each component. Else, the returned expression contains + Derivative instances + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, curl + >>> R = CoordSys3D('R') + >>> v1 = R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k + >>> curl(v1) + 0 + >>> v2 = R.x*R.y*R.z*R.i + >>> curl(v2) + R.x*R.y*R.j + (-R.x*R.z)*R.k + + """ + + coord_sys = _get_coord_systems(vect) + + if len(coord_sys) == 0: + return Vector.zero + elif len(coord_sys) == 1: + coord_sys = next(iter(coord_sys)) + i, j, k = coord_sys.base_vectors() + x, y, z = coord_sys.base_scalars() + h1, h2, h3 = coord_sys.lame_coefficients() + vectx = vect.dot(i) + vecty = vect.dot(j) + vectz = vect.dot(k) + outvec = Vector.zero + outvec += (Derivative(vectz * h3, y) - + Derivative(vecty * h2, z)) * i / (h2 * h3) + outvec += (Derivative(vectx * h1, z) - + Derivative(vectz * h3, x)) * j / (h1 * h3) + outvec += (Derivative(vecty * h2, x) - + Derivative(vectx * h1, y)) * k / (h2 * h1) + + if doit: + return outvec.doit() + return outvec + else: + if isinstance(vect, (Add, VectorAdd)): + from sympy.vector import express + try: + cs = next(iter(coord_sys)) + args = [express(i, cs, variables=True) for i in vect.args] + except ValueError: + args = vect.args + return VectorAdd.fromiter(curl(i, doit=doit) for i in args) + elif isinstance(vect, (Mul, VectorMul)): + vector = [i for i in vect.args if isinstance(i, (Vector, Cross, Gradient))][0] + scalar = Mul.fromiter(i for i in vect.args if not isinstance(i, (Vector, Cross, Gradient))) + res = Cross(gradient(scalar), vector).doit() + scalar*curl(vector, doit=doit) + if doit: + return res.doit() + return res + elif isinstance(vect, (Cross, Curl, Gradient)): + return Curl(vect) + else: + raise Curl(vect) + + +def divergence(vect, doit=True): + """ + Returns the divergence of a vector field computed wrt the base + scalars of the given coordinate system. + + Parameters + ========== + + vector : Vector + The vector operand + + doit : bool + If True, the result is returned after calling .doit() on + each component. Else, the returned expression contains + Derivative instances + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, divergence + >>> R = CoordSys3D('R') + >>> v1 = R.x*R.y*R.z * (R.i+R.j+R.k) + + >>> divergence(v1) + R.x*R.y + R.x*R.z + R.y*R.z + >>> v2 = 2*R.y*R.z*R.j + >>> divergence(v2) + 2*R.z + + """ + coord_sys = _get_coord_systems(vect) + if len(coord_sys) == 0: + return S.Zero + elif len(coord_sys) == 1: + if isinstance(vect, (Cross, Curl, Gradient)): + return Divergence(vect) + # TODO: is case of many coord systems, this gets a random one: + coord_sys = next(iter(coord_sys)) + i, j, k = coord_sys.base_vectors() + x, y, z = coord_sys.base_scalars() + h1, h2, h3 = coord_sys.lame_coefficients() + vx = _diff_conditional(vect.dot(i), x, h2, h3) \ + / (h1 * h2 * h3) + vy = _diff_conditional(vect.dot(j), y, h3, h1) \ + / (h1 * h2 * h3) + vz = _diff_conditional(vect.dot(k), z, h1, h2) \ + / (h1 * h2 * h3) + res = vx + vy + vz + if doit: + return res.doit() + return res + else: + if isinstance(vect, (Add, VectorAdd)): + return Add.fromiter(divergence(i, doit=doit) for i in vect.args) + elif isinstance(vect, (Mul, VectorMul)): + vector = [i for i in vect.args if isinstance(i, (Vector, Cross, Gradient))][0] + scalar = Mul.fromiter(i for i in vect.args if not isinstance(i, (Vector, Cross, Gradient))) + res = Dot(vector, gradient(scalar)) + scalar*divergence(vector, doit=doit) + if doit: + return res.doit() + return res + elif isinstance(vect, (Cross, Curl, Gradient)): + return Divergence(vect) + else: + raise Divergence(vect) + + +def gradient(scalar_field, doit=True): + """ + Returns the vector gradient of a scalar field computed wrt the + base scalars of the given coordinate system. + + Parameters + ========== + + scalar_field : SymPy Expr + The scalar field to compute the gradient of + + doit : bool + If True, the result is returned after calling .doit() on + each component. Else, the returned expression contains + Derivative instances + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, gradient + >>> R = CoordSys3D('R') + >>> s1 = R.x*R.y*R.z + >>> gradient(s1) + R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k + >>> s2 = 5*R.x**2*R.z + >>> gradient(s2) + 10*R.x*R.z*R.i + 5*R.x**2*R.k + + """ + coord_sys = _get_coord_systems(scalar_field) + + if len(coord_sys) == 0: + return Vector.zero + elif len(coord_sys) == 1: + coord_sys = next(iter(coord_sys)) + h1, h2, h3 = coord_sys.lame_coefficients() + i, j, k = coord_sys.base_vectors() + x, y, z = coord_sys.base_scalars() + vx = Derivative(scalar_field, x) / h1 + vy = Derivative(scalar_field, y) / h2 + vz = Derivative(scalar_field, z) / h3 + + if doit: + return (vx * i + vy * j + vz * k).doit() + return vx * i + vy * j + vz * k + else: + if isinstance(scalar_field, (Add, VectorAdd)): + return VectorAdd.fromiter(gradient(i) for i in scalar_field.args) + if isinstance(scalar_field, (Mul, VectorMul)): + s = _split_mul_args_wrt_coordsys(scalar_field) + return VectorAdd.fromiter(scalar_field / i * gradient(i) for i in s) + return Gradient(scalar_field) + + +class Laplacian(Expr): + """ + Represents unevaluated Laplacian. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Laplacian + >>> R = CoordSys3D('R') + >>> v = 3*R.x**3*R.y**2*R.z**3 + >>> Laplacian(v) + Laplacian(3*R.x**3*R.y**2*R.z**3) + + """ + + def __new__(cls, expr): + expr = sympify(expr) + obj = Expr.__new__(cls, expr) + obj._expr = expr + return obj + + def doit(self, **hints): + from sympy.vector.functions import laplacian + return laplacian(self._expr) + + +def _diff_conditional(expr, base_scalar, coeff_1, coeff_2): + """ + First re-expresses expr in the system that base_scalar belongs to. + If base_scalar appears in the re-expressed form, differentiates + it wrt base_scalar. + Else, returns 0 + """ + from sympy.vector.functions import express + new_expr = express(expr, base_scalar.system, variables=True) + arg = coeff_1 * coeff_2 * new_expr + return Derivative(arg, base_scalar) if arg else S.Zero diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/orienters.py b/mgm/lib/python3.10/site-packages/sympy/vector/orienters.py new file mode 100644 index 0000000000000000000000000000000000000000..0c22089e568bc817c943c1beecebde0fea46b6ae --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/orienters.py @@ -0,0 +1,398 @@ +from sympy.core.basic import Basic +from sympy.core.sympify import sympify +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.matrices.dense import (eye, rot_axis1, rot_axis2, rot_axis3) +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.core.cache import cacheit +from sympy.core.symbol import Str +import sympy.vector + + +class Orienter(Basic): + """ + Super-class for all orienter classes. + """ + + def rotation_matrix(self): + """ + The rotation matrix corresponding to this orienter + instance. + """ + return self._parent_orient + + +class AxisOrienter(Orienter): + """ + Class to denote an axis orienter. + """ + + def __new__(cls, angle, axis): + if not isinstance(axis, sympy.vector.Vector): + raise TypeError("axis should be a Vector") + angle = sympify(angle) + + obj = super().__new__(cls, angle, axis) + obj._angle = angle + obj._axis = axis + + return obj + + def __init__(self, angle, axis): + """ + Axis rotation is a rotation about an arbitrary axis by + some angle. The angle is supplied as a SymPy expr scalar, and + the axis is supplied as a Vector. + + Parameters + ========== + + angle : Expr + The angle by which the new system is to be rotated + + axis : Vector + The axis around which the rotation has to be performed + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q1 = symbols('q1') + >>> N = CoordSys3D('N') + >>> from sympy.vector import AxisOrienter + >>> orienter = AxisOrienter(q1, N.i + 2 * N.j) + >>> B = N.orient_new('B', (orienter, )) + + """ + # Dummy initializer for docstrings + pass + + @cacheit + def rotation_matrix(self, system): + """ + The rotation matrix corresponding to this orienter + instance. + + Parameters + ========== + + system : CoordSys3D + The coordinate system wrt which the rotation matrix + is to be computed + """ + + axis = sympy.vector.express(self.axis, system).normalize() + axis = axis.to_matrix(system) + theta = self.angle + parent_orient = ((eye(3) - axis * axis.T) * cos(theta) + + Matrix([[0, -axis[2], axis[1]], + [axis[2], 0, -axis[0]], + [-axis[1], axis[0], 0]]) * sin(theta) + + axis * axis.T) + parent_orient = parent_orient.T + return parent_orient + + @property + def angle(self): + return self._angle + + @property + def axis(self): + return self._axis + + +class ThreeAngleOrienter(Orienter): + """ + Super-class for Body and Space orienters. + """ + + def __new__(cls, angle1, angle2, angle3, rot_order): + if isinstance(rot_order, Str): + rot_order = rot_order.name + + approved_orders = ('123', '231', '312', '132', '213', + '321', '121', '131', '212', '232', + '313', '323', '') + original_rot_order = rot_order + rot_order = str(rot_order).upper() + if not (len(rot_order) == 3): + raise TypeError('rot_order should be a str of length 3') + rot_order = [i.replace('X', '1') for i in rot_order] + rot_order = [i.replace('Y', '2') for i in rot_order] + rot_order = [i.replace('Z', '3') for i in rot_order] + rot_order = ''.join(rot_order) + if rot_order not in approved_orders: + raise TypeError('Invalid rot_type parameter') + a1 = int(rot_order[0]) + a2 = int(rot_order[1]) + a3 = int(rot_order[2]) + angle1 = sympify(angle1) + angle2 = sympify(angle2) + angle3 = sympify(angle3) + if cls._in_order: + parent_orient = (_rot(a1, angle1) * + _rot(a2, angle2) * + _rot(a3, angle3)) + else: + parent_orient = (_rot(a3, angle3) * + _rot(a2, angle2) * + _rot(a1, angle1)) + parent_orient = parent_orient.T + + obj = super().__new__( + cls, angle1, angle2, angle3, Str(rot_order)) + obj._angle1 = angle1 + obj._angle2 = angle2 + obj._angle3 = angle3 + obj._rot_order = original_rot_order + obj._parent_orient = parent_orient + + return obj + + @property + def angle1(self): + return self._angle1 + + @property + def angle2(self): + return self._angle2 + + @property + def angle3(self): + return self._angle3 + + @property + def rot_order(self): + return self._rot_order + + +class BodyOrienter(ThreeAngleOrienter): + """ + Class to denote a body-orienter. + """ + + _in_order = True + + def __new__(cls, angle1, angle2, angle3, rot_order): + obj = ThreeAngleOrienter.__new__(cls, angle1, angle2, angle3, + rot_order) + return obj + + def __init__(self, angle1, angle2, angle3, rot_order): + """ + Body orientation takes this coordinate system through three + successive simple rotations. + + Body fixed rotations include both Euler Angles and + Tait-Bryan Angles, see https://en.wikipedia.org/wiki/Euler_angles. + + Parameters + ========== + + angle1, angle2, angle3 : Expr + Three successive angles to rotate the coordinate system by + + rotation_order : string + String defining the order of axes for rotation + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, BodyOrienter + >>> from sympy import symbols + >>> q1, q2, q3 = symbols('q1 q2 q3') + >>> N = CoordSys3D('N') + + A 'Body' fixed rotation is described by three angles and + three body-fixed rotation axes. To orient a coordinate system D + with respect to N, each sequential rotation is always about + the orthogonal unit vectors fixed to D. For example, a '123' + rotation will specify rotations about N.i, then D.j, then + D.k. (Initially, D.i is same as N.i) + Therefore, + + >>> body_orienter = BodyOrienter(q1, q2, q3, '123') + >>> D = N.orient_new('D', (body_orienter, )) + + is same as + + >>> from sympy.vector import AxisOrienter + >>> axis_orienter1 = AxisOrienter(q1, N.i) + >>> D = N.orient_new('D', (axis_orienter1, )) + >>> axis_orienter2 = AxisOrienter(q2, D.j) + >>> D = D.orient_new('D', (axis_orienter2, )) + >>> axis_orienter3 = AxisOrienter(q3, D.k) + >>> D = D.orient_new('D', (axis_orienter3, )) + + Acceptable rotation orders are of length 3, expressed in XYZ or + 123, and cannot have a rotation about about an axis twice in a row. + + >>> body_orienter1 = BodyOrienter(q1, q2, q3, '123') + >>> body_orienter2 = BodyOrienter(q1, q2, 0, 'ZXZ') + >>> body_orienter3 = BodyOrienter(0, 0, 0, 'XYX') + + """ + # Dummy initializer for docstrings + pass + + +class SpaceOrienter(ThreeAngleOrienter): + """ + Class to denote a space-orienter. + """ + + _in_order = False + + def __new__(cls, angle1, angle2, angle3, rot_order): + obj = ThreeAngleOrienter.__new__(cls, angle1, angle2, angle3, + rot_order) + return obj + + def __init__(self, angle1, angle2, angle3, rot_order): + """ + Space rotation is similar to Body rotation, but the rotations + are applied in the opposite order. + + Parameters + ========== + + angle1, angle2, angle3 : Expr + Three successive angles to rotate the coordinate system by + + rotation_order : string + String defining the order of axes for rotation + + See Also + ======== + + BodyOrienter : Orienter to orient systems wrt Euler angles. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, SpaceOrienter + >>> from sympy import symbols + >>> q1, q2, q3 = symbols('q1 q2 q3') + >>> N = CoordSys3D('N') + + To orient a coordinate system D with respect to N, each + sequential rotation is always about N's orthogonal unit vectors. + For example, a '123' rotation will specify rotations about + N.i, then N.j, then N.k. + Therefore, + + >>> space_orienter = SpaceOrienter(q1, q2, q3, '312') + >>> D = N.orient_new('D', (space_orienter, )) + + is same as + + >>> from sympy.vector import AxisOrienter + >>> axis_orienter1 = AxisOrienter(q1, N.i) + >>> B = N.orient_new('B', (axis_orienter1, )) + >>> axis_orienter2 = AxisOrienter(q2, N.j) + >>> C = B.orient_new('C', (axis_orienter2, )) + >>> axis_orienter3 = AxisOrienter(q3, N.k) + >>> D = C.orient_new('C', (axis_orienter3, )) + + """ + # Dummy initializer for docstrings + pass + + +class QuaternionOrienter(Orienter): + """ + Class to denote a quaternion-orienter. + """ + + def __new__(cls, q0, q1, q2, q3): + q0 = sympify(q0) + q1 = sympify(q1) + q2 = sympify(q2) + q3 = sympify(q3) + parent_orient = (Matrix([[q0 ** 2 + q1 ** 2 - q2 ** 2 - + q3 ** 2, + 2 * (q1 * q2 - q0 * q3), + 2 * (q0 * q2 + q1 * q3)], + [2 * (q1 * q2 + q0 * q3), + q0 ** 2 - q1 ** 2 + + q2 ** 2 - q3 ** 2, + 2 * (q2 * q3 - q0 * q1)], + [2 * (q1 * q3 - q0 * q2), + 2 * (q0 * q1 + q2 * q3), + q0 ** 2 - q1 ** 2 - + q2 ** 2 + q3 ** 2]])) + parent_orient = parent_orient.T + + obj = super().__new__(cls, q0, q1, q2, q3) + obj._q0 = q0 + obj._q1 = q1 + obj._q2 = q2 + obj._q3 = q3 + obj._parent_orient = parent_orient + + return obj + + def __init__(self, angle1, angle2, angle3, rot_order): + """ + Quaternion orientation orients the new CoordSys3D with + Quaternions, defined as a finite rotation about lambda, a unit + vector, by some amount theta. + + This orientation is described by four parameters: + + q0 = cos(theta/2) + + q1 = lambda_x sin(theta/2) + + q2 = lambda_y sin(theta/2) + + q3 = lambda_z sin(theta/2) + + Quaternion does not take in a rotation order. + + Parameters + ========== + + q0, q1, q2, q3 : Expr + The quaternions to rotate the coordinate system by + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy import symbols + >>> q0, q1, q2, q3 = symbols('q0 q1 q2 q3') + >>> N = CoordSys3D('N') + >>> from sympy.vector import QuaternionOrienter + >>> q_orienter = QuaternionOrienter(q0, q1, q2, q3) + >>> B = N.orient_new('B', (q_orienter, )) + + """ + # Dummy initializer for docstrings + pass + + @property + def q0(self): + return self._q0 + + @property + def q1(self): + return self._q1 + + @property + def q2(self): + return self._q2 + + @property + def q3(self): + return self._q3 + + +def _rot(axis, angle): + """DCM for simple axis 1, 2 or 3 rotations. """ + if axis == 1: + return Matrix(rot_axis1(angle).T) + elif axis == 2: + return Matrix(rot_axis2(angle).T) + elif axis == 3: + return Matrix(rot_axis3(angle).T) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/parametricregion.py b/mgm/lib/python3.10/site-packages/sympy/vector/parametricregion.py new file mode 100644 index 0000000000000000000000000000000000000000..0d55f790b52121fd982225f02505336a05536928 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/parametricregion.py @@ -0,0 +1,189 @@ +from functools import singledispatch +from sympy.core.numbers import pi +from sympy.functions.elementary.trigonometric import tan +from sympy.simplify import trigsimp +from sympy.core import Basic, Tuple +from sympy.core.symbol import _symbol +from sympy.solvers import solve +from sympy.geometry import Point, Segment, Curve, Ellipse, Polygon +from sympy.vector import ImplicitRegion + + +class ParametricRegion(Basic): + """ + Represents a parametric region in space. + + Examples + ======== + + >>> from sympy import cos, sin, pi + >>> from sympy.abc import r, theta, t, a, b, x, y + >>> from sympy.vector import ParametricRegion + + >>> ParametricRegion((t, t**2), (t, -1, 2)) + ParametricRegion((t, t**2), (t, -1, 2)) + >>> ParametricRegion((x, y), (x, 3, 4), (y, 5, 6)) + ParametricRegion((x, y), (x, 3, 4), (y, 5, 6)) + >>> ParametricRegion((r*cos(theta), r*sin(theta)), (r, -2, 2), (theta, 0, pi)) + ParametricRegion((r*cos(theta), r*sin(theta)), (r, -2, 2), (theta, 0, pi)) + >>> ParametricRegion((a*cos(t), b*sin(t)), t) + ParametricRegion((a*cos(t), b*sin(t)), t) + + >>> circle = ParametricRegion((r*cos(theta), r*sin(theta)), r, (theta, 0, pi)) + >>> circle.parameters + (r, theta) + >>> circle.definition + (r*cos(theta), r*sin(theta)) + >>> circle.limits + {theta: (0, pi)} + + Dimension of a parametric region determines whether a region is a curve, surface + or volume region. It does not represent its dimensions in space. + + >>> circle.dimensions + 1 + + Parameters + ========== + + definition : tuple to define base scalars in terms of parameters. + + bounds : Parameter or a tuple of length 3 to define parameter and corresponding lower and upper bound. + + """ + def __new__(cls, definition, *bounds): + parameters = () + limits = {} + + if not isinstance(bounds, Tuple): + bounds = Tuple(*bounds) + + for bound in bounds: + if isinstance(bound, (tuple, Tuple)): + if len(bound) != 3: + raise ValueError("Tuple should be in the form (parameter, lowerbound, upperbound)") + parameters += (bound[0],) + limits[bound[0]] = (bound[1], bound[2]) + else: + parameters += (bound,) + + if not isinstance(definition, (tuple, Tuple)): + definition = (definition,) + + obj = super().__new__(cls, Tuple(*definition), *bounds) + obj._parameters = parameters + obj._limits = limits + + return obj + + @property + def definition(self): + return self.args[0] + + @property + def limits(self): + return self._limits + + @property + def parameters(self): + return self._parameters + + @property + def dimensions(self): + return len(self.limits) + + +@singledispatch +def parametric_region_list(reg): + """ + Returns a list of ParametricRegion objects representing the geometric region. + + Examples + ======== + + >>> from sympy.abc import t + >>> from sympy.vector import parametric_region_list + >>> from sympy.geometry import Point, Curve, Ellipse, Segment, Polygon + + >>> p = Point(2, 5) + >>> parametric_region_list(p) + [ParametricRegion((2, 5))] + + >>> c = Curve((t**3, 4*t), (t, -3, 4)) + >>> parametric_region_list(c) + [ParametricRegion((t**3, 4*t), (t, -3, 4))] + + >>> e = Ellipse(Point(1, 3), 2, 3) + >>> parametric_region_list(e) + [ParametricRegion((2*cos(t) + 1, 3*sin(t) + 3), (t, 0, 2*pi))] + + >>> s = Segment(Point(1, 3), Point(2, 6)) + >>> parametric_region_list(s) + [ParametricRegion((t + 1, 3*t + 3), (t, 0, 1))] + + >>> p1, p2, p3, p4 = [(0, 1), (2, -3), (5, 3), (-2, 3)] + >>> poly = Polygon(p1, p2, p3, p4) + >>> parametric_region_list(poly) + [ParametricRegion((2*t, 1 - 4*t), (t, 0, 1)), ParametricRegion((3*t + 2, 6*t - 3), (t, 0, 1)),\ + ParametricRegion((5 - 7*t, 3), (t, 0, 1)), ParametricRegion((2*t - 2, 3 - 2*t), (t, 0, 1))] + + """ + raise ValueError("SymPy cannot determine parametric representation of the region.") + + +@parametric_region_list.register(Point) +def _(obj): + return [ParametricRegion(obj.args)] + + +@parametric_region_list.register(Curve) # type: ignore +def _(obj): + definition = obj.arbitrary_point(obj.parameter).args + bounds = obj.limits + return [ParametricRegion(definition, bounds)] + + +@parametric_region_list.register(Ellipse) # type: ignore +def _(obj, parameter='t'): + definition = obj.arbitrary_point(parameter).args + t = _symbol(parameter, real=True) + bounds = (t, 0, 2*pi) + return [ParametricRegion(definition, bounds)] + + +@parametric_region_list.register(Segment) # type: ignore +def _(obj, parameter='t'): + t = _symbol(parameter, real=True) + definition = obj.arbitrary_point(t).args + + for i in range(0, 3): + lower_bound = solve(definition[i] - obj.points[0].args[i], t) + upper_bound = solve(definition[i] - obj.points[1].args[i], t) + + if len(lower_bound) == 1 and len(upper_bound) == 1: + bounds = t, lower_bound[0], upper_bound[0] + break + + definition_tuple = obj.arbitrary_point(parameter).args + return [ParametricRegion(definition_tuple, bounds)] + + +@parametric_region_list.register(Polygon) # type: ignore +def _(obj, parameter='t'): + l = [parametric_region_list(side, parameter)[0] for side in obj.sides] + return l + + +@parametric_region_list.register(ImplicitRegion) # type: ignore +def _(obj, parameters=('t', 's')): + definition = obj.rational_parametrization(parameters) + bounds = [] + + for i in range(len(obj.variables) - 1): + # Each parameter is replaced by its tangent to simplify intergation + parameter = _symbol(parameters[i], real=True) + definition = [trigsimp(elem.subs(parameter, tan(parameter/2))) for elem in definition] + bounds.append((parameter, 0, 2*pi),) + + definition = Tuple(*definition) + return [ParametricRegion(definition, *bounds)] diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/point.py b/mgm/lib/python3.10/site-packages/sympy/vector/point.py new file mode 100644 index 0000000000000000000000000000000000000000..e46bb22d91034751d7cbf16d9de0470dc6e58cbc --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/point.py @@ -0,0 +1,151 @@ +from sympy.core.basic import Basic +from sympy.core.symbol import Str +from sympy.vector.vector import Vector +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.functions import _path +from sympy.core.cache import cacheit + + +class Point(Basic): + """ + Represents a point in 3-D space. + """ + + def __new__(cls, name, position=Vector.zero, parent_point=None): + name = str(name) + # Check the args first + if not isinstance(position, Vector): + raise TypeError( + "position should be an instance of Vector, not %s" % type( + position)) + if (not isinstance(parent_point, Point) and + parent_point is not None): + raise TypeError( + "parent_point should be an instance of Point, not %s" % type( + parent_point)) + # Super class construction + if parent_point is None: + obj = super().__new__(cls, Str(name), position) + else: + obj = super().__new__(cls, Str(name), position, parent_point) + # Decide the object parameters + obj._name = name + obj._pos = position + if parent_point is None: + obj._parent = None + obj._root = obj + else: + obj._parent = parent_point + obj._root = parent_point._root + # Return object + return obj + + @cacheit + def position_wrt(self, other): + """ + Returns the position vector of this Point with respect to + another Point/CoordSys3D. + + Parameters + ========== + + other : Point/CoordSys3D + If other is a Point, the position of this Point wrt it is + returned. If its an instance of CoordSyRect, the position + wrt its origin is returned. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> p1 = N.origin.locate_new('p1', 10 * N.i) + >>> N.origin.position_wrt(p1) + (-10)*N.i + + """ + + if (not isinstance(other, Point) and + not isinstance(other, CoordSys3D)): + raise TypeError(str(other) + + "is not a Point or CoordSys3D") + if isinstance(other, CoordSys3D): + other = other.origin + # Handle special cases + if other == self: + return Vector.zero + elif other == self._parent: + return self._pos + elif other._parent == self: + return -1 * other._pos + # Else, use point tree to calculate position + rootindex, path = _path(self, other) + result = Vector.zero + i = -1 + for i in range(rootindex): + result += path[i]._pos + i += 2 + while i < len(path): + result -= path[i]._pos + i += 1 + return result + + def locate_new(self, name, position): + """ + Returns a new Point located at the given position wrt this + Point. + Thus, the position vector of the new Point wrt this one will + be equal to the given 'position' parameter. + + Parameters + ========== + + name : str + Name of the new point + + position : Vector + The position vector of the new Point wrt this one + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> p1 = N.origin.locate_new('p1', 10 * N.i) + >>> p1.position_wrt(N.origin) + 10*N.i + + """ + return Point(name, position, self) + + def express_coordinates(self, coordinate_system): + """ + Returns the Cartesian/rectangular coordinates of this point + wrt the origin of the given CoordSys3D instance. + + Parameters + ========== + + coordinate_system : CoordSys3D + The coordinate system to express the coordinates of this + Point in. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> p1 = N.origin.locate_new('p1', 10 * N.i) + >>> p2 = p1.locate_new('p2', 5 * N.j) + >>> p2.express_coordinates(N) + (10, 5, 0) + + """ + + # Determine the position vector + pos_vect = self.position_wrt(coordinate_system.origin) + # Express it in the given coordinate system + return tuple(pos_vect.to_matrix(coordinate_system)) + + def _sympystr(self, printer): + return self._name diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/scalar.py b/mgm/lib/python3.10/site-packages/sympy/vector/scalar.py new file mode 100644 index 0000000000000000000000000000000000000000..42742b021ea5cf5a72482a1b862640f2fff0dc3b --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/scalar.py @@ -0,0 +1,69 @@ +from sympy.core import AtomicExpr, Symbol, S +from sympy.core.sympify import _sympify +from sympy.printing.pretty.stringpict import prettyForm +from sympy.printing.precedence import PRECEDENCE + + +class BaseScalar(AtomicExpr): + """ + A coordinate symbol/base scalar. + + Ideally, users should not instantiate this class. + + """ + + def __new__(cls, index, system, pretty_str=None, latex_str=None): + from sympy.vector.coordsysrect import CoordSys3D + if pretty_str is None: + pretty_str = "x{}".format(index) + elif isinstance(pretty_str, Symbol): + pretty_str = pretty_str.name + if latex_str is None: + latex_str = "x_{}".format(index) + elif isinstance(latex_str, Symbol): + latex_str = latex_str.name + + index = _sympify(index) + system = _sympify(system) + obj = super().__new__(cls, index, system) + if not isinstance(system, CoordSys3D): + raise TypeError("system should be a CoordSys3D") + if index not in range(0, 3): + raise ValueError("Invalid index specified.") + # The _id is used for equating purposes, and for hashing + obj._id = (index, system) + obj._name = obj.name = system._name + '.' + system._variable_names[index] + obj._pretty_form = '' + pretty_str + obj._latex_form = latex_str + obj._system = system + + return obj + + is_commutative = True + is_symbol = True + + @property + def free_symbols(self): + return {self} + + _diff_wrt = True + + def _eval_derivative(self, s): + if self == s: + return S.One + return S.Zero + + def _latex(self, printer=None): + return self._latex_form + + def _pretty(self, printer=None): + return prettyForm(self._pretty_form) + + precedence = PRECEDENCE['Atom'] + + @property + def system(self): + return self._system + + def _sympystr(self, printer): + return self._name diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/__init__.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/__init__.py new file mode 100644 index 0000000000000000000000000000000000000000..e69de29bb2d1d6434b8b29ae775ad8c2e48c5391 diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/__pycache__/test_dyadic.cpython-310.pyc b/mgm/lib/python3.10/site-packages/sympy/vector/tests/__pycache__/test_dyadic.cpython-310.pyc new file mode 100644 index 0000000000000000000000000000000000000000..17882e7cfe18211bf357f1a0987de3fe635ac1cd Binary files /dev/null and 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--git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_coordsysrect.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_coordsysrect.py new file mode 100644 index 0000000000000000000000000000000000000000..53eb8c89ec1643a71800efe3e370acff3cb6f9c0 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_coordsysrect.py @@ -0,0 +1,464 @@ +from sympy.testing.pytest import raises +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.scalar import BaseScalar +from sympy.core.function import expand +from sympy.core.numbers import pi +from sympy.core.symbol import symbols +from sympy.functions.elementary.hyperbolic import (cosh, sinh) +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.functions.elementary.trigonometric import (acos, atan2, cos, sin) +from sympy.matrices.dense import zeros +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.simplify.simplify import simplify +from sympy.vector.functions import express +from sympy.vector.point import Point +from sympy.vector.vector import Vector +from sympy.vector.orienters import (AxisOrienter, BodyOrienter, + SpaceOrienter, QuaternionOrienter) + + +x, y, z = symbols('x y z') +a, b, c, q = symbols('a b c q') +q1, q2, q3, q4 = symbols('q1 q2 q3 q4') + + +def test_func_args(): + A = CoordSys3D('A') + assert A.x.func(*A.x.args) == A.x + expr = 3*A.x + 4*A.y + assert expr.func(*expr.args) == expr + assert A.i.func(*A.i.args) == A.i + v = A.x*A.i + A.y*A.j + A.z*A.k + assert v.func(*v.args) == v + assert A.origin.func(*A.origin.args) == A.origin + + +def test_coordsys3d_equivalence(): + A = CoordSys3D('A') + A1 = CoordSys3D('A') + assert A1 == A + B = CoordSys3D('B') + assert A != B + + +def test_orienters(): + A = CoordSys3D('A') + axis_orienter = AxisOrienter(a, A.k) + body_orienter = BodyOrienter(a, b, c, '123') + space_orienter = SpaceOrienter(a, b, c, '123') + q_orienter = QuaternionOrienter(q1, q2, q3, q4) + assert axis_orienter.rotation_matrix(A) == Matrix([ + [ cos(a), sin(a), 0], + [-sin(a), cos(a), 0], + [ 0, 0, 1]]) + assert body_orienter.rotation_matrix() == Matrix([ + [ cos(b)*cos(c), sin(a)*sin(b)*cos(c) + sin(c)*cos(a), + sin(a)*sin(c) - sin(b)*cos(a)*cos(c)], + [-sin(c)*cos(b), -sin(a)*sin(b)*sin(c) + cos(a)*cos(c), + sin(a)*cos(c) + sin(b)*sin(c)*cos(a)], + [ sin(b), -sin(a)*cos(b), + cos(a)*cos(b)]]) + assert space_orienter.rotation_matrix() == Matrix([ + [cos(b)*cos(c), sin(c)*cos(b), -sin(b)], + [sin(a)*sin(b)*cos(c) - sin(c)*cos(a), + sin(a)*sin(b)*sin(c) + cos(a)*cos(c), sin(a)*cos(b)], + [sin(a)*sin(c) + sin(b)*cos(a)*cos(c), -sin(a)*cos(c) + + sin(b)*sin(c)*cos(a), cos(a)*cos(b)]]) + assert q_orienter.rotation_matrix() == Matrix([ + [q1**2 + q2**2 - q3**2 - q4**2, 2*q1*q4 + 2*q2*q3, + -2*q1*q3 + 2*q2*q4], + [-2*q1*q4 + 2*q2*q3, q1**2 - q2**2 + q3**2 - q4**2, + 2*q1*q2 + 2*q3*q4], + [2*q1*q3 + 2*q2*q4, + -2*q1*q2 + 2*q3*q4, q1**2 - q2**2 - q3**2 + q4**2]]) + + +def test_coordinate_vars(): + """ + Tests the coordinate variables functionality with respect to + reorientation of coordinate systems. + """ + A = CoordSys3D('A') + # Note that the name given on the lhs is different from A.x._name + assert BaseScalar(0, A, 'A_x', r'\mathbf{{x}_{A}}') == A.x + assert BaseScalar(1, A, 'A_y', r'\mathbf{{y}_{A}}') == A.y + assert BaseScalar(2, A, 'A_z', r'\mathbf{{z}_{A}}') == A.z + assert BaseScalar(0, A, 'A_x', r'\mathbf{{x}_{A}}').__hash__() == A.x.__hash__() + assert isinstance(A.x, BaseScalar) and \ + isinstance(A.y, BaseScalar) and \ + isinstance(A.z, BaseScalar) + assert A.x*A.y == A.y*A.x + assert A.scalar_map(A) == {A.x: A.x, A.y: A.y, A.z: A.z} + assert A.x.system == A + assert A.x.diff(A.x) == 1 + B = A.orient_new_axis('B', q, A.k) + assert B.scalar_map(A) == {B.z: A.z, B.y: -A.x*sin(q) + A.y*cos(q), + B.x: A.x*cos(q) + A.y*sin(q)} + assert A.scalar_map(B) == {A.x: B.x*cos(q) - B.y*sin(q), + A.y: B.x*sin(q) + B.y*cos(q), A.z: B.z} + assert express(B.x, A, variables=True) == A.x*cos(q) + A.y*sin(q) + assert express(B.y, A, variables=True) == -A.x*sin(q) + A.y*cos(q) + assert express(B.z, A, variables=True) == A.z + assert expand(express(B.x*B.y*B.z, A, variables=True)) == \ + expand(A.z*(-A.x*sin(q) + A.y*cos(q))*(A.x*cos(q) + A.y*sin(q))) + assert express(B.x*B.i + B.y*B.j + B.z*B.k, A) == \ + (B.x*cos(q) - B.y*sin(q))*A.i + (B.x*sin(q) + \ + B.y*cos(q))*A.j + B.z*A.k + assert simplify(express(B.x*B.i + B.y*B.j + B.z*B.k, A, \ + variables=True)) == \ + A.x*A.i + A.y*A.j + A.z*A.k + assert express(A.x*A.i + A.y*A.j + A.z*A.k, B) == \ + (A.x*cos(q) + A.y*sin(q))*B.i + \ + (-A.x*sin(q) + A.y*cos(q))*B.j + A.z*B.k + assert simplify(express(A.x*A.i + A.y*A.j + A.z*A.k, B, \ + variables=True)) == \ + B.x*B.i + B.y*B.j + B.z*B.k + N = B.orient_new_axis('N', -q, B.k) + assert N.scalar_map(A) == \ + {N.x: A.x, N.z: A.z, N.y: A.y} + C = A.orient_new_axis('C', q, A.i + A.j + A.k) + mapping = A.scalar_map(C) + assert mapping[A.x].equals(C.x*(2*cos(q) + 1)/3 + + C.y*(-2*sin(q + pi/6) + 1)/3 + + C.z*(-2*cos(q + pi/3) + 1)/3) + assert mapping[A.y].equals(C.x*(-2*cos(q + pi/3) + 1)/3 + + C.y*(2*cos(q) + 1)/3 + + C.z*(-2*sin(q + pi/6) + 1)/3) + assert mapping[A.z].equals(C.x*(-2*sin(q + pi/6) + 1)/3 + + C.y*(-2*cos(q + pi/3) + 1)/3 + + C.z*(2*cos(q) + 1)/3) + D = A.locate_new('D', a*A.i + b*A.j + c*A.k) + assert D.scalar_map(A) == {D.z: A.z - c, D.x: A.x - a, D.y: A.y - b} + E = A.orient_new_axis('E', a, A.k, a*A.i + b*A.j + c*A.k) + assert A.scalar_map(E) == {A.z: E.z + c, + A.x: E.x*cos(a) - E.y*sin(a) + a, + A.y: E.x*sin(a) + E.y*cos(a) + b} + assert E.scalar_map(A) == {E.x: (A.x - a)*cos(a) + (A.y - b)*sin(a), + E.y: (-A.x + a)*sin(a) + (A.y - b)*cos(a), + E.z: A.z - c} + F = A.locate_new('F', Vector.zero) + assert A.scalar_map(F) == {A.z: F.z, A.x: F.x, A.y: F.y} + + +def test_rotation_matrix(): + N = CoordSys3D('N') + A = N.orient_new_axis('A', q1, N.k) + B = A.orient_new_axis('B', q2, A.i) + C = B.orient_new_axis('C', q3, B.j) + D = N.orient_new_axis('D', q4, N.j) + E = N.orient_new_space('E', q1, q2, q3, '123') + F = N.orient_new_quaternion('F', q1, q2, q3, q4) + G = N.orient_new_body('G', q1, q2, q3, '123') + assert N.rotation_matrix(C) == Matrix([ + [- sin(q1) * sin(q2) * sin(q3) + cos(q1) * cos(q3), - sin(q1) * + cos(q2), sin(q1) * sin(q2) * cos(q3) + sin(q3) * cos(q1)], \ + [sin(q1) * cos(q3) + sin(q2) * sin(q3) * cos(q1), \ + cos(q1) * cos(q2), sin(q1) * sin(q3) - sin(q2) * cos(q1) * \ + cos(q3)], [- sin(q3) * cos(q2), sin(q2), cos(q2) * cos(q3)]]) + test_mat = D.rotation_matrix(C) - Matrix( + [[cos(q1) * cos(q3) * cos(q4) - sin(q3) * (- sin(q4) * cos(q2) + + sin(q1) * sin(q2) * cos(q4)), - sin(q2) * sin(q4) - sin(q1) * + cos(q2) * cos(q4), sin(q3) * cos(q1) * cos(q4) + cos(q3) * \ + (- sin(q4) * cos(q2) + sin(q1) * sin(q2) * cos(q4))], \ + [sin(q1) * cos(q3) + sin(q2) * sin(q3) * cos(q1), cos(q1) * \ + cos(q2), sin(q1) * sin(q3) - sin(q2) * cos(q1) * cos(q3)], \ + [sin(q4) * cos(q1) * cos(q3) - sin(q3) * (cos(q2) * cos(q4) + \ + sin(q1) * sin(q2) * \ + sin(q4)), sin(q2) * + cos(q4) - sin(q1) * sin(q4) * cos(q2), sin(q3) * \ + sin(q4) * cos(q1) + cos(q3) * (cos(q2) * cos(q4) + \ + sin(q1) * sin(q2) * sin(q4))]]) + assert test_mat.expand() == zeros(3, 3) + assert E.rotation_matrix(N) == Matrix( + [[cos(q2)*cos(q3), sin(q3)*cos(q2), -sin(q2)], + [sin(q1)*sin(q2)*cos(q3) - sin(q3)*cos(q1), \ + sin(q1)*sin(q2)*sin(q3) + cos(q1)*cos(q3), sin(q1)*cos(q2)], \ + [sin(q1)*sin(q3) + sin(q2)*cos(q1)*cos(q3), - \ + sin(q1)*cos(q3) + sin(q2)*sin(q3)*cos(q1), cos(q1)*cos(q2)]]) + assert F.rotation_matrix(N) == Matrix([[ + q1**2 + q2**2 - q3**2 - q4**2, + 2*q1*q4 + 2*q2*q3, -2*q1*q3 + 2*q2*q4],[ -2*q1*q4 + 2*q2*q3, + q1**2 - q2**2 + q3**2 - q4**2, 2*q1*q2 + 2*q3*q4], + [2*q1*q3 + 2*q2*q4, + -2*q1*q2 + 2*q3*q4, + q1**2 - q2**2 - q3**2 + q4**2]]) + assert G.rotation_matrix(N) == Matrix([[ + cos(q2)*cos(q3), sin(q1)*sin(q2)*cos(q3) + sin(q3)*cos(q1), + sin(q1)*sin(q3) - sin(q2)*cos(q1)*cos(q3)], [ + -sin(q3)*cos(q2), -sin(q1)*sin(q2)*sin(q3) + cos(q1)*cos(q3), + sin(q1)*cos(q3) + sin(q2)*sin(q3)*cos(q1)],[ + sin(q2), -sin(q1)*cos(q2), cos(q1)*cos(q2)]]) + + +def test_vector_with_orientation(): + """ + Tests the effects of orientation of coordinate systems on + basic vector operations. + """ + N = CoordSys3D('N') + A = N.orient_new_axis('A', q1, N.k) + B = A.orient_new_axis('B', q2, A.i) + C = B.orient_new_axis('C', q3, B.j) + + # Test to_matrix + v1 = a*N.i + b*N.j + c*N.k + assert v1.to_matrix(A) == Matrix([[ a*cos(q1) + b*sin(q1)], + [-a*sin(q1) + b*cos(q1)], + [ c]]) + + # Test dot + assert N.i.dot(A.i) == cos(q1) + assert N.i.dot(A.j) == -sin(q1) + assert N.i.dot(A.k) == 0 + assert N.j.dot(A.i) == sin(q1) + assert N.j.dot(A.j) == cos(q1) + assert N.j.dot(A.k) == 0 + assert N.k.dot(A.i) == 0 + assert N.k.dot(A.j) == 0 + assert N.k.dot(A.k) == 1 + + assert N.i.dot(A.i + A.j) == -sin(q1) + cos(q1) == \ + (A.i + A.j).dot(N.i) + + assert A.i.dot(C.i) == cos(q3) + assert A.i.dot(C.j) == 0 + assert A.i.dot(C.k) == sin(q3) + assert A.j.dot(C.i) == sin(q2)*sin(q3) + assert A.j.dot(C.j) == cos(q2) + assert A.j.dot(C.k) == -sin(q2)*cos(q3) + assert A.k.dot(C.i) == -cos(q2)*sin(q3) + assert A.k.dot(C.j) == sin(q2) + assert A.k.dot(C.k) == cos(q2)*cos(q3) + + # Test cross + assert N.i.cross(A.i) == sin(q1)*A.k + assert N.i.cross(A.j) == cos(q1)*A.k + assert N.i.cross(A.k) == -sin(q1)*A.i - cos(q1)*A.j + assert N.j.cross(A.i) == -cos(q1)*A.k + assert N.j.cross(A.j) == sin(q1)*A.k + assert N.j.cross(A.k) == cos(q1)*A.i - sin(q1)*A.j + assert N.k.cross(A.i) == A.j + assert N.k.cross(A.j) == -A.i + assert N.k.cross(A.k) == Vector.zero + + assert N.i.cross(A.i) == sin(q1)*A.k + assert N.i.cross(A.j) == cos(q1)*A.k + assert N.i.cross(A.i + A.j) == sin(q1)*A.k + cos(q1)*A.k + assert (A.i + A.j).cross(N.i) == (-sin(q1) - cos(q1))*N.k + + assert A.i.cross(C.i) == sin(q3)*C.j + assert A.i.cross(C.j) == -sin(q3)*C.i + cos(q3)*C.k + assert A.i.cross(C.k) == -cos(q3)*C.j + assert C.i.cross(A.i) == (-sin(q3)*cos(q2))*A.j + \ + (-sin(q2)*sin(q3))*A.k + assert C.j.cross(A.i) == (sin(q2))*A.j + (-cos(q2))*A.k + assert express(C.k.cross(A.i), C).trigsimp() == cos(q3)*C.j + + +def test_orient_new_methods(): + N = CoordSys3D('N') + orienter1 = AxisOrienter(q4, N.j) + orienter2 = SpaceOrienter(q1, q2, q3, '123') + orienter3 = QuaternionOrienter(q1, q2, q3, q4) + orienter4 = BodyOrienter(q1, q2, q3, '123') + D = N.orient_new('D', (orienter1, )) + E = N.orient_new('E', (orienter2, )) + F = N.orient_new('F', (orienter3, )) + G = N.orient_new('G', (orienter4, )) + assert D == N.orient_new_axis('D', q4, N.j) + assert E == N.orient_new_space('E', q1, q2, q3, '123') + assert F == N.orient_new_quaternion('F', q1, q2, q3, q4) + assert G == N.orient_new_body('G', q1, q2, q3, '123') + + +def test_locatenew_point(): + """ + Tests Point class, and locate_new method in CoordSys3D. + """ + A = CoordSys3D('A') + assert isinstance(A.origin, Point) + v = a*A.i + b*A.j + c*A.k + C = A.locate_new('C', v) + assert C.origin.position_wrt(A) == \ + C.position_wrt(A) == \ + C.origin.position_wrt(A.origin) == v + assert A.origin.position_wrt(C) == \ + A.position_wrt(C) == \ + A.origin.position_wrt(C.origin) == -v + assert A.origin.express_coordinates(C) == (-a, -b, -c) + p = A.origin.locate_new('p', -v) + assert p.express_coordinates(A) == (-a, -b, -c) + assert p.position_wrt(C.origin) == p.position_wrt(C) == \ + -2 * v + p1 = p.locate_new('p1', 2*v) + assert p1.position_wrt(C.origin) == Vector.zero + assert p1.express_coordinates(C) == (0, 0, 0) + p2 = p.locate_new('p2', A.i) + assert p1.position_wrt(p2) == 2*v - A.i + assert p2.express_coordinates(C) == (-2*a + 1, -2*b, -2*c) + + +def test_create_new(): + a = CoordSys3D('a') + c = a.create_new('c', transformation='spherical') + assert c._parent == a + assert c.transformation_to_parent() == \ + (c.r*sin(c.theta)*cos(c.phi), c.r*sin(c.theta)*sin(c.phi), c.r*cos(c.theta)) + assert c.transformation_from_parent() == \ + (sqrt(a.x**2 + a.y**2 + a.z**2), acos(a.z/sqrt(a.x**2 + a.y**2 + a.z**2)), atan2(a.y, a.x)) + + +def test_evalf(): + A = CoordSys3D('A') + v = 3*A.i + 4*A.j + a*A.k + assert v.n() == v.evalf() + assert v.evalf(subs={a:1}) == v.subs(a, 1).evalf() + + +def test_lame_coefficients(): + a = CoordSys3D('a', 'spherical') + assert a.lame_coefficients() == (1, a.r, sin(a.theta)*a.r) + a = CoordSys3D('a') + assert a.lame_coefficients() == (1, 1, 1) + a = CoordSys3D('a', 'cartesian') + assert a.lame_coefficients() == (1, 1, 1) + a = CoordSys3D('a', 'cylindrical') + assert a.lame_coefficients() == (1, a.r, 1) + + +def test_transformation_equations(): + + x, y, z = symbols('x y z') + # Str + a = CoordSys3D('a', transformation='spherical', + variable_names=["r", "theta", "phi"]) + r, theta, phi = a.base_scalars() + + assert r == a.r + assert theta == a.theta + assert phi == a.phi + + raises(AttributeError, lambda: a.x) + raises(AttributeError, lambda: a.y) + raises(AttributeError, lambda: a.z) + + assert a.transformation_to_parent() == ( + r*sin(theta)*cos(phi), + r*sin(theta)*sin(phi), + r*cos(theta) + ) + assert a.lame_coefficients() == (1, r, r*sin(theta)) + assert a.transformation_from_parent_function()(x, y, z) == ( + sqrt(x ** 2 + y ** 2 + z ** 2), + acos((z) / sqrt(x**2 + y**2 + z**2)), + atan2(y, x) + ) + a = CoordSys3D('a', transformation='cylindrical', + variable_names=["r", "theta", "z"]) + r, theta, z = a.base_scalars() + assert a.transformation_to_parent() == ( + r*cos(theta), + r*sin(theta), + z + ) + assert a.lame_coefficients() == (1, a.r, 1) + assert a.transformation_from_parent_function()(x, y, z) == (sqrt(x**2 + y**2), + atan2(y, x), z) + + a = CoordSys3D('a', 'cartesian') + assert a.transformation_to_parent() == (a.x, a.y, a.z) + assert a.lame_coefficients() == (1, 1, 1) + assert a.transformation_from_parent_function()(x, y, z) == (x, y, z) + + # Variables and expressions + + # Cartesian with equation tuple: + x, y, z = symbols('x y z') + a = CoordSys3D('a', ((x, y, z), (x, y, z))) + a._calculate_inv_trans_equations() + assert a.transformation_to_parent() == (a.x1, a.x2, a.x3) + assert a.lame_coefficients() == (1, 1, 1) + assert a.transformation_from_parent_function()(x, y, z) == (x, y, z) + r, theta, z = symbols("r theta z") + + # Cylindrical with equation tuple: + a = CoordSys3D('a', [(r, theta, z), (r*cos(theta), r*sin(theta), z)], + variable_names=["r", "theta", "z"]) + r, theta, z = a.base_scalars() + assert a.transformation_to_parent() == ( + r*cos(theta), r*sin(theta), z + ) + assert a.lame_coefficients() == ( + sqrt(sin(theta)**2 + cos(theta)**2), + sqrt(r**2*sin(theta)**2 + r**2*cos(theta)**2), + 1 + ) # ==> this should simplify to (1, r, 1), tests are too slow with `simplify`. + + # Definitions with `lambda`: + + # Cartesian with `lambda` + a = CoordSys3D('a', lambda x, y, z: (x, y, z)) + assert a.transformation_to_parent() == (a.x1, a.x2, a.x3) + assert a.lame_coefficients() == (1, 1, 1) + a._calculate_inv_trans_equations() + assert a.transformation_from_parent_function()(x, y, z) == (x, y, z) + + # Spherical with `lambda` + a = CoordSys3D('a', lambda r, theta, phi: (r*sin(theta)*cos(phi), r*sin(theta)*sin(phi), r*cos(theta)), + variable_names=["r", "theta", "phi"]) + r, theta, phi = a.base_scalars() + assert a.transformation_to_parent() == ( + r*sin(theta)*cos(phi), r*sin(phi)*sin(theta), r*cos(theta) + ) + assert a.lame_coefficients() == ( + sqrt(sin(phi)**2*sin(theta)**2 + sin(theta)**2*cos(phi)**2 + cos(theta)**2), + sqrt(r**2*sin(phi)**2*cos(theta)**2 + r**2*sin(theta)**2 + r**2*cos(phi)**2*cos(theta)**2), + sqrt(r**2*sin(phi)**2*sin(theta)**2 + r**2*sin(theta)**2*cos(phi)**2) + ) # ==> this should simplify to (1, r, sin(theta)*r), `simplify` is too slow. + + # Cylindrical with `lambda` + a = CoordSys3D('a', lambda r, theta, z: + (r*cos(theta), r*sin(theta), z), + variable_names=["r", "theta", "z"] + ) + r, theta, z = a.base_scalars() + assert a.transformation_to_parent() == (r*cos(theta), r*sin(theta), z) + assert a.lame_coefficients() == ( + sqrt(sin(theta)**2 + cos(theta)**2), + sqrt(r**2*sin(theta)**2 + r**2*cos(theta)**2), + 1 + ) # ==> this should simplify to (1, a.x, 1) + + raises(TypeError, lambda: CoordSys3D('a', transformation={ + x: x*sin(y)*cos(z), y:x*sin(y)*sin(z), z: x*cos(y)})) + + +def test_check_orthogonality(): + x, y, z = symbols('x y z') + u,v = symbols('u, v') + a = CoordSys3D('a', transformation=((x, y, z), (x*sin(y)*cos(z), x*sin(y)*sin(z), x*cos(y)))) + assert a._check_orthogonality(a._transformation) is True + a = CoordSys3D('a', transformation=((x, y, z), (x * cos(y), x * sin(y), z))) + assert a._check_orthogonality(a._transformation) is True + a = CoordSys3D('a', transformation=((u, v, z), (cosh(u) * cos(v), sinh(u) * sin(v), z))) + assert a._check_orthogonality(a._transformation) is True + + raises(ValueError, lambda: CoordSys3D('a', transformation=((x, y, z), (x, x, z)))) + raises(ValueError, lambda: CoordSys3D('a', transformation=( + (x, y, z), (x*sin(y/2)*cos(z), x*sin(y)*sin(z), x*cos(y))))) + + +def test_rotation_trans_equations(): + a = CoordSys3D('a') + from sympy.core.symbol import symbols + q0 = symbols('q0') + assert a._rotation_trans_equations(a._parent_rotation_matrix, a.base_scalars()) == (a.x, a.y, a.z) + assert a._rotation_trans_equations(a._inverse_rotation_matrix(), a.base_scalars()) == (a.x, a.y, a.z) + b = a.orient_new_axis('b', 0, -a.k) + assert b._rotation_trans_equations(b._parent_rotation_matrix, b.base_scalars()) == (b.x, b.y, b.z) + assert b._rotation_trans_equations(b._inverse_rotation_matrix(), b.base_scalars()) == (b.x, b.y, b.z) + c = a.orient_new_axis('c', q0, -a.k) + assert c._rotation_trans_equations(c._parent_rotation_matrix, c.base_scalars()) == \ + (-sin(q0) * c.y + cos(q0) * c.x, sin(q0) * c.x + cos(q0) * c.y, c.z) + assert c._rotation_trans_equations(c._inverse_rotation_matrix(), c.base_scalars()) == \ + (sin(q0) * c.y + cos(q0) * c.x, -sin(q0) * c.x + cos(q0) * c.y, c.z) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_dyadic.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_dyadic.py new file mode 100644 index 0000000000000000000000000000000000000000..2e396fcf2a81af897b59c0065f6b15f5c6933222 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_dyadic.py @@ -0,0 +1,134 @@ +from sympy.core.numbers import pi +from sympy.core.symbol import symbols +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.simplify.simplify import simplify +from sympy.vector import (CoordSys3D, Vector, Dyadic, + DyadicAdd, DyadicMul, DyadicZero, + BaseDyadic, express) + + +A = CoordSys3D('A') + + +def test_dyadic(): + a, b = symbols('a, b') + assert Dyadic.zero != 0 + assert isinstance(Dyadic.zero, DyadicZero) + assert BaseDyadic(A.i, A.j) != BaseDyadic(A.j, A.i) + assert (BaseDyadic(Vector.zero, A.i) == + BaseDyadic(A.i, Vector.zero) == Dyadic.zero) + + d1 = A.i | A.i + d2 = A.j | A.j + d3 = A.i | A.j + + assert isinstance(d1, BaseDyadic) + d_mul = a*d1 + assert isinstance(d_mul, DyadicMul) + assert d_mul.base_dyadic == d1 + assert d_mul.measure_number == a + assert isinstance(a*d1 + b*d3, DyadicAdd) + assert d1 == A.i.outer(A.i) + assert d3 == A.i.outer(A.j) + v1 = a*A.i - A.k + v2 = A.i + b*A.j + assert v1 | v2 == v1.outer(v2) == a * (A.i|A.i) + (a*b) * (A.i|A.j) +\ + - (A.k|A.i) - b * (A.k|A.j) + assert d1 * 0 == Dyadic.zero + assert d1 != Dyadic.zero + assert d1 * 2 == 2 * (A.i | A.i) + assert d1 / 2. == 0.5 * d1 + + assert d1.dot(0 * d1) == Vector.zero + assert d1 & d2 == Dyadic.zero + assert d1.dot(A.i) == A.i == d1 & A.i + + assert d1.cross(Vector.zero) == Dyadic.zero + assert d1.cross(A.i) == Dyadic.zero + assert d1 ^ A.j == d1.cross(A.j) + assert d1.cross(A.k) == - A.i | A.j + assert d2.cross(A.i) == - A.j | A.k == d2 ^ A.i + + assert A.i ^ d1 == Dyadic.zero + assert A.j.cross(d1) == - A.k | A.i == A.j ^ d1 + assert Vector.zero.cross(d1) == Dyadic.zero + assert A.k ^ d1 == A.j | A.i + assert A.i.dot(d1) == A.i & d1 == A.i + assert A.j.dot(d1) == Vector.zero + assert Vector.zero.dot(d1) == Vector.zero + assert A.j & d2 == A.j + + assert d1.dot(d3) == d1 & d3 == A.i | A.j == d3 + assert d3 & d1 == Dyadic.zero + + q = symbols('q') + B = A.orient_new_axis('B', q, A.k) + assert express(d1, B) == express(d1, B, B) + + expr1 = ((cos(q)**2) * (B.i | B.i) + (-sin(q) * cos(q)) * + (B.i | B.j) + (-sin(q) * cos(q)) * (B.j | B.i) + (sin(q)**2) * + (B.j | B.j)) + assert (express(d1, B) - expr1).simplify() == Dyadic.zero + + expr2 = (cos(q)) * (B.i | A.i) + (-sin(q)) * (B.j | A.i) + assert (express(d1, B, A) - expr2).simplify() == Dyadic.zero + + expr3 = (cos(q)) * (A.i | B.i) + (-sin(q)) * (A.i | B.j) + assert (express(d1, A, B) - expr3).simplify() == Dyadic.zero + + assert d1.to_matrix(A) == Matrix([[1, 0, 0], [0, 0, 0], [0, 0, 0]]) + assert d1.to_matrix(A, B) == Matrix([[cos(q), -sin(q), 0], + [0, 0, 0], + [0, 0, 0]]) + assert d3.to_matrix(A) == Matrix([[0, 1, 0], [0, 0, 0], [0, 0, 0]]) + a, b, c, d, e, f = symbols('a, b, c, d, e, f') + v1 = a * A.i + b * A.j + c * A.k + v2 = d * A.i + e * A.j + f * A.k + d4 = v1.outer(v2) + assert d4.to_matrix(A) == Matrix([[a * d, a * e, a * f], + [b * d, b * e, b * f], + [c * d, c * e, c * f]]) + d5 = v1.outer(v1) + C = A.orient_new_axis('C', q, A.i) + for expected, actual in zip(C.rotation_matrix(A) * d5.to_matrix(A) * \ + C.rotation_matrix(A).T, d5.to_matrix(C)): + assert (expected - actual).simplify() == 0 + + +def test_dyadic_simplify(): + x, y, z, k, n, m, w, f, s, A = symbols('x, y, z, k, n, m, w, f, s, A') + N = CoordSys3D('N') + + dy = N.i | N.i + test1 = (1 / x + 1 / y) * dy + assert (N.i & test1 & N.i) != (x + y) / (x * y) + test1 = test1.simplify() + assert test1.simplify() == simplify(test1) + assert (N.i & test1 & N.i) == (x + y) / (x * y) + + test2 = (A**2 * s**4 / (4 * pi * k * m**3)) * dy + test2 = test2.simplify() + assert (N.i & test2 & N.i) == (A**2 * s**4 / (4 * pi * k * m**3)) + + test3 = ((4 + 4 * x - 2 * (2 + 2 * x)) / (2 + 2 * x)) * dy + test3 = test3.simplify() + assert (N.i & test3 & N.i) == 0 + + test4 = ((-4 * x * y**2 - 2 * y**3 - 2 * x**2 * y) / (x + y)**2) * dy + test4 = test4.simplify() + assert (N.i & test4 & N.i) == -2 * y + + +def test_dyadic_srepr(): + from sympy.printing.repr import srepr + N = CoordSys3D('N') + + dy = N.i | N.j + res = "BaseDyadic(CoordSys3D(Str('N'), Tuple(ImmutableDenseMatrix([["\ + "Integer(1), Integer(0), Integer(0)], [Integer(0), Integer(1), "\ + "Integer(0)], [Integer(0), Integer(0), Integer(1)]]), "\ + "VectorZero())).i, CoordSys3D(Str('N'), Tuple(ImmutableDenseMatrix("\ + "[[Integer(1), Integer(0), Integer(0)], [Integer(0), Integer(1), "\ + "Integer(0)], [Integer(0), Integer(0), Integer(1)]]), VectorZero())).j)" + assert srepr(dy) == res diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_field_functions.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_field_functions.py new file mode 100644 index 0000000000000000000000000000000000000000..035c2ce0234b81069c5ad8dcb1c74f4de0164a8f --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_field_functions.py @@ -0,0 +1,321 @@ +from sympy.core.function import Derivative +from sympy.vector.vector import Vector +from sympy.vector.coordsysrect import CoordSys3D +from sympy.simplify import simplify +from sympy.core.symbol import symbols +from sympy.core import S +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.vector.vector import Dot +from sympy.vector.operators import curl, divergence, gradient, Gradient, Divergence, Cross +from sympy.vector.deloperator import Del +from sympy.vector.functions import (is_conservative, is_solenoidal, + scalar_potential, directional_derivative, + laplacian, scalar_potential_difference) +from sympy.testing.pytest import raises + +C = CoordSys3D('C') +i, j, k = C.base_vectors() +x, y, z = C.base_scalars() +delop = Del() +a, b, c, q = symbols('a b c q') + + +def test_del_operator(): + # Tests for curl + + assert delop ^ Vector.zero == Vector.zero + assert ((delop ^ Vector.zero).doit() == Vector.zero == + curl(Vector.zero)) + assert delop.cross(Vector.zero) == delop ^ Vector.zero + assert (delop ^ i).doit() == Vector.zero + assert delop.cross(2*y**2*j, doit=True) == Vector.zero + assert delop.cross(2*y**2*j) == delop ^ 2*y**2*j + v = x*y*z * (i + j + k) + assert ((delop ^ v).doit() == + (-x*y + x*z)*i + (x*y - y*z)*j + (-x*z + y*z)*k == + curl(v)) + assert delop ^ v == delop.cross(v) + assert (delop.cross(2*x**2*j) == + (Derivative(0, C.y) - Derivative(2*C.x**2, C.z))*C.i + + (-Derivative(0, C.x) + Derivative(0, C.z))*C.j + + (-Derivative(0, C.y) + Derivative(2*C.x**2, C.x))*C.k) + assert (delop.cross(2*x**2*j, doit=True) == 4*x*k == + curl(2*x**2*j)) + + #Tests for divergence + assert delop & Vector.zero is S.Zero == divergence(Vector.zero) + assert (delop & Vector.zero).doit() is S.Zero + assert delop.dot(Vector.zero) == delop & Vector.zero + assert (delop & i).doit() is S.Zero + assert (delop & x**2*i).doit() == 2*x == divergence(x**2*i) + assert (delop.dot(v, doit=True) == x*y + y*z + z*x == + divergence(v)) + assert delop & v == delop.dot(v) + assert delop.dot(1/(x*y*z) * (i + j + k), doit=True) == \ + - 1 / (x*y*z**2) - 1 / (x*y**2*z) - 1 / (x**2*y*z) + v = x*i + y*j + z*k + assert (delop & v == Derivative(C.x, C.x) + + Derivative(C.y, C.y) + Derivative(C.z, C.z)) + assert delop.dot(v, doit=True) == 3 == divergence(v) + assert delop & v == delop.dot(v) + assert simplify((delop & v).doit()) == 3 + + #Tests for gradient + assert (delop.gradient(0, doit=True) == Vector.zero == + gradient(0)) + assert delop.gradient(0) == delop(0) + assert (delop(S.Zero)).doit() == Vector.zero + assert (delop(x) == (Derivative(C.x, C.x))*C.i + + (Derivative(C.x, C.y))*C.j + (Derivative(C.x, C.z))*C.k) + assert (delop(x)).doit() == i == gradient(x) + assert (delop(x*y*z) == + (Derivative(C.x*C.y*C.z, C.x))*C.i + + (Derivative(C.x*C.y*C.z, C.y))*C.j + + (Derivative(C.x*C.y*C.z, C.z))*C.k) + assert (delop.gradient(x*y*z, doit=True) == + y*z*i + z*x*j + x*y*k == + gradient(x*y*z)) + assert delop(x*y*z) == delop.gradient(x*y*z) + assert (delop(2*x**2)).doit() == 4*x*i + assert ((delop(a*sin(y) / x)).doit() == + -a*sin(y)/x**2 * i + a*cos(y)/x * j) + + #Tests for directional derivative + assert (Vector.zero & delop)(a) is S.Zero + assert ((Vector.zero & delop)(a)).doit() is S.Zero + assert ((v & delop)(Vector.zero)).doit() == Vector.zero + assert ((v & delop)(S.Zero)).doit() is S.Zero + assert ((i & delop)(x)).doit() == 1 + assert ((j & delop)(y)).doit() == 1 + assert ((k & delop)(z)).doit() == 1 + assert ((i & delop)(x*y*z)).doit() == y*z + assert ((v & delop)(x)).doit() == x + assert ((v & delop)(x*y*z)).doit() == 3*x*y*z + assert (v & delop)(x + y + z) == C.x + C.y + C.z + assert ((v & delop)(x + y + z)).doit() == x + y + z + assert ((v & delop)(v)).doit() == v + assert ((i & delop)(v)).doit() == i + assert ((j & delop)(v)).doit() == j + assert ((k & delop)(v)).doit() == k + assert ((v & delop)(Vector.zero)).doit() == Vector.zero + + # Tests for laplacian on scalar fields + assert laplacian(x*y*z) is S.Zero + assert laplacian(x**2) == S(2) + assert laplacian(x**2*y**2*z**2) == \ + 2*y**2*z**2 + 2*x**2*z**2 + 2*x**2*y**2 + A = CoordSys3D('A', transformation="spherical", variable_names=["r", "theta", "phi"]) + B = CoordSys3D('B', transformation='cylindrical', variable_names=["r", "theta", "z"]) + assert laplacian(A.r + A.theta + A.phi) == 2/A.r + cos(A.theta)/(A.r**2*sin(A.theta)) + assert laplacian(B.r + B.theta + B.z) == 1/B.r + + # Tests for laplacian on vector fields + assert laplacian(x*y*z*(i + j + k)) == Vector.zero + assert laplacian(x*y**2*z*(i + j + k)) == \ + 2*x*z*i + 2*x*z*j + 2*x*z*k + + +def test_product_rules(): + """ + Tests the six product rules defined with respect to the Del + operator + + References + ========== + + .. [1] https://en.wikipedia.org/wiki/Del + + """ + + #Define the scalar and vector functions + f = 2*x*y*z + g = x*y + y*z + z*x + u = x**2*i + 4*j - y**2*z*k + v = 4*i + x*y*z*k + + # First product rule + lhs = delop(f * g, doit=True) + rhs = (f * delop(g) + g * delop(f)).doit() + assert simplify(lhs) == simplify(rhs) + + # Second product rule + lhs = delop(u & v).doit() + rhs = ((u ^ (delop ^ v)) + (v ^ (delop ^ u)) + \ + ((u & delop)(v)) + ((v & delop)(u))).doit() + assert simplify(lhs) == simplify(rhs) + + # Third product rule + lhs = (delop & (f*v)).doit() + rhs = ((f * (delop & v)) + (v & (delop(f)))).doit() + assert simplify(lhs) == simplify(rhs) + + # Fourth product rule + lhs = (delop & (u ^ v)).doit() + rhs = ((v & (delop ^ u)) - (u & (delop ^ v))).doit() + assert simplify(lhs) == simplify(rhs) + + # Fifth product rule + lhs = (delop ^ (f * v)).doit() + rhs = (((delop(f)) ^ v) + (f * (delop ^ v))).doit() + assert simplify(lhs) == simplify(rhs) + + # Sixth product rule + lhs = (delop ^ (u ^ v)).doit() + rhs = (u * (delop & v) - v * (delop & u) + + (v & delop)(u) - (u & delop)(v)).doit() + assert simplify(lhs) == simplify(rhs) + + +P = C.orient_new_axis('P', q, C.k) # type: ignore +scalar_field = 2*x**2*y*z +grad_field = gradient(scalar_field) +vector_field = y**2*i + 3*x*j + 5*y*z*k +curl_field = curl(vector_field) + + +def test_conservative(): + assert is_conservative(Vector.zero) is True + assert is_conservative(i) is True + assert is_conservative(2 * i + 3 * j + 4 * k) is True + assert (is_conservative(y*z*i + x*z*j + x*y*k) is + True) + assert is_conservative(x * j) is False + assert is_conservative(grad_field) is True + assert is_conservative(curl_field) is False + assert (is_conservative(4*x*y*z*i + 2*x**2*z*j) is + False) + assert is_conservative(z*P.i + P.x*k) is True + + +def test_solenoidal(): + assert is_solenoidal(Vector.zero) is True + assert is_solenoidal(i) is True + assert is_solenoidal(2 * i + 3 * j + 4 * k) is True + assert (is_solenoidal(y*z*i + x*z*j + x*y*k) is + True) + assert is_solenoidal(y * j) is False + assert is_solenoidal(grad_field) is False + assert is_solenoidal(curl_field) is True + assert is_solenoidal((-2*y + 3)*k) is True + assert is_solenoidal(cos(q)*i + sin(q)*j + cos(q)*P.k) is True + assert is_solenoidal(z*P.i + P.x*k) is True + + +def test_directional_derivative(): + assert directional_derivative(C.x*C.y*C.z, 3*C.i + 4*C.j + C.k) == C.x*C.y + 4*C.x*C.z + 3*C.y*C.z + assert directional_derivative(5*C.x**2*C.z, 3*C.i + 4*C.j + C.k) == 5*C.x**2 + 30*C.x*C.z + assert directional_derivative(5*C.x**2*C.z, 4*C.j) is S.Zero + + D = CoordSys3D("D", "spherical", variable_names=["r", "theta", "phi"], + vector_names=["e_r", "e_theta", "e_phi"]) + r, theta, phi = D.base_scalars() + e_r, e_theta, e_phi = D.base_vectors() + assert directional_derivative(r**2*e_r, e_r) == 2*r*e_r + assert directional_derivative(5*r**2*phi, 3*e_r + 4*e_theta + e_phi) == 5*r**2 + 30*r*phi + + +def test_scalar_potential(): + assert scalar_potential(Vector.zero, C) == 0 + assert scalar_potential(i, C) == x + assert scalar_potential(j, C) == y + assert scalar_potential(k, C) == z + assert scalar_potential(y*z*i + x*z*j + x*y*k, C) == x*y*z + assert scalar_potential(grad_field, C) == scalar_field + assert scalar_potential(z*P.i + P.x*k, C) == x*z*cos(q) + y*z*sin(q) + assert scalar_potential(z*P.i + P.x*k, P) == P.x*P.z + raises(ValueError, lambda: scalar_potential(x*j, C)) + + +def test_scalar_potential_difference(): + point1 = C.origin.locate_new('P1', 1*i + 2*j + 3*k) + point2 = C.origin.locate_new('P2', 4*i + 5*j + 6*k) + genericpointC = C.origin.locate_new('RP', x*i + y*j + z*k) + genericpointP = P.origin.locate_new('PP', P.x*P.i + P.y*P.j + P.z*P.k) + assert scalar_potential_difference(S.Zero, C, point1, point2) == 0 + assert (scalar_potential_difference(scalar_field, C, C.origin, + genericpointC) == + scalar_field) + assert (scalar_potential_difference(grad_field, C, C.origin, + genericpointC) == + scalar_field) + assert scalar_potential_difference(grad_field, C, point1, point2) == 948 + assert (scalar_potential_difference(y*z*i + x*z*j + + x*y*k, C, point1, + genericpointC) == + x*y*z - 6) + potential_diff_P = (2*P.z*(P.x*sin(q) + P.y*cos(q))* + (P.x*cos(q) - P.y*sin(q))**2) + assert (scalar_potential_difference(grad_field, P, P.origin, + genericpointP).simplify() == + potential_diff_P.simplify()) + + +def test_differential_operators_curvilinear_system(): + A = CoordSys3D('A', transformation="spherical", variable_names=["r", "theta", "phi"]) + B = CoordSys3D('B', transformation='cylindrical', variable_names=["r", "theta", "z"]) + # Test for spherical coordinate system and gradient + assert gradient(3*A.r + 4*A.theta) == 3*A.i + 4/A.r*A.j + assert gradient(3*A.r*A.phi + 4*A.theta) == 3*A.phi*A.i + 4/A.r*A.j + (3/sin(A.theta))*A.k + assert gradient(0*A.r + 0*A.theta+0*A.phi) == Vector.zero + assert gradient(A.r*A.theta*A.phi) == A.theta*A.phi*A.i + A.phi*A.j + (A.theta/sin(A.theta))*A.k + # Test for spherical coordinate system and divergence + assert divergence(A.r * A.i + A.theta * A.j + A.phi * A.k) == \ + (sin(A.theta)*A.r + cos(A.theta)*A.r*A.theta)/(sin(A.theta)*A.r**2) + 3 + 1/(sin(A.theta)*A.r) + assert divergence(3*A.r*A.phi*A.i + A.theta*A.j + A.r*A.theta*A.phi*A.k) == \ + (sin(A.theta)*A.r + cos(A.theta)*A.r*A.theta)/(sin(A.theta)*A.r**2) + 9*A.phi + A.theta/sin(A.theta) + assert divergence(Vector.zero) == 0 + assert divergence(0*A.i + 0*A.j + 0*A.k) == 0 + # Test for spherical coordinate system and curl + assert curl(A.r*A.i + A.theta*A.j + A.phi*A.k) == \ + (cos(A.theta)*A.phi/(sin(A.theta)*A.r))*A.i + (-A.phi/A.r)*A.j + A.theta/A.r*A.k + assert curl(A.r*A.j + A.phi*A.k) == (cos(A.theta)*A.phi/(sin(A.theta)*A.r))*A.i + (-A.phi/A.r)*A.j + 2*A.k + + # Test for cylindrical coordinate system and gradient + assert gradient(0*B.r + 0*B.theta+0*B.z) == Vector.zero + assert gradient(B.r*B.theta*B.z) == B.theta*B.z*B.i + B.z*B.j + B.r*B.theta*B.k + assert gradient(3*B.r) == 3*B.i + assert gradient(2*B.theta) == 2/B.r * B.j + assert gradient(4*B.z) == 4*B.k + # Test for cylindrical coordinate system and divergence + assert divergence(B.r*B.i + B.theta*B.j + B.z*B.k) == 3 + 1/B.r + assert divergence(B.r*B.j + B.z*B.k) == 1 + # Test for cylindrical coordinate system and curl + assert curl(B.r*B.j + B.z*B.k) == 2*B.k + assert curl(3*B.i + 2/B.r*B.j + 4*B.k) == Vector.zero + +def test_mixed_coordinates(): + # gradient + a = CoordSys3D('a') + b = CoordSys3D('b') + c = CoordSys3D('c') + assert gradient(a.x*b.y) == b.y*a.i + a.x*b.j + assert gradient(3*cos(q)*a.x*b.x+a.y*(a.x+(cos(q)+b.x))) ==\ + (a.y + 3*b.x*cos(q))*a.i + (a.x + b.x + cos(q))*a.j + (3*a.x*cos(q) + a.y)*b.i + # Some tests need further work: + # assert gradient(a.x*(cos(a.x+b.x))) == (cos(a.x + b.x))*a.i + a.x*Gradient(cos(a.x + b.x)) + # assert gradient(cos(a.x + b.x)*cos(a.x + b.z)) == Gradient(cos(a.x + b.x)*cos(a.x + b.z)) + assert gradient(a.x**b.y) == Gradient(a.x**b.y) + # assert gradient(cos(a.x+b.y)*a.z) == None + assert gradient(cos(a.x*b.y)) == Gradient(cos(a.x*b.y)) + assert gradient(3*cos(q)*a.x*b.x*a.z*a.y+ b.y*b.z + cos(a.x+a.y)*b.z) == \ + (3*a.y*a.z*b.x*cos(q) - b.z*sin(a.x + a.y))*a.i + \ + (3*a.x*a.z*b.x*cos(q) - b.z*sin(a.x + a.y))*a.j + (3*a.x*a.y*b.x*cos(q))*a.k + \ + (3*a.x*a.y*a.z*cos(q))*b.i + b.z*b.j + (b.y + cos(a.x + a.y))*b.k + # divergence + assert divergence(a.i*a.x+a.j*a.y+a.z*a.k + b.i*b.x+b.j*b.y+b.z*b.k + c.i*c.x+c.j*c.y+c.z*c.k) == S(9) + # assert divergence(3*a.i*a.x*cos(a.x+b.z) + a.j*b.x*c.z) == None + assert divergence(3*a.i*a.x*a.z + b.j*b.x*c.z + 3*a.j*a.z*a.y) == \ + 6*a.z + b.x*Dot(b.j, c.k) + assert divergence(3*cos(q)*a.x*b.x*b.i*c.x) == \ + 3*a.x*b.x*cos(q)*Dot(b.i, c.i) + 3*a.x*c.x*cos(q) + 3*b.x*c.x*cos(q)*Dot(b.i, a.i) + assert divergence(a.x*b.x*c.x*Cross(a.x*a.i, a.y*b.j)) ==\ + a.x*b.x*c.x*Divergence(Cross(a.x*a.i, a.y*b.j)) + \ + b.x*c.x*Dot(Cross(a.x*a.i, a.y*b.j), a.i) + \ + a.x*c.x*Dot(Cross(a.x*a.i, a.y*b.j), b.i) + \ + a.x*b.x*Dot(Cross(a.x*a.i, a.y*b.j), c.i) + assert divergence(a.x*b.x*c.x*(a.x*a.i + b.x*b.i)) == \ + 4*a.x*b.x*c.x +\ + a.x**2*c.x*Dot(a.i, b.i) +\ + a.x**2*b.x*Dot(a.i, c.i) +\ + b.x**2*c.x*Dot(b.i, a.i) +\ + a.x*b.x**2*Dot(b.i, c.i) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_functions.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_functions.py new file mode 100644 index 0000000000000000000000000000000000000000..dfdf9821b6c853755ce12d0cbdfa599bd4f312e4 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_functions.py @@ -0,0 +1,184 @@ +from sympy.vector.vector import Vector +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.functions import express, matrix_to_vector, orthogonalize +from sympy.core.numbers import Rational +from sympy.core.singleton import S +from sympy.core.symbol import symbols +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.testing.pytest import raises + +N = CoordSys3D('N') +q1, q2, q3, q4, q5 = symbols('q1 q2 q3 q4 q5') +A = N.orient_new_axis('A', q1, N.k) # type: ignore +B = A.orient_new_axis('B', q2, A.i) +C = B.orient_new_axis('C', q3, B.j) + + +def test_express(): + assert express(Vector.zero, N) == Vector.zero + assert express(S.Zero, N) is S.Zero + assert express(A.i, C) == cos(q3)*C.i + sin(q3)*C.k + assert express(A.j, C) == sin(q2)*sin(q3)*C.i + cos(q2)*C.j - \ + sin(q2)*cos(q3)*C.k + assert express(A.k, C) == -sin(q3)*cos(q2)*C.i + sin(q2)*C.j + \ + cos(q2)*cos(q3)*C.k + assert express(A.i, N) == cos(q1)*N.i + sin(q1)*N.j + assert express(A.j, N) == -sin(q1)*N.i + cos(q1)*N.j + assert express(A.k, N) == N.k + assert express(A.i, A) == A.i + assert express(A.j, A) == A.j + assert express(A.k, A) == A.k + assert express(A.i, B) == B.i + assert express(A.j, B) == cos(q2)*B.j - sin(q2)*B.k + assert express(A.k, B) == sin(q2)*B.j + cos(q2)*B.k + assert express(A.i, C) == cos(q3)*C.i + sin(q3)*C.k + assert express(A.j, C) == sin(q2)*sin(q3)*C.i + cos(q2)*C.j - \ + sin(q2)*cos(q3)*C.k + assert express(A.k, C) == -sin(q3)*cos(q2)*C.i + sin(q2)*C.j + \ + cos(q2)*cos(q3)*C.k + # Check to make sure UnitVectors get converted properly + assert express(N.i, N) == N.i + assert express(N.j, N) == N.j + assert express(N.k, N) == N.k + assert express(N.i, A) == (cos(q1)*A.i - sin(q1)*A.j) + assert express(N.j, A) == (sin(q1)*A.i + cos(q1)*A.j) + assert express(N.k, A) == A.k + assert express(N.i, B) == (cos(q1)*B.i - sin(q1)*cos(q2)*B.j + + sin(q1)*sin(q2)*B.k) + assert express(N.j, B) == (sin(q1)*B.i + cos(q1)*cos(q2)*B.j - + sin(q2)*cos(q1)*B.k) + assert express(N.k, B) == (sin(q2)*B.j + cos(q2)*B.k) + assert express(N.i, C) == ( + (cos(q1)*cos(q3) - sin(q1)*sin(q2)*sin(q3))*C.i - + sin(q1)*cos(q2)*C.j + + (sin(q3)*cos(q1) + sin(q1)*sin(q2)*cos(q3))*C.k) + assert express(N.j, C) == ( + (sin(q1)*cos(q3) + sin(q2)*sin(q3)*cos(q1))*C.i + + cos(q1)*cos(q2)*C.j + + (sin(q1)*sin(q3) - sin(q2)*cos(q1)*cos(q3))*C.k) + assert express(N.k, C) == (-sin(q3)*cos(q2)*C.i + sin(q2)*C.j + + cos(q2)*cos(q3)*C.k) + + assert express(A.i, N) == (cos(q1)*N.i + sin(q1)*N.j) + assert express(A.j, N) == (-sin(q1)*N.i + cos(q1)*N.j) + assert express(A.k, N) == N.k + assert express(A.i, A) == A.i + assert express(A.j, A) == A.j + assert express(A.k, A) == A.k + assert express(A.i, B) == B.i + assert express(A.j, B) == (cos(q2)*B.j - sin(q2)*B.k) + assert express(A.k, B) == (sin(q2)*B.j + cos(q2)*B.k) + assert express(A.i, C) == (cos(q3)*C.i + sin(q3)*C.k) + assert express(A.j, C) == (sin(q2)*sin(q3)*C.i + cos(q2)*C.j - + sin(q2)*cos(q3)*C.k) + assert express(A.k, C) == (-sin(q3)*cos(q2)*C.i + sin(q2)*C.j + + cos(q2)*cos(q3)*C.k) + + assert express(B.i, N) == (cos(q1)*N.i + sin(q1)*N.j) + assert express(B.j, N) == (-sin(q1)*cos(q2)*N.i + + cos(q1)*cos(q2)*N.j + sin(q2)*N.k) + assert express(B.k, N) == (sin(q1)*sin(q2)*N.i - + sin(q2)*cos(q1)*N.j + cos(q2)*N.k) + assert express(B.i, A) == A.i + assert express(B.j, A) == (cos(q2)*A.j + sin(q2)*A.k) + assert express(B.k, A) == (-sin(q2)*A.j + cos(q2)*A.k) + assert express(B.i, B) == B.i + assert express(B.j, B) == B.j + assert express(B.k, B) == B.k + assert express(B.i, C) == (cos(q3)*C.i + sin(q3)*C.k) + assert express(B.j, C) == C.j + assert express(B.k, C) == (-sin(q3)*C.i + cos(q3)*C.k) + + assert express(C.i, N) == ( + (cos(q1)*cos(q3) - sin(q1)*sin(q2)*sin(q3))*N.i + + (sin(q1)*cos(q3) + sin(q2)*sin(q3)*cos(q1))*N.j - + sin(q3)*cos(q2)*N.k) + assert express(C.j, N) == ( + -sin(q1)*cos(q2)*N.i + cos(q1)*cos(q2)*N.j + sin(q2)*N.k) + assert express(C.k, N) == ( + (sin(q3)*cos(q1) + sin(q1)*sin(q2)*cos(q3))*N.i + + (sin(q1)*sin(q3) - sin(q2)*cos(q1)*cos(q3))*N.j + + cos(q2)*cos(q3)*N.k) + assert express(C.i, A) == (cos(q3)*A.i + sin(q2)*sin(q3)*A.j - + sin(q3)*cos(q2)*A.k) + assert express(C.j, A) == (cos(q2)*A.j + sin(q2)*A.k) + assert express(C.k, A) == (sin(q3)*A.i - sin(q2)*cos(q3)*A.j + + cos(q2)*cos(q3)*A.k) + assert express(C.i, B) == (cos(q3)*B.i - sin(q3)*B.k) + assert express(C.j, B) == B.j + assert express(C.k, B) == (sin(q3)*B.i + cos(q3)*B.k) + assert express(C.i, C) == C.i + assert express(C.j, C) == C.j + assert express(C.k, C) == C.k == (C.k) + + # Check to make sure Vectors get converted back to UnitVectors + assert N.i == express((cos(q1)*A.i - sin(q1)*A.j), N).simplify() + assert N.j == express((sin(q1)*A.i + cos(q1)*A.j), N).simplify() + assert N.i == express((cos(q1)*B.i - sin(q1)*cos(q2)*B.j + + sin(q1)*sin(q2)*B.k), N).simplify() + assert N.j == express((sin(q1)*B.i + cos(q1)*cos(q2)*B.j - + sin(q2)*cos(q1)*B.k), N).simplify() + assert N.k == express((sin(q2)*B.j + cos(q2)*B.k), N).simplify() + + + assert A.i == express((cos(q1)*N.i + sin(q1)*N.j), A).simplify() + assert A.j == express((-sin(q1)*N.i + cos(q1)*N.j), A).simplify() + + assert A.j == express((cos(q2)*B.j - sin(q2)*B.k), A).simplify() + assert A.k == express((sin(q2)*B.j + cos(q2)*B.k), A).simplify() + + assert A.i == express((cos(q3)*C.i + sin(q3)*C.k), A).simplify() + assert A.j == express((sin(q2)*sin(q3)*C.i + cos(q2)*C.j - + sin(q2)*cos(q3)*C.k), A).simplify() + + assert A.k == express((-sin(q3)*cos(q2)*C.i + sin(q2)*C.j + + cos(q2)*cos(q3)*C.k), A).simplify() + assert B.i == express((cos(q1)*N.i + sin(q1)*N.j), B).simplify() + assert B.j == express((-sin(q1)*cos(q2)*N.i + + cos(q1)*cos(q2)*N.j + sin(q2)*N.k), B).simplify() + + assert B.k == express((sin(q1)*sin(q2)*N.i - + sin(q2)*cos(q1)*N.j + cos(q2)*N.k), B).simplify() + + assert B.j == express((cos(q2)*A.j + sin(q2)*A.k), B).simplify() + assert B.k == express((-sin(q2)*A.j + cos(q2)*A.k), B).simplify() + assert B.i == express((cos(q3)*C.i + sin(q3)*C.k), B).simplify() + assert B.k == express((-sin(q3)*C.i + cos(q3)*C.k), B).simplify() + assert C.i == express((cos(q3)*A.i + sin(q2)*sin(q3)*A.j - + sin(q3)*cos(q2)*A.k), C).simplify() + assert C.j == express((cos(q2)*A.j + sin(q2)*A.k), C).simplify() + assert C.k == express((sin(q3)*A.i - sin(q2)*cos(q3)*A.j + + cos(q2)*cos(q3)*A.k), C).simplify() + assert C.i == express((cos(q3)*B.i - sin(q3)*B.k), C).simplify() + assert C.k == express((sin(q3)*B.i + cos(q3)*B.k), C).simplify() + + +def test_matrix_to_vector(): + m = Matrix([[1], [2], [3]]) + assert matrix_to_vector(m, C) == C.i + 2*C.j + 3*C.k + m = Matrix([[0], [0], [0]]) + assert matrix_to_vector(m, N) == matrix_to_vector(m, C) == \ + Vector.zero + m = Matrix([[q1], [q2], [q3]]) + assert matrix_to_vector(m, N) == q1*N.i + q2*N.j + q3*N.k + + +def test_orthogonalize(): + C = CoordSys3D('C') + a, b = symbols('a b', integer=True) + i, j, k = C.base_vectors() + v1 = i + 2*j + v2 = 2*i + 3*j + v3 = 3*i + 5*j + v4 = 3*i + j + v5 = 2*i + 2*j + v6 = a*i + b*j + v7 = 4*a*i + 4*b*j + assert orthogonalize(v1, v2) == [C.i + 2*C.j, C.i*Rational(2, 5) + -C.j/5] + # from wikipedia + assert orthogonalize(v4, v5, orthonormal=True) == \ + [(3*sqrt(10))*C.i/10 + (sqrt(10))*C.j/10, (-sqrt(10))*C.i/10 + (3*sqrt(10))*C.j/10] + raises(ValueError, lambda: orthogonalize(v1, v2, v3)) + raises(ValueError, lambda: orthogonalize(v6, v7)) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_implicitregion.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_implicitregion.py new file mode 100644 index 0000000000000000000000000000000000000000..3686d847a7f165cb5ba9aeb813e5922aaa17e1e0 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_implicitregion.py @@ -0,0 +1,90 @@ +from sympy.core.relational import Eq +from sympy.core.singleton import S +from sympy.abc import x, y, z, s, t +from sympy.sets import FiniteSet, EmptySet +from sympy.geometry import Point +from sympy.vector import ImplicitRegion +from sympy.testing.pytest import raises + + +def test_ImplicitRegion(): + ellipse = ImplicitRegion((x, y), (x**2/4 + y**2/16 - 1)) + assert ellipse.equation == x**2/4 + y**2/16 - 1 + assert ellipse.variables == (x, y) + assert ellipse.degree == 2 + r = ImplicitRegion((x, y, z), Eq(x**4 + y**2 - x*y, 6)) + assert r.equation == x**4 + y**2 - x*y - 6 + assert r.variables == (x, y, z) + assert r.degree == 4 + + +def test_regular_point(): + r1 = ImplicitRegion((x,), x**2 - 16) + assert r1.regular_point() == (-4,) + c1 = ImplicitRegion((x, y), x**2 + y**2 - 4) + assert c1.regular_point() == (0, -2) + c2 = ImplicitRegion((x, y), (x - S(5)/2)**2 + y**2 - (S(1)/4)**2) + assert c2.regular_point() == (S(5)/2, -S(1)/4) + c3 = ImplicitRegion((x, y), (y - 5)**2 - 16*(x - 5)) + assert c3.regular_point() == (5, 5) + r2 = ImplicitRegion((x, y), x**2 - 4*x*y - 3*y**2 + 4*x + 8*y - 5) + assert r2.regular_point() == (S(4)/7, S(9)/7) + r3 = ImplicitRegion((x, y), x**2 - 2*x*y + 3*y**2 - 2*x - 5*y + 3/2) + raises(ValueError, lambda: r3.regular_point()) + + +def test_singular_points_and_multiplicty(): + r1 = ImplicitRegion((x, y, z), Eq(x + y + z, 0)) + assert r1.singular_points() == EmptySet + r2 = ImplicitRegion((x, y, z), x*y*z + y**4 -x**2*z**2) + assert r2.singular_points() == FiniteSet((0, 0, z), (x, 0, 0)) + assert r2.multiplicity((0, 0, 0)) == 3 + assert r2.multiplicity((0, 0, 6)) == 2 + r3 = ImplicitRegion((x, y, z), z**2 - x**2 - y**2) + assert r3.singular_points() == FiniteSet((0, 0, 0)) + assert r3.multiplicity((0, 0, 0)) == 2 + r4 = ImplicitRegion((x, y), x**2 + y**2 - 2*x) + assert r4.singular_points() == EmptySet + assert r4.multiplicity(Point(1, 3)) == 0 + + +def test_rational_parametrization(): + p = ImplicitRegion((x,), x - 2) + assert p.rational_parametrization() == (x - 2,) + + line = ImplicitRegion((x, y), Eq(y, 3*x + 2)) + assert line.rational_parametrization() == (x, 3*x + 2) + + circle1 = ImplicitRegion((x, y), (x-2)**2 + (y+3)**2 - 4) + assert circle1.rational_parametrization(parameters=t) == (4*t/(t**2 + 1) + 2, 4*t**2/(t**2 + 1) - 5) + circle2 = ImplicitRegion((x, y), (x - S.Half)**2 + y**2 - (S(1)/2)**2) + + assert circle2.rational_parametrization(parameters=t) == (t/(t**2 + 1) + S(1)/2, t**2/(t**2 + 1) - S(1)/2) + circle3 = ImplicitRegion((x, y), Eq(x**2 + y**2, 2*x)) + assert circle3.rational_parametrization(parameters=(t,)) == (2*t/(t**2 + 1) + 1, 2*t**2/(t**2 + 1) - 1) + + parabola = ImplicitRegion((x, y), (y - 3)**2 - 4*(x + 6)) + assert parabola.rational_parametrization(t) == (-6 + 4/t**2, 3 + 4/t) + + rect_hyperbola = ImplicitRegion((x, y), x*y - 1) + assert rect_hyperbola.rational_parametrization(t) == (-1 + (t + 1)/t, t) + + cubic_curve = ImplicitRegion((x, y), x**3 + x**2 - y**2) + assert cubic_curve.rational_parametrization(parameters=(t)) == (t**2 - 1, t*(t**2 - 1)) + cuspidal = ImplicitRegion((x, y), (x**3 - y**2)) + assert cuspidal.rational_parametrization(t) == (t**2, t**3) + + I = ImplicitRegion((x, y), x**3 + x**2 - y**2) + assert I.rational_parametrization(t) == (t**2 - 1, t*(t**2 - 1)) + + sphere = ImplicitRegion((x, y, z), Eq(x**2 + y**2 + z**2, 2*x)) + assert sphere.rational_parametrization(parameters=(s, t)) == (2/(s**2 + t**2 + 1), 2*t/(s**2 + t**2 + 1), 2*s/(s**2 + t**2 + 1)) + + conic = ImplicitRegion((x, y), Eq(x**2 + 4*x*y + 3*y**2 + x - y + 10, 0)) + assert conic.rational_parametrization(t) == ( + S(17)/2 + 4/(3*t**2 + 4*t + 1), 4*t/(3*t**2 + 4*t + 1) - S(11)/2) + + r1 = ImplicitRegion((x, y), y**2 - x**3 + x) + raises(NotImplementedError, lambda: r1.rational_parametrization()) + r2 = ImplicitRegion((x, y), y**2 - x**3 - x**2 + 1) + raises(NotImplementedError, lambda: r2.rational_parametrization()) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_integrals.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_integrals.py new file mode 100644 index 0000000000000000000000000000000000000000..08e15562cacf088d469266ca33a3cb993584aa9a --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_integrals.py @@ -0,0 +1,106 @@ +from sympy.core.numbers import pi +from sympy.core.singleton import S +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.testing.pytest import raises +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.integrals import ParametricIntegral, vector_integrate +from sympy.vector.parametricregion import ParametricRegion +from sympy.vector.implicitregion import ImplicitRegion +from sympy.abc import x, y, z, u, v, r, t, theta, phi +from sympy.geometry import Point, Segment, Curve, Circle, Polygon, Plane + +C = CoordSys3D('C') + +def test_parametric_lineintegrals(): + halfcircle = ParametricRegion((4*cos(theta), 4*sin(theta)), (theta, -pi/2, pi/2)) + assert ParametricIntegral(C.x*C.y**4, halfcircle) == S(8192)/5 + + curve = ParametricRegion((t, t**2, t**3), (t, 0, 1)) + field1 = 8*C.x**2*C.y*C.z*C.i + 5*C.z*C.j - 4*C.x*C.y*C.k + assert ParametricIntegral(field1, curve) == 1 + line = ParametricRegion((4*t - 1, 2 - 2*t, t), (t, 0, 1)) + assert ParametricIntegral(C.x*C.z*C.i - C.y*C.z*C.k, line) == 3 + + assert ParametricIntegral(4*C.x**3, ParametricRegion((1, t), (t, 0, 2))) == 8 + + helix = ParametricRegion((cos(t), sin(t), 3*t), (t, 0, 4*pi)) + assert ParametricIntegral(C.x*C.y*C.z, helix) == -3*sqrt(10)*pi + + field2 = C.y*C.i + C.z*C.j + C.z*C.k + assert ParametricIntegral(field2, ParametricRegion((cos(t), sin(t), t**2), (t, 0, pi))) == -5*pi/2 + pi**4/2 + +def test_parametric_surfaceintegrals(): + + semisphere = ParametricRegion((2*sin(phi)*cos(theta), 2*sin(phi)*sin(theta), 2*cos(phi)),\ + (theta, 0, 2*pi), (phi, 0, pi/2)) + assert ParametricIntegral(C.z, semisphere) == 8*pi + + cylinder = ParametricRegion((sqrt(3)*cos(theta), sqrt(3)*sin(theta), z), (z, 0, 6), (theta, 0, 2*pi)) + assert ParametricIntegral(C.y, cylinder) == 0 + + cone = ParametricRegion((v*cos(u), v*sin(u), v), (u, 0, 2*pi), (v, 0, 1)) + assert ParametricIntegral(C.x*C.i + C.y*C.j + C.z**4*C.k, cone) == pi/3 + + triangle1 = ParametricRegion((x, y), (x, 0, 2), (y, 0, 10 - 5*x)) + triangle2 = ParametricRegion((x, y), (y, 0, 10 - 5*x), (x, 0, 2)) + assert ParametricIntegral(-15.6*C.y*C.k, triangle1) == ParametricIntegral(-15.6*C.y*C.k, triangle2) + assert ParametricIntegral(C.z, triangle1) == 10*C.z + +def test_parametric_volumeintegrals(): + + cube = ParametricRegion((x, y, z), (x, 0, 1), (y, 0, 1), (z, 0, 1)) + assert ParametricIntegral(1, cube) == 1 + + solidsphere1 = ParametricRegion((r*sin(phi)*cos(theta), r*sin(phi)*sin(theta), r*cos(phi)),\ + (r, 0, 2), (theta, 0, 2*pi), (phi, 0, pi)) + solidsphere2 = ParametricRegion((r*sin(phi)*cos(theta), r*sin(phi)*sin(theta), r*cos(phi)),\ + (r, 0, 2), (phi, 0, pi), (theta, 0, 2*pi)) + assert ParametricIntegral(C.x**2 + C.y**2, solidsphere1) == -256*pi/15 + assert ParametricIntegral(C.x**2 + C.y**2, solidsphere2) == 256*pi/15 + + region_under_plane1 = ParametricRegion((x, y, z), (x, 0, 3), (y, 0, -2*x/3 + 2),\ + (z, 0, 6 - 2*x - 3*y)) + region_under_plane2 = ParametricRegion((x, y, z), (x, 0, 3), (z, 0, 6 - 2*x - 3*y),\ + (y, 0, -2*x/3 + 2)) + + assert ParametricIntegral(C.x*C.i + C.j - 100*C.k, region_under_plane1) == \ + ParametricIntegral(C.x*C.i + C.j - 100*C.k, region_under_plane2) + assert ParametricIntegral(2*C.x, region_under_plane2) == -9 + +def test_vector_integrate(): + halfdisc = ParametricRegion((r*cos(theta), r* sin(theta)), (r, -2, 2), (theta, 0, pi)) + assert vector_integrate(C.x**2, halfdisc) == 4*pi + assert vector_integrate(C.x, ParametricRegion((t, t**2), (t, 2, 3))) == -17*sqrt(17)/12 + 37*sqrt(37)/12 + + assert vector_integrate(C.y**3*C.z, (C.x, 0, 3), (C.y, -1, 4)) == 765*C.z/4 + + s1 = Segment(Point(0, 0), Point(0, 1)) + assert vector_integrate(-15*C.y, s1) == S(-15)/2 + s2 = Segment(Point(4, 3, 9), Point(1, 1, 7)) + assert vector_integrate(C.y*C.i, s2) == -6 + + curve = Curve((sin(t), cos(t)), (t, 0, 2)) + assert vector_integrate(5*C.z, curve) == 10*C.z + + c1 = Circle(Point(2, 3), 6) + assert vector_integrate(C.x*C.y, c1) == 72*pi + c2 = Circle(Point(0, 0), Point(1, 1), Point(1, 0)) + assert vector_integrate(1, c2) == c2.circumference + + triangle = Polygon((0, 0), (1, 0), (1, 1)) + assert vector_integrate(C.x*C.i - 14*C.y*C.j, triangle) == 0 + p1, p2, p3, p4 = [(0, 0), (1, 0), (5, 1), (0, 1)] + poly = Polygon(p1, p2, p3, p4) + assert vector_integrate(-23*C.z, poly) == -161*C.z - 23*sqrt(17)*C.z + + point = Point(2, 3) + assert vector_integrate(C.i*C.y - C.z, point) == ParametricIntegral(C.y*C.i, ParametricRegion((2, 3))) + + c3 = ImplicitRegion((x, y), x**2 + y**2 - 4) + assert vector_integrate(45, c3) == 180*pi + c4 = ImplicitRegion((x, y), (x - 3)**2 + (y - 4)**2 - 9) + assert vector_integrate(1, c4) == 6*pi + + pl = Plane(Point(1, 1, 1), Point(2, 3, 4), Point(2, 2, 2)) + raises(ValueError, lambda: vector_integrate(C.x*C.z*C.i + C.k, pl)) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_operators.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_operators.py new file mode 100644 index 0000000000000000000000000000000000000000..5734edadd00547c67d6f864b50afd966ad8392a6 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_operators.py @@ -0,0 +1,43 @@ +from sympy.vector import CoordSys3D, Gradient, Divergence, Curl, VectorZero, Laplacian +from sympy.printing.repr import srepr + +R = CoordSys3D('R') +s1 = R.x*R.y*R.z # type: ignore +s2 = R.x + 3*R.y**2 # type: ignore +s3 = R.x**2 + R.y**2 + R.z**2 # type: ignore +v1 = R.x*R.i + R.z*R.z*R.j # type: ignore +v2 = R.x*R.i + R.y*R.j + R.z*R.k # type: ignore +v3 = R.x**2*R.i + R.y**2*R.j + R.z**2*R.k # type: ignore + + +def test_Gradient(): + assert Gradient(s1) == Gradient(R.x*R.y*R.z) + assert Gradient(s2) == Gradient(R.x + 3*R.y**2) + assert Gradient(s1).doit() == R.y*R.z*R.i + R.x*R.z*R.j + R.x*R.y*R.k + assert Gradient(s2).doit() == R.i + 6*R.y*R.j + + +def test_Divergence(): + assert Divergence(v1) == Divergence(R.x*R.i + R.z*R.z*R.j) + assert Divergence(v2) == Divergence(R.x*R.i + R.y*R.j + R.z*R.k) + assert Divergence(v1).doit() == 1 + assert Divergence(v2).doit() == 3 + # issue 22384 + Rc = CoordSys3D('R', transformation='cylindrical') + assert Divergence(Rc.i).doit() == 1/Rc.r + + +def test_Curl(): + assert Curl(v1) == Curl(R.x*R.i + R.z*R.z*R.j) + assert Curl(v2) == Curl(R.x*R.i + R.y*R.j + R.z*R.k) + assert Curl(v1).doit() == (-2*R.z)*R.i + assert Curl(v2).doit() == VectorZero() + + +def test_Laplacian(): + assert Laplacian(s3) == Laplacian(R.x**2 + R.y**2 + R.z**2) + assert Laplacian(v3) == Laplacian(R.x**2*R.i + R.y**2*R.j + R.z**2*R.k) + assert Laplacian(s3).doit() == 6 + assert Laplacian(v3).doit() == 2*R.i + 2*R.j + 2*R.k + assert srepr(Laplacian(s3)) == \ + 'Laplacian(Add(Pow(R.x, Integer(2)), Pow(R.y, Integer(2)), Pow(R.z, Integer(2))))' diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_parametricregion.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_parametricregion.py new file mode 100644 index 0000000000000000000000000000000000000000..e785b96744f9e2c39e91b997fcb70f8a921256bd --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_parametricregion.py @@ -0,0 +1,97 @@ +from sympy.core.numbers import pi +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.parametricregion import ParametricRegion, parametric_region_list +from sympy.geometry import Point, Segment, Curve, Ellipse, Line, Parabola, Polygon +from sympy.testing.pytest import raises +from sympy.abc import a, b, r, t, x, y, z, theta, phi + + +C = CoordSys3D('C') + +def test_ParametricRegion(): + + point = ParametricRegion((3, 4)) + assert point.definition == (3, 4) + assert point.parameters == () + assert point.limits == {} + assert point.dimensions == 0 + + # line x = y + line_xy = ParametricRegion((y, y), (y, 1, 5)) + assert line_xy .definition == (y, y) + assert line_xy.parameters == (y,) + assert line_xy.dimensions == 1 + + # line y = z + line_yz = ParametricRegion((x,t,t), x, (t, 1, 2)) + assert line_yz.definition == (x,t,t) + assert line_yz.parameters == (x, t) + assert line_yz.limits == {t: (1, 2)} + assert line_yz.dimensions == 1 + + p1 = ParametricRegion((9*a, -16*b), (a, 0, 2), (b, -1, 5)) + assert p1.definition == (9*a, -16*b) + assert p1.parameters == (a, b) + assert p1.limits == {a: (0, 2), b: (-1, 5)} + assert p1.dimensions == 2 + + p2 = ParametricRegion((t, t**3), t) + assert p2.parameters == (t,) + assert p2.limits == {} + assert p2.dimensions == 0 + + circle = ParametricRegion((r*cos(theta), r*sin(theta)), r, (theta, 0, 2*pi)) + assert circle.definition == (r*cos(theta), r*sin(theta)) + assert circle.dimensions == 1 + + halfdisc = ParametricRegion((r*cos(theta), r*sin(theta)), (r, -2, 2), (theta, 0, pi)) + assert halfdisc.definition == (r*cos(theta), r*sin(theta)) + assert halfdisc.parameters == (r, theta) + assert halfdisc.limits == {r: (-2, 2), theta: (0, pi)} + assert halfdisc.dimensions == 2 + + ellipse = ParametricRegion((a*cos(t), b*sin(t)), (t, 0, 8)) + assert ellipse.parameters == (t,) + assert ellipse.limits == {t: (0, 8)} + assert ellipse.dimensions == 1 + + cylinder = ParametricRegion((r*cos(theta), r*sin(theta), z), (r, 0, 1), (theta, 0, 2*pi), (z, 0, 4)) + assert cylinder.parameters == (r, theta, z) + assert cylinder.dimensions == 3 + + sphere = ParametricRegion((r*sin(phi)*cos(theta),r*sin(phi)*sin(theta), r*cos(phi)), + r, (theta, 0, 2*pi), (phi, 0, pi)) + assert sphere.definition == (r*sin(phi)*cos(theta),r*sin(phi)*sin(theta), r*cos(phi)) + assert sphere.parameters == (r, theta, phi) + assert sphere.dimensions == 2 + + raises(ValueError, lambda: ParametricRegion((a*t**2, 2*a*t), (a, -2))) + raises(ValueError, lambda: ParametricRegion((a, b), (a**2, sin(b)), (a, 2, 4, 6))) + + +def test_parametric_region_list(): + + point = Point(-5, 12) + assert parametric_region_list(point) == [ParametricRegion((-5, 12))] + + e = Ellipse(Point(2, 8), 2, 6) + assert parametric_region_list(e, t) == [ParametricRegion((2*cos(t) + 2, 6*sin(t) + 8), (t, 0, 2*pi))] + + c = Curve((t, t**3), (t, 5, 3)) + assert parametric_region_list(c) == [ParametricRegion((t, t**3), (t, 5, 3))] + + s = Segment(Point(2, 11, -6), Point(0, 2, 5)) + assert parametric_region_list(s, t) == [ParametricRegion((2 - 2*t, 11 - 9*t, 11*t - 6), (t, 0, 1))] + s1 = Segment(Point(0, 0), (1, 0)) + assert parametric_region_list(s1, t) == [ParametricRegion((t, 0), (t, 0, 1))] + s2 = Segment(Point(1, 2, 3), Point(1, 2, 5)) + assert parametric_region_list(s2, t) == [ParametricRegion((1, 2, 2*t + 3), (t, 0, 1))] + s3 = Segment(Point(12, 56), Point(12, 56)) + assert parametric_region_list(s3) == [ParametricRegion((12, 56))] + + poly = Polygon((1,3), (-3, 8), (2, 4)) + assert parametric_region_list(poly, t) == [ParametricRegion((1 - 4*t, 5*t + 3), (t, 0, 1)), ParametricRegion((5*t - 3, 8 - 4*t), (t, 0, 1)), ParametricRegion((2 - t, 4 - t), (t, 0, 1))] + + p1 = Parabola(Point(0, 0), Line(Point(5, 8), Point(7,8))) + raises(ValueError, lambda: parametric_region_list(p1)) diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_printing.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_printing.py new file mode 100644 index 0000000000000000000000000000000000000000..ae76905e967bdf93485f135c6a69f968e1208986 --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_printing.py @@ -0,0 +1,221 @@ +# -*- coding: utf-8 -*- +from sympy.core.function import Function +from sympy.integrals.integrals import Integral +from sympy.printing.latex import latex +from sympy.printing.pretty import pretty as xpretty +from sympy.vector import CoordSys3D, Del, Vector, express +from sympy.abc import a, b, c +from sympy.testing.pytest import XFAIL + + +def pretty(expr): + """ASCII pretty-printing""" + return xpretty(expr, use_unicode=False, wrap_line=False) + + +def upretty(expr): + """Unicode pretty-printing""" + return xpretty(expr, use_unicode=True, wrap_line=False) + + +# Initialize the basic and tedious vector/dyadic expressions +# needed for testing. +# Some of the pretty forms shown denote how the expressions just +# above them should look with pretty printing. +N = CoordSys3D('N') +C = N.orient_new_axis('C', a, N.k) # type: ignore +v = [] +d = [] +v.append(Vector.zero) +v.append(N.i) # type: ignore +v.append(-N.i) # type: ignore +v.append(N.i + N.j) # type: ignore +v.append(a*N.i) # type: ignore +v.append(a*N.i - b*N.j) # type: ignore +v.append((a**2 + N.x)*N.i + N.k) # type: ignore +v.append((a**2 + b)*N.i + 3*(C.y - c)*N.k) # type: ignore +f = Function('f') +v.append(N.j - (Integral(f(b)) - C.x**2)*N.k) # type: ignore +upretty_v_8 = """\ + ⎛ 2 ⌠ ⎞ \n\ +j_N + ⎜x_C - ⎮ f(b) db⎟ k_N\n\ + ⎝ ⌡ ⎠ \ +""" +pretty_v_8 = """\ +j_N + / / \\\n\ + | 2 | |\n\ + |x_C - | f(b) db|\n\ + | | |\n\ + \\ / / \ +""" + +v.append(N.i + C.k) # type: ignore +v.append(express(N.i, C)) # type: ignore +v.append((a**2 + b)*N.i + (Integral(f(b)))*N.k) # type: ignore +upretty_v_11 = """\ +⎛ 2 ⎞ ⎛⌠ ⎞ \n\ +⎝a + b⎠ i_N + ⎜⎮ f(b) db⎟ k_N\n\ + ⎝⌡ ⎠ \ +""" +pretty_v_11 = """\ +/ 2 \\ + / / \\\n\ +\\a + b/ i_N| | |\n\ + | | f(b) db|\n\ + | | |\n\ + \\/ / \ +""" + +for x in v: + d.append(x | N.k) # type: ignore +s = 3*N.x**2*C.y # type: ignore +upretty_s = """\ + 2\n\ +3⋅y_C⋅x_N \ +""" +pretty_s = """\ + 2\n\ +3*y_C*x_N \ +""" + +# This is the pretty form for ((a**2 + b)*N.i + 3*(C.y - c)*N.k) | N.k +upretty_d_7 = """\ +⎛ 2 ⎞ \n\ +⎝a + b⎠ (i_N|k_N) + (3⋅y_C - 3⋅c) (k_N|k_N)\ +""" +pretty_d_7 = """\ +/ 2 \\ (i_N|k_N) + (3*y_C - 3*c) (k_N|k_N)\n\ +\\a + b/ \ +""" + + +def test_str_printing(): + assert str(v[0]) == '0' + assert str(v[1]) == 'N.i' + assert str(v[2]) == '(-1)*N.i' + assert str(v[3]) == 'N.i + N.j' + assert str(v[8]) == 'N.j + (C.x**2 - Integral(f(b), b))*N.k' + assert str(v[9]) == 'C.k + N.i' + assert str(s) == '3*C.y*N.x**2' + assert str(d[0]) == '0' + assert str(d[1]) == '(N.i|N.k)' + assert str(d[4]) == 'a*(N.i|N.k)' + assert str(d[5]) == 'a*(N.i|N.k) + (-b)*(N.j|N.k)' + assert str(d[8]) == ('(N.j|N.k) + (C.x**2 - ' + + 'Integral(f(b), b))*(N.k|N.k)') + + +@XFAIL +def test_pretty_printing_ascii(): + assert pretty(v[0]) == '0' + assert pretty(v[1]) == 'i_N' + assert pretty(v[5]) == '(a) i_N + (-b) j_N' + assert pretty(v[8]) == pretty_v_8 + assert pretty(v[2]) == '(-1) i_N' + assert pretty(v[11]) == pretty_v_11 + assert pretty(s) == pretty_s + assert pretty(d[0]) == '(0|0)' + assert pretty(d[5]) == '(a) (i_N|k_N) + (-b) (j_N|k_N)' + assert pretty(d[7]) == pretty_d_7 + assert pretty(d[10]) == '(cos(a)) (i_C|k_N) + (-sin(a)) (j_C|k_N)' + + +def test_pretty_print_unicode_v(): + assert upretty(v[0]) == '0' + assert upretty(v[1]) == 'i_N' + assert upretty(v[5]) == '(a) i_N + (-b) j_N' + # Make sure the printing works in other objects + assert upretty(v[5].args) == '((a) i_N, (-b) j_N)' + assert upretty(v[8]) == upretty_v_8 + assert upretty(v[2]) == '(-1) i_N' + assert upretty(v[11]) == upretty_v_11 + assert upretty(s) == upretty_s + assert upretty(d[0]) == '(0|0)' + assert upretty(d[5]) == '(a) (i_N|k_N) + (-b) (j_N|k_N)' + assert upretty(d[7]) == upretty_d_7 + assert upretty(d[10]) == '(cos(a)) (i_C|k_N) + (-sin(a)) (j_C|k_N)' + + +def test_latex_printing(): + assert latex(v[0]) == '\\mathbf{\\hat{0}}' + assert latex(v[1]) == '\\mathbf{\\hat{i}_{N}}' + assert latex(v[2]) == '- \\mathbf{\\hat{i}_{N}}' + assert latex(v[5]) == ('\\left(a\\right)\\mathbf{\\hat{i}_{N}} + ' + + '\\left(- b\\right)\\mathbf{\\hat{j}_{N}}') + assert latex(v[6]) == ('\\left(\\mathbf{{x}_{N}} + a^{2}\\right)\\mathbf{\\hat{i}_' + + '{N}} + \\mathbf{\\hat{k}_{N}}') + assert latex(v[8]) == ('\\mathbf{\\hat{j}_{N}} + \\left(\\mathbf{{x}_' + + '{C}}^{2} - \\int f{\\left(b \\right)}\\,' + + ' db\\right)\\mathbf{\\hat{k}_{N}}') + assert latex(s) == '3 \\mathbf{{y}_{C}} \\mathbf{{x}_{N}}^{2}' + assert latex(d[0]) == '(\\mathbf{\\hat{0}}|\\mathbf{\\hat{0}})' + assert latex(d[4]) == ('\\left(a\\right)\\left(\\mathbf{\\hat{i}_{N}}{\\middle|}' + + '\\mathbf{\\hat{k}_{N}}\\right)') + assert latex(d[9]) == ('\\left(\\mathbf{\\hat{k}_{C}}{\\middle|}' + + '\\mathbf{\\hat{k}_{N}}\\right) + \\left(' + + '\\mathbf{\\hat{i}_{N}}{\\middle|}\\mathbf{' + + '\\hat{k}_{N}}\\right)') + assert latex(d[11]) == ('\\left(a^{2} + b\\right)\\left(\\mathbf{\\hat{i}_{N}}' + + '{\\middle|}\\mathbf{\\hat{k}_{N}}\\right) + ' + + '\\left(\\int f{\\left(b \\right)}\\, db\\right)\\left(' + + '\\mathbf{\\hat{k}_{N}}{\\middle|}\\mathbf{' + + '\\hat{k}_{N}}\\right)') + +def test_issue_23058(): + from sympy import symbols, sin, cos, pi, UnevaluatedExpr + + delop = Del() + CC_ = CoordSys3D("C") + y = CC_.y + xhat = CC_.i + + t = symbols("t") + ten = symbols("10", positive=True) + eps, mu = 4*pi*ten**(-11), ten**(-5) + + Bx = 2 * ten**(-4) * cos(ten**5 * t) * sin(ten**(-3) * y) + vecB = Bx * xhat + vecE = (1/eps) * Integral(delop.cross(vecB/mu).doit(), t) + vecE = vecE.doit() + + vecB_str = """\ +⎛ ⎛y_C⎞ ⎛ 5 ⎞⎞ \n\ +⎜2⋅sin⎜───⎟⋅cos⎝10 ⋅t⎠⎟ i_C\n\ +⎜ ⎜ 3⎟ ⎟ \n\ +⎜ ⎝10 ⎠ ⎟ \n\ +⎜─────────────────────⎟ \n\ +⎜ 4 ⎟ \n\ +⎝ 10 ⎠ \ +""" + vecE_str = """\ +⎛ 4 ⎛ 5 ⎞ ⎛y_C⎞ ⎞ \n\ +⎜-10 ⋅sin⎝10 ⋅t⎠⋅cos⎜───⎟ ⎟ k_C\n\ +⎜ ⎜ 3⎟ ⎟ \n\ +⎜ ⎝10 ⎠ ⎟ \n\ +⎜─────────────────────────⎟ \n\ +⎝ 2⋅π ⎠ \ +""" + + assert upretty(vecB) == vecB_str + assert upretty(vecE) == vecE_str + + ten = UnevaluatedExpr(10) + eps, mu = 4*pi*ten**(-11), ten**(-5) + + Bx = 2 * ten**(-4) * cos(ten**5 * t) * sin(ten**(-3) * y) + vecB = Bx * xhat + + vecB_str = """\ +⎛ -4 ⎛ 5⎞ ⎛ -3⎞⎞ \n\ +⎝2⋅10 ⋅cos⎝t⋅10 ⎠⋅sin⎝y_C⋅10 ⎠⎠ i_C \ +""" + assert upretty(vecB) == vecB_str + +def test_custom_names(): + A = CoordSys3D('A', vector_names=['x', 'y', 'z'], + variable_names=['i', 'j', 'k']) + assert A.i.__str__() == 'A.i' + assert A.x.__str__() == 'A.x' + assert A.i._pretty_form == 'i_A' + assert A.x._pretty_form == 'x_A' + assert A.i._latex_form == r'\mathbf{{i}_{A}}' + assert A.x._latex_form == r"\mathbf{\hat{x}_{A}}" diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_vector.py b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_vector.py new file mode 100644 index 0000000000000000000000000000000000000000..b68fb9fb3efb1f11f1d5a8908aa80dc1f9d7e46e --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/tests/test_vector.py @@ -0,0 +1,266 @@ +from sympy.core import Rational, S +from sympy.simplify import simplify, trigsimp +from sympy.core.function import (Derivative, Function, diff) +from sympy.core.numbers import pi +from sympy.core.symbol import symbols +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.functions.elementary.trigonometric import (cos, sin) +from sympy.integrals.integrals import Integral +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.vector.vector import Vector, BaseVector, VectorAdd, \ + VectorMul, VectorZero +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.vector import Cross, Dot, cross +from sympy.testing.pytest import raises + +C = CoordSys3D('C') + +i, j, k = C.base_vectors() +a, b, c = symbols('a b c') + + +def test_cross(): + v1 = C.x * i + C.z * C.z * j + v2 = C.x * i + C.y * j + C.z * k + assert Cross(v1, v2) == Cross(C.x*C.i + C.z**2*C.j, C.x*C.i + C.y*C.j + C.z*C.k) + assert Cross(v1, v2).doit() == C.z**3*C.i + (-C.x*C.z)*C.j + (C.x*C.y - C.x*C.z**2)*C.k + assert cross(v1, v2) == C.z**3*C.i + (-C.x*C.z)*C.j + (C.x*C.y - C.x*C.z**2)*C.k + assert Cross(v1, v2) == -Cross(v2, v1) + assert Cross(v1, v2) + Cross(v2, v1) == Vector.zero + + +def test_dot(): + v1 = C.x * i + C.z * C.z * j + v2 = C.x * i + C.y * j + C.z * k + assert Dot(v1, v2) == Dot(C.x*C.i + C.z**2*C.j, C.x*C.i + C.y*C.j + C.z*C.k) + assert Dot(v1, v2).doit() == C.x**2 + C.y*C.z**2 + assert Dot(v1, v2).doit() == C.x**2 + C.y*C.z**2 + assert Dot(v1, v2) == Dot(v2, v1) + + +def test_vector_sympy(): + """ + Test whether the Vector framework confirms to the hashing + and equality testing properties of SymPy. + """ + v1 = 3*j + assert v1 == j*3 + assert v1.components == {j: 3} + v2 = 3*i + 4*j + 5*k + v3 = 2*i + 4*j + i + 4*k + k + assert v3 == v2 + assert v3.__hash__() == v2.__hash__() + + +def test_vector(): + assert isinstance(i, BaseVector) + assert i != j + assert j != k + assert k != i + assert i - i == Vector.zero + assert i + Vector.zero == i + assert i - Vector.zero == i + assert Vector.zero != 0 + assert -Vector.zero == Vector.zero + + v1 = a*i + b*j + c*k + v2 = a**2*i + b**2*j + c**2*k + v3 = v1 + v2 + v4 = 2 * v1 + v5 = a * i + + assert isinstance(v1, VectorAdd) + assert v1 - v1 == Vector.zero + assert v1 + Vector.zero == v1 + assert v1.dot(i) == a + assert v1.dot(j) == b + assert v1.dot(k) == c + assert i.dot(v2) == a**2 + assert j.dot(v2) == b**2 + assert k.dot(v2) == c**2 + assert v3.dot(i) == a**2 + a + assert v3.dot(j) == b**2 + b + assert v3.dot(k) == c**2 + c + + assert v1 + v2 == v2 + v1 + assert v1 - v2 == -1 * (v2 - v1) + assert a * v1 == v1 * a + + assert isinstance(v5, VectorMul) + assert v5.base_vector == i + assert v5.measure_number == a + assert isinstance(v4, Vector) + assert isinstance(v4, VectorAdd) + assert isinstance(v4, Vector) + assert isinstance(Vector.zero, VectorZero) + assert isinstance(Vector.zero, Vector) + assert isinstance(v1 * 0, VectorZero) + + assert v1.to_matrix(C) == Matrix([[a], [b], [c]]) + + assert i.components == {i: 1} + assert v5.components == {i: a} + assert v1.components == {i: a, j: b, k: c} + + assert VectorAdd(v1, Vector.zero) == v1 + assert VectorMul(a, v1) == v1*a + assert VectorMul(1, i) == i + assert VectorAdd(v1, Vector.zero) == v1 + assert VectorMul(0, Vector.zero) == Vector.zero + raises(TypeError, lambda: v1.outer(1)) + raises(TypeError, lambda: v1.dot(1)) + + +def test_vector_magnitude_normalize(): + assert Vector.zero.magnitude() == 0 + assert Vector.zero.normalize() == Vector.zero + + assert i.magnitude() == 1 + assert j.magnitude() == 1 + assert k.magnitude() == 1 + assert i.normalize() == i + assert j.normalize() == j + assert k.normalize() == k + + v1 = a * i + assert v1.normalize() == (a/sqrt(a**2))*i + assert v1.magnitude() == sqrt(a**2) + + v2 = a*i + b*j + c*k + assert v2.magnitude() == sqrt(a**2 + b**2 + c**2) + assert v2.normalize() == v2 / v2.magnitude() + + v3 = i + j + assert v3.normalize() == (sqrt(2)/2)*C.i + (sqrt(2)/2)*C.j + + +def test_vector_simplify(): + A, s, k, m = symbols('A, s, k, m') + + test1 = (1 / a + 1 / b) * i + assert (test1 & i) != (a + b) / (a * b) + test1 = simplify(test1) + assert (test1 & i) == (a + b) / (a * b) + assert test1.simplify() == simplify(test1) + + test2 = (A**2 * s**4 / (4 * pi * k * m**3)) * i + test2 = simplify(test2) + assert (test2 & i) == (A**2 * s**4 / (4 * pi * k * m**3)) + + test3 = ((4 + 4 * a - 2 * (2 + 2 * a)) / (2 + 2 * a)) * i + test3 = simplify(test3) + assert (test3 & i) == 0 + + test4 = ((-4 * a * b**2 - 2 * b**3 - 2 * a**2 * b) / (a + b)**2) * i + test4 = simplify(test4) + assert (test4 & i) == -2 * b + + v = (sin(a)+cos(a))**2*i - j + assert trigsimp(v) == (2*sin(a + pi/4)**2)*i + (-1)*j + assert trigsimp(v) == v.trigsimp() + + assert simplify(Vector.zero) == Vector.zero + + +def test_vector_dot(): + assert i.dot(Vector.zero) == 0 + assert Vector.zero.dot(i) == 0 + assert i & Vector.zero == 0 + + assert i.dot(i) == 1 + assert i.dot(j) == 0 + assert i.dot(k) == 0 + assert i & i == 1 + assert i & j == 0 + assert i & k == 0 + + assert j.dot(i) == 0 + assert j.dot(j) == 1 + assert j.dot(k) == 0 + assert j & i == 0 + assert j & j == 1 + assert j & k == 0 + + assert k.dot(i) == 0 + assert k.dot(j) == 0 + assert k.dot(k) == 1 + assert k & i == 0 + assert k & j == 0 + assert k & k == 1 + + raises(TypeError, lambda: k.dot(1)) + + +def test_vector_cross(): + assert i.cross(Vector.zero) == Vector.zero + assert Vector.zero.cross(i) == Vector.zero + + assert i.cross(i) == Vector.zero + assert i.cross(j) == k + assert i.cross(k) == -j + assert i ^ i == Vector.zero + assert i ^ j == k + assert i ^ k == -j + + assert j.cross(i) == -k + assert j.cross(j) == Vector.zero + assert j.cross(k) == i + assert j ^ i == -k + assert j ^ j == Vector.zero + assert j ^ k == i + + assert k.cross(i) == j + assert k.cross(j) == -i + assert k.cross(k) == Vector.zero + assert k ^ i == j + assert k ^ j == -i + assert k ^ k == Vector.zero + + assert k.cross(1) == Cross(k, 1) + + +def test_projection(): + v1 = i + j + k + v2 = 3*i + 4*j + v3 = 0*i + 0*j + assert v1.projection(v1) == i + j + k + assert v1.projection(v2) == Rational(7, 3)*C.i + Rational(7, 3)*C.j + Rational(7, 3)*C.k + assert v1.projection(v1, scalar=True) == S.One + assert v1.projection(v2, scalar=True) == Rational(7, 3) + assert v3.projection(v1) == Vector.zero + assert v3.projection(v1, scalar=True) == S.Zero + + +def test_vector_diff_integrate(): + f = Function('f') + v = f(a)*C.i + a**2*C.j - C.k + assert Derivative(v, a) == Derivative((f(a))*C.i + + a**2*C.j + (-1)*C.k, a) + assert (diff(v, a) == v.diff(a) == Derivative(v, a).doit() == + (Derivative(f(a), a))*C.i + 2*a*C.j) + assert (Integral(v, a) == (Integral(f(a), a))*C.i + + (Integral(a**2, a))*C.j + (Integral(-1, a))*C.k) + + +def test_vector_args(): + raises(ValueError, lambda: BaseVector(3, C)) + raises(TypeError, lambda: BaseVector(0, Vector.zero)) + + +def test_srepr(): + from sympy.printing.repr import srepr + res = "CoordSys3D(Str('C'), Tuple(ImmutableDenseMatrix([[Integer(1), "\ + "Integer(0), Integer(0)], [Integer(0), Integer(1), Integer(0)], "\ + "[Integer(0), Integer(0), Integer(1)]]), VectorZero())).i" + assert srepr(C.i) == res + + +def test_scalar(): + from sympy.vector import CoordSys3D + C = CoordSys3D('C') + v1 = 3*C.i + 4*C.j + 5*C.k + v2 = 3*C.i - 4*C.j + 5*C.k + assert v1.is_Vector is True + assert v1.is_scalar is False + assert (v1.dot(v2)).is_scalar is True + assert (v1.cross(v2)).is_scalar is False diff --git a/mgm/lib/python3.10/site-packages/sympy/vector/vector.py b/mgm/lib/python3.10/site-packages/sympy/vector/vector.py new file mode 100644 index 0000000000000000000000000000000000000000..d64ea6d70890e38d6a1b39476de0b3c153d95bfa --- /dev/null +++ b/mgm/lib/python3.10/site-packages/sympy/vector/vector.py @@ -0,0 +1,623 @@ +from __future__ import annotations +from itertools import product + +from sympy.core.add import Add +from sympy.core.assumptions import StdFactKB +from sympy.core.expr import AtomicExpr, Expr +from sympy.core.power import Pow +from sympy.core.singleton import S +from sympy.core.sorting import default_sort_key +from sympy.core.sympify import sympify +from sympy.functions.elementary.miscellaneous import sqrt +from sympy.matrices.immutable import ImmutableDenseMatrix as Matrix +from sympy.vector.basisdependent import (BasisDependentZero, + BasisDependent, BasisDependentMul, BasisDependentAdd) +from sympy.vector.coordsysrect import CoordSys3D +from sympy.vector.dyadic import Dyadic, BaseDyadic, DyadicAdd + + +class Vector(BasisDependent): + """ + Super class for all Vector classes. + Ideally, neither this class nor any of its subclasses should be + instantiated by the user. + """ + + is_scalar = False + is_Vector = True + _op_priority = 12.0 + + _expr_type: type[Vector] + _mul_func: type[Vector] + _add_func: type[Vector] + _zero_func: type[Vector] + _base_func: type[Vector] + zero: VectorZero + + @property + def components(self): + """ + Returns the components of this vector in the form of a + Python dictionary mapping BaseVector instances to the + corresponding measure numbers. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> C = CoordSys3D('C') + >>> v = 3*C.i + 4*C.j + 5*C.k + >>> v.components + {C.i: 3, C.j: 4, C.k: 5} + + """ + # The '_components' attribute is defined according to the + # subclass of Vector the instance belongs to. + return self._components + + def magnitude(self): + """ + Returns the magnitude of this vector. + """ + return sqrt(self & self) + + def normalize(self): + """ + Returns the normalized version of this vector. + """ + return self / self.magnitude() + + def dot(self, other): + """ + Returns the dot product of this Vector, either with another + Vector, or a Dyadic, or a Del operator. + If 'other' is a Vector, returns the dot product scalar (SymPy + expression). + If 'other' is a Dyadic, the dot product is returned as a Vector. + If 'other' is an instance of Del, returns the directional + derivative operator as a Python function. If this function is + applied to a scalar expression, it returns the directional + derivative of the scalar field wrt this Vector. + + Parameters + ========== + + other: Vector/Dyadic/Del + The Vector or Dyadic we are dotting with, or a Del operator . + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Del + >>> C = CoordSys3D('C') + >>> delop = Del() + >>> C.i.dot(C.j) + 0 + >>> C.i & C.i + 1 + >>> v = 3*C.i + 4*C.j + 5*C.k + >>> v.dot(C.k) + 5 + >>> (C.i & delop)(C.x*C.y*C.z) + C.y*C.z + >>> d = C.i.outer(C.i) + >>> C.i.dot(d) + C.i + + """ + + # Check special cases + if isinstance(other, Dyadic): + if isinstance(self, VectorZero): + return Vector.zero + outvec = Vector.zero + for k, v in other.components.items(): + vect_dot = k.args[0].dot(self) + outvec += vect_dot * v * k.args[1] + return outvec + from sympy.vector.deloperator import Del + if not isinstance(other, (Del, Vector)): + raise TypeError(str(other) + " is not a vector, dyadic or " + + "del operator") + + # Check if the other is a del operator + if isinstance(other, Del): + def directional_derivative(field): + from sympy.vector.functions import directional_derivative + return directional_derivative(field, self) + return directional_derivative + + return dot(self, other) + + def __and__(self, other): + return self.dot(other) + + __and__.__doc__ = dot.__doc__ + + def cross(self, other): + """ + Returns the cross product of this Vector with another Vector or + Dyadic instance. + The cross product is a Vector, if 'other' is a Vector. If 'other' + is a Dyadic, this returns a Dyadic instance. + + Parameters + ========== + + other: Vector/Dyadic + The Vector or Dyadic we are crossing with. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> C = CoordSys3D('C') + >>> C.i.cross(C.j) + C.k + >>> C.i ^ C.i + 0 + >>> v = 3*C.i + 4*C.j + 5*C.k + >>> v ^ C.i + 5*C.j + (-4)*C.k + >>> d = C.i.outer(C.i) + >>> C.j.cross(d) + (-1)*(C.k|C.i) + + """ + + # Check special cases + if isinstance(other, Dyadic): + if isinstance(self, VectorZero): + return Dyadic.zero + outdyad = Dyadic.zero + for k, v in other.components.items(): + cross_product = self.cross(k.args[0]) + outer = cross_product.outer(k.args[1]) + outdyad += v * outer + return outdyad + + return cross(self, other) + + def __xor__(self, other): + return self.cross(other) + + __xor__.__doc__ = cross.__doc__ + + def outer(self, other): + """ + Returns the outer product of this vector with another, in the + form of a Dyadic instance. + + Parameters + ========== + + other : Vector + The Vector with respect to which the outer product is to + be computed. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> N = CoordSys3D('N') + >>> N.i.outer(N.j) + (N.i|N.j) + + """ + + # Handle the special cases + if not isinstance(other, Vector): + raise TypeError("Invalid operand for outer product") + elif (isinstance(self, VectorZero) or + isinstance(other, VectorZero)): + return Dyadic.zero + + # Iterate over components of both the vectors to generate + # the required Dyadic instance + args = [(v1 * v2) * BaseDyadic(k1, k2) for (k1, v1), (k2, v2) + in product(self.components.items(), other.components.items())] + + return DyadicAdd(*args) + + def projection(self, other, scalar=False): + """ + Returns the vector or scalar projection of the 'other' on 'self'. + + Examples + ======== + + >>> from sympy.vector.coordsysrect import CoordSys3D + >>> C = CoordSys3D('C') + >>> i, j, k = C.base_vectors() + >>> v1 = i + j + k + >>> v2 = 3*i + 4*j + >>> v1.projection(v2) + 7/3*C.i + 7/3*C.j + 7/3*C.k + >>> v1.projection(v2, scalar=True) + 7/3 + + """ + if self.equals(Vector.zero): + return S.Zero if scalar else Vector.zero + + if scalar: + return self.dot(other) / self.dot(self) + else: + return self.dot(other) / self.dot(self) * self + + @property + def _projections(self): + """ + Returns the components of this vector but the output includes + also zero values components. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Vector + >>> C = CoordSys3D('C') + >>> v1 = 3*C.i + 4*C.j + 5*C.k + >>> v1._projections + (3, 4, 5) + >>> v2 = C.x*C.y*C.z*C.i + >>> v2._projections + (C.x*C.y*C.z, 0, 0) + >>> v3 = Vector.zero + >>> v3._projections + (0, 0, 0) + """ + + from sympy.vector.operators import _get_coord_systems + if isinstance(self, VectorZero): + return (S.Zero, S.Zero, S.Zero) + base_vec = next(iter(_get_coord_systems(self))).base_vectors() + return tuple([self.dot(i) for i in base_vec]) + + def __or__(self, other): + return self.outer(other) + + __or__.__doc__ = outer.__doc__ + + def to_matrix(self, system): + """ + Returns the matrix form of this vector with respect to the + specified coordinate system. + + Parameters + ========== + + system : CoordSys3D + The system wrt which the matrix form is to be computed + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> C = CoordSys3D('C') + >>> from sympy.abc import a, b, c + >>> v = a*C.i + b*C.j + c*C.k + >>> v.to_matrix(C) + Matrix([ + [a], + [b], + [c]]) + + """ + + return Matrix([self.dot(unit_vec) for unit_vec in + system.base_vectors()]) + + def separate(self): + """ + The constituents of this vector in different coordinate systems, + as per its definition. + + Returns a dict mapping each CoordSys3D to the corresponding + constituent Vector. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> R1 = CoordSys3D('R1') + >>> R2 = CoordSys3D('R2') + >>> v = R1.i + R2.i + >>> v.separate() == {R1: R1.i, R2: R2.i} + True + + """ + + parts = {} + for vect, measure in self.components.items(): + parts[vect.system] = (parts.get(vect.system, Vector.zero) + + vect * measure) + return parts + + def _div_helper(one, other): + """ Helper for division involving vectors. """ + if isinstance(one, Vector) and isinstance(other, Vector): + raise TypeError("Cannot divide two vectors") + elif isinstance(one, Vector): + if other == S.Zero: + raise ValueError("Cannot divide a vector by zero") + return VectorMul(one, Pow(other, S.NegativeOne)) + else: + raise TypeError("Invalid division involving a vector") + + +class BaseVector(Vector, AtomicExpr): + """ + Class to denote a base vector. + + """ + + def __new__(cls, index, system, pretty_str=None, latex_str=None): + if pretty_str is None: + pretty_str = "x{}".format(index) + if latex_str is None: + latex_str = "x_{}".format(index) + pretty_str = str(pretty_str) + latex_str = str(latex_str) + # Verify arguments + if index not in range(0, 3): + raise ValueError("index must be 0, 1 or 2") + if not isinstance(system, CoordSys3D): + raise TypeError("system should be a CoordSys3D") + name = system._vector_names[index] + # Initialize an object + obj = super().__new__(cls, S(index), system) + # Assign important attributes + obj._base_instance = obj + obj._components = {obj: S.One} + obj._measure_number = S.One + obj._name = system._name + '.' + name + obj._pretty_form = '' + pretty_str + obj._latex_form = latex_str + obj._system = system + # The _id is used for printing purposes + obj._id = (index, system) + assumptions = {'commutative': True} + obj._assumptions = StdFactKB(assumptions) + + # This attr is used for re-expression to one of the systems + # involved in the definition of the Vector. Applies to + # VectorMul and VectorAdd too. + obj._sys = system + + return obj + + @property + def system(self): + return self._system + + def _sympystr(self, printer): + return self._name + + def _sympyrepr(self, printer): + index, system = self._id + return printer._print(system) + '.' + system._vector_names[index] + + @property + def free_symbols(self): + return {self} + + +class VectorAdd(BasisDependentAdd, Vector): + """ + Class to denote sum of Vector instances. + """ + + def __new__(cls, *args, **options): + obj = BasisDependentAdd.__new__(cls, *args, **options) + return obj + + def _sympystr(self, printer): + ret_str = '' + items = list(self.separate().items()) + items.sort(key=lambda x: x[0].__str__()) + for system, vect in items: + base_vects = system.base_vectors() + for x in base_vects: + if x in vect.components: + temp_vect = self.components[x] * x + ret_str += printer._print(temp_vect) + " + " + return ret_str[:-3] + + +class VectorMul(BasisDependentMul, Vector): + """ + Class to denote products of scalars and BaseVectors. + """ + + def __new__(cls, *args, **options): + obj = BasisDependentMul.__new__(cls, *args, **options) + return obj + + @property + def base_vector(self): + """ The BaseVector involved in the product. """ + return self._base_instance + + @property + def measure_number(self): + """ The scalar expression involved in the definition of + this VectorMul. + """ + return self._measure_number + + +class VectorZero(BasisDependentZero, Vector): + """ + Class to denote a zero vector + """ + + _op_priority = 12.1 + _pretty_form = '0' + _latex_form = r'\mathbf{\hat{0}}' + + def __new__(cls): + obj = BasisDependentZero.__new__(cls) + return obj + + +class Cross(Vector): + """ + Represents unevaluated Cross product. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Cross + >>> R = CoordSys3D('R') + >>> v1 = R.i + R.j + R.k + >>> v2 = R.x * R.i + R.y * R.j + R.z * R.k + >>> Cross(v1, v2) + Cross(R.i + R.j + R.k, R.x*R.i + R.y*R.j + R.z*R.k) + >>> Cross(v1, v2).doit() + (-R.y + R.z)*R.i + (R.x - R.z)*R.j + (-R.x + R.y)*R.k + + """ + + def __new__(cls, expr1, expr2): + expr1 = sympify(expr1) + expr2 = sympify(expr2) + if default_sort_key(expr1) > default_sort_key(expr2): + return -Cross(expr2, expr1) + obj = Expr.__new__(cls, expr1, expr2) + obj._expr1 = expr1 + obj._expr2 = expr2 + return obj + + def doit(self, **hints): + return cross(self._expr1, self._expr2) + + +class Dot(Expr): + """ + Represents unevaluated Dot product. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D, Dot + >>> from sympy import symbols + >>> R = CoordSys3D('R') + >>> a, b, c = symbols('a b c') + >>> v1 = R.i + R.j + R.k + >>> v2 = a * R.i + b * R.j + c * R.k + >>> Dot(v1, v2) + Dot(R.i + R.j + R.k, a*R.i + b*R.j + c*R.k) + >>> Dot(v1, v2).doit() + a + b + c + + """ + + def __new__(cls, expr1, expr2): + expr1 = sympify(expr1) + expr2 = sympify(expr2) + expr1, expr2 = sorted([expr1, expr2], key=default_sort_key) + obj = Expr.__new__(cls, expr1, expr2) + obj._expr1 = expr1 + obj._expr2 = expr2 + return obj + + def doit(self, **hints): + return dot(self._expr1, self._expr2) + + +def cross(vect1, vect2): + """ + Returns cross product of two vectors. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy.vector.vector import cross + >>> R = CoordSys3D('R') + >>> v1 = R.i + R.j + R.k + >>> v2 = R.x * R.i + R.y * R.j + R.z * R.k + >>> cross(v1, v2) + (-R.y + R.z)*R.i + (R.x - R.z)*R.j + (-R.x + R.y)*R.k + + """ + if isinstance(vect1, Add): + return VectorAdd.fromiter(cross(i, vect2) for i in vect1.args) + if isinstance(vect2, Add): + return VectorAdd.fromiter(cross(vect1, i) for i in vect2.args) + if isinstance(vect1, BaseVector) and isinstance(vect2, BaseVector): + if vect1._sys == vect2._sys: + n1 = vect1.args[0] + n2 = vect2.args[0] + if n1 == n2: + return Vector.zero + n3 = ({0,1,2}.difference({n1, n2})).pop() + sign = 1 if ((n1 + 1) % 3 == n2) else -1 + return sign*vect1._sys.base_vectors()[n3] + from .functions import express + try: + v = express(vect1, vect2._sys) + except ValueError: + return Cross(vect1, vect2) + else: + return cross(v, vect2) + if isinstance(vect1, VectorZero) or isinstance(vect2, VectorZero): + return Vector.zero + if isinstance(vect1, VectorMul): + v1, m1 = next(iter(vect1.components.items())) + return m1*cross(v1, vect2) + if isinstance(vect2, VectorMul): + v2, m2 = next(iter(vect2.components.items())) + return m2*cross(vect1, v2) + + return Cross(vect1, vect2) + + +def dot(vect1, vect2): + """ + Returns dot product of two vectors. + + Examples + ======== + + >>> from sympy.vector import CoordSys3D + >>> from sympy.vector.vector import dot + >>> R = CoordSys3D('R') + >>> v1 = R.i + R.j + R.k + >>> v2 = R.x * R.i + R.y * R.j + R.z * R.k + >>> dot(v1, v2) + R.x + R.y + R.z + + """ + if isinstance(vect1, Add): + return Add.fromiter(dot(i, vect2) for i in vect1.args) + if isinstance(vect2, Add): + return Add.fromiter(dot(vect1, i) for i in vect2.args) + if isinstance(vect1, BaseVector) and isinstance(vect2, BaseVector): + if vect1._sys == vect2._sys: + return S.One if vect1 == vect2 else S.Zero + from .functions import express + try: + v = express(vect2, vect1._sys) + except ValueError: + return Dot(vect1, vect2) + else: + return dot(vect1, v) + if isinstance(vect1, VectorZero) or isinstance(vect2, VectorZero): + return S.Zero + if isinstance(vect1, VectorMul): + v1, m1 = next(iter(vect1.components.items())) + return m1*dot(v1, vect2) + if isinstance(vect2, VectorMul): + v2, m2 = next(iter(vect2.components.items())) + return m2*dot(vect1, v2) + + return Dot(vect1, vect2) + + +Vector._expr_type = Vector +Vector._mul_func = VectorMul +Vector._add_func = VectorAdd +Vector._zero_func = VectorZero +Vector._base_func = BaseVector +Vector.zero = VectorZero() diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/jit_opt_limit.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/jit_opt_limit.h new file mode 100644 index 0000000000000000000000000000000000000000..fe84f615bcc52d221d4ce830004b886695e2dd96 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/jit_opt_limit.h @@ -0,0 +1,39 @@ +#pragma once +#include +#include +#include + +// `TorchScript` offers a simple optimization limit checker +// that can be configured through environment variable `PYTORCH_JIT_OPT_LIMIT`. +// The purpose is to limit how many optimization you can make per pass. +// This is useful for debugging any passes. + +// Opt limit checker is enabled on a per file basis (hence per pass). For +// example, in `constant_propagation.cpp`, `PYTORCH_JIT_OPT_LIMIT` should be set +// to `constant_propagation=` or, simply, to +// `constant_propagation=` where is the number of +// optimizations you want to make for the pass. (i.e. +// `PYTORCH_JIT_OPT_LIMIT="constant_propagation="`). + +// Multiple files can be configured by separating each file name with a colon +// `:` as in the following example, +// `PYTORCH_JIT_OPT_LIMIT="constant_propagation=:dead_code_elimination="` + +// You can call opt limiter by calling JIT_OPT_ALLOWED. It will return true if +// we haven't reached the optimization limit yet. Otherwise, it will return +// false. Typical usage: + +// if (!JIT_OPT_ALLOWED) { +// GRAPH_DUMP(...); //supplied from jit_log +// return; +// } + +namespace torch { +namespace jit { + +TORCH_API bool opt_limit(const char* pass_name); + +#define JIT_OPT_ALLOWED opt_limit(__FILE__) + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/common_subexpression_elimination.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/common_subexpression_elimination.h new file mode 100644 index 0000000000000000000000000000000000000000..9c8956029dace1988981fa98e8a05f9498c25f81 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/common_subexpression_elimination.h @@ -0,0 +1,11 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +TORCH_API bool EliminateCommonSubexpression( + const std::shared_ptr& graph); +} +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/cuda_graph_fuser.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/cuda_graph_fuser.h new file mode 100644 index 0000000000000000000000000000000000000000..b1d04277166a8838c16b2acf404afaed349438b1 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/cuda_graph_fuser.h @@ -0,0 +1,42 @@ +#pragma once + +#include +#include +#include +#include +#include +#include + +namespace torch { +namespace jit { + +// Register CudaFuseGraph in custom passes +struct TORCH_API RegisterCudaFuseGraph + : public PassManager { + static bool registerPass(bool enabled) { + TORCH_WARN( + "RegisterCudaFuseGraph::registerPass() is deprecated. " + "Please use torch::jit::fuser::cuda::setEnabled()."); + return fuser::cuda::setEnabled(enabled); + } + + static bool isRegistered() { + TORCH_WARN( + "RegisterCudaFuseGraph::isRegistered() is deprecated. " + "Please use torch::jit::fuser::cuda::isEnabled()."); + return fuser::cuda::isEnabled(); + } +}; + +struct CudaFuserComparisonCallback { + using callback_type = + std::function; + bool run_fallback; + callback_type callback; +}; + +TORCH_API CudaFuserComparisonCallback getCudaFuserComparisonCallback(); +TORCH_API void setCudaFuserComparisonCallback(CudaFuserComparisonCallback); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/device_type_analysis.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/device_type_analysis.h new file mode 100644 index 0000000000000000000000000000000000000000..159592a6c6672dd2fccf0768496aea1de44f1ff9 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/device_type_analysis.h @@ -0,0 +1,13 @@ +#pragma once + +#include + +namespace torch { +namespace jit { +struct Graph; + +// Propagates Device type info throughout the given graph. +TORCH_API bool DeviceTypePropagation(std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/dtype_analysis.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/dtype_analysis.h new file mode 100644 index 0000000000000000000000000000000000000000..b4bcdcdc7ae7ea32abf2bfb49a07be8ec48dd82d --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/dtype_analysis.h @@ -0,0 +1,17 @@ +#pragma once + +#include +#include +#include + +namespace torch { +namespace jit { +struct Graph; + +// Propagate tensor properties (e.g., dtype, device, is_contiguous, layout) +// propagation on all tensor objects. Currently, we only support dtype +// propagation +TORCH_API bool DtypePropagation(std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/frozen_concat_linear.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/frozen_concat_linear.h new file mode 100644 index 0000000000000000000000000000000000000000..d64cda0a88f2bbc0ebe585bf8b63e5bd94744743 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/frozen_concat_linear.h @@ -0,0 +1,13 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Concats multiple linear ops with the same Tensor input +// into a single linear op. +TORCH_API bool FrozenConcatLinear(std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/frozen_conv_folding.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/frozen_conv_folding.h new file mode 100644 index 0000000000000000000000000000000000000000..65dc138ccd6a41be0fa709516c97a8b89eeafd98 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/frozen_conv_folding.h @@ -0,0 +1,24 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Fuses Convolution -> Batchnorm into a single Convolution by +// folding batchnorm weights into conv weights. +// This pass only works on Frozen Graphs; otherwise it is a No-Op. +TORCH_API bool FoldFrozenConvBatchnorm(std::shared_ptr& graph); + +// Fuses Convolution -> Add/Sub into a single Convolution by +// folding add constant tensor into conv weights. +// This pass only works on Frozen Graphs; otherwise it is a No-Op. +TORCH_API bool FoldFrozenConvAddOrSub(std::shared_ptr& graph); + +// Fuses Convolution -> Mul/Div into a single Convolution by +// folding add constant tensor into conv weights. +// This pass only works on Frozen Graphs; otherwise it is a No-Op. +TORCH_API bool FoldFrozenConvMulOrDiv(std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/inline_autodiff_subgraphs.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/inline_autodiff_subgraphs.h new file mode 100644 index 0000000000000000000000000000000000000000..8edc81224a07321786937bdebde0d19c5c119c22 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/inline_autodiff_subgraphs.h @@ -0,0 +1,15 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +TORCH_API bool canRunWithAutograd(Node* node); + +TORCH_API void InlineAutodiffSubgraphs( + std::shared_ptr& graph, + size_t threshold = 5); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/inline_fork_wait.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/inline_fork_wait.h new file mode 100644 index 0000000000000000000000000000000000000000..c2dbacdc4ddab7a18f495cfc9f8dc34640f65902 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/inline_fork_wait.h @@ -0,0 +1,16 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Inline Fork and Wait calls. This is used, for example, in ONNX export, where +// we do not support the explicit parallelism structures and would rather +// just have a flat graph. This inlines the forked section in the fork() +// callsite and replaces uses of the result of wait() calls with the values +// produced from the (now-inlined) forked section. +TORCH_API void InlineForkWait(const std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/insert_guards.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/insert_guards.h new file mode 100644 index 0000000000000000000000000000000000000000..28d9f168bf3d559ad434883954004797ae96e690 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/insert_guards.h @@ -0,0 +1,21 @@ +#pragma once + +#include +#include +#include +#include +#include +#include + +#include +#include + +namespace torch { +namespace jit { + +TORCH_API void InsertGuards(std::shared_ptr graph); + +TORCH_API void RemoveProfilingNodes(const std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/mobile_optimizer_type.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/mobile_optimizer_type.h new file mode 100644 index 0000000000000000000000000000000000000000..d11f288dca343308bf2167c89a3d6b2d0792a569 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/mobile_optimizer_type.h @@ -0,0 +1,13 @@ +#pragma once + +#include + +enum class MobileOptimizerType : int8_t { + CONV_BN_FUSION, + INSERT_FOLD_PREPACK_OPS, + REMOVE_DROPOUT, + FUSE_ADD_RELU, + HOIST_CONV_PACKED_PARAMS, + CONV_1D_TO_2D, + VULKAN_AUTOMATIC_GPU_TRANSFER, +}; diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/onednn_graph_fuser.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/onednn_graph_fuser.h new file mode 100644 index 0000000000000000000000000000000000000000..aeb79470b01ae60e38282b4d29b6942af4189ac5 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/onednn_graph_fuser.h @@ -0,0 +1,64 @@ +#pragma once + +#include +#include + +#include + +namespace torch { +namespace jit { +namespace fuser { +namespace onednn { + +static std::atomic onednn_enabled{true}; + +static std::atomic& getLlgaEnabled() { + return onednn_enabled; +} + +TORCH_API void fuseGraph(std::shared_ptr& g); + +} // namespace onednn +} // namespace fuser + +struct C10_EXPORT RegisterLlgaFuseGraph + : public PassManager { + static bool setEnabled(bool enabled) { + TORCH_CHECK( + AT_MKLDNN_ENABLED(), + "Running oneDNN Graph fuser is only supported with MKLDNN builds."); + bool oldState = fuser::onednn::getLlgaEnabled(); + fuser::onednn::getLlgaEnabled() = enabled; + if (enabled) { + registerPass(fuser::onednn::fuseGraph); + } else { + clearPass(); + } + return oldState; + } + + static bool isEnabled() { + return fuser::onednn::getLlgaEnabled(); + } + + // override PassManager::registerPass to register pre-pass + static bool registerPass(GraphPass p) { + if (!isRegistered()) { + passID(registerPrePass(std::move(p)), true); + isRegistered(true); + return false; + } + return true; + } + + // override PassManager::clearPass to clear pre-pass + static void clearPass() { + if (isRegistered()) { + clearPrePass(passID()); + isRegistered(true); + } + } +}; + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/onnx.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/onnx.h new file mode 100644 index 0000000000000000000000000000000000000000..11bee679164043cca58fd3f35a108fd078101a95 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/onnx.h @@ -0,0 +1,28 @@ +#pragma once + +#include +#include +#include + +namespace torch { +namespace jit { + +TORCH_API std::shared_ptr ToONNX( + std::shared_ptr& state, + ::torch::onnx::OperatorExportTypes operator_export_type); +TORCH_API std::unordered_map BlockToONNX( + Block* old_block, + Block* new_block, + ::torch::onnx::OperatorExportTypes operator_export_type, + std::unordered_map& env, + bool is_sub_block = false); +TORCH_API void NodeToONNX( + Node* old_node, + Block* new_block, + ::torch::onnx::OperatorExportTypes operator_export_type, + std::unordered_map& env); +TORCH_API void RemovePrintOps(std::shared_ptr& graph); +TORCH_API void PreprocessCaffe2Ops(std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/peephole_dict_idioms.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/peephole_dict_idioms.h new file mode 100644 index 0000000000000000000000000000000000000000..283c313d9ee2ae8024ba286d1a5bd0ea5cf1fdd3 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/peephole_dict_idioms.h @@ -0,0 +1,38 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Peephole Optimizes Dict Ops such as len() and __getitem__ +// 1. getitem optimizations +// Given a function like this: +// def foo(): +// d = {0 : 1} +// x = d[0] +// return x +// This pass produces (after dead code elimination): +// def foo(a, b): +// return 1 +// +// This optimization can only happen if the dict is not modified +// and the dict has constant, non overlapping keys. +// +// 2. len optimizations +// Given a function like this: +// def foo(): +// d = {0 : 1} +// return len(d) +// This pass produces (after dead code elimination): +// def foo(): +// return 1 +// +// This has the same requirements as the getitem optimizations. +// +// Currently this is invoked as part of PeepholeOptimize +// return true if graph is modified. +TORCH_API bool PeepholeOptimizeDictIdioms(const std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/peephole_non_tensor.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/peephole_non_tensor.h new file mode 100644 index 0000000000000000000000000000000000000000..1e4daebd060cc9365c8994219803a65891c69d4e --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/peephole_non_tensor.h @@ -0,0 +1,14 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// return true if graph is modified +// Optimizing General Graph Patterns that +// are not covered in peephole.cpp and peephole_list_idioms +TORCH_API bool PeepholeOptimizeNonTensor(const std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/remove_exceptions.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/remove_exceptions.h new file mode 100644 index 0000000000000000000000000000000000000000..22b9050cdf5d12ff0cd5bcc5be51d1ad4f26f879 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/remove_exceptions.h @@ -0,0 +1,23 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Considering prim::RaiseException nodes unreachable, simplify prim::If nodes +// when one of the branches contains prim::RaiseException. +// +// This pass is illegal in general case as the modified graph might not throw +// an exception that the original graph would throw. The purpose of the pass is +// to cleanup the graph in a "risky" way by removing pathways leading to +// RaiseExceptions nodes. In some sense, this pass could be considered as a +// "Release" mode, while the original graph was in a "Debug" mode. +// The pass should only be used when such transformation is guaranteed to be +// safe by some other mechanisms. For instance, when we know exact shapes of +// tensors flowing throuth the graph and tensors with such shapes never cause +// exceptions. +TORCH_API void EliminateExceptions(std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/restore_mutation.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/restore_mutation.h new file mode 100644 index 0000000000000000000000000000000000000000..cf128fbd7b08d88eab66404e351f538c7a99251f --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/restore_mutation.h @@ -0,0 +1,64 @@ +#pragma once + +#include +#include +#include +#include +#include +#include + +namespace torch { +namespace jit { + +// A map which stores if an activation operator can perform type promotion +const std::unordered_map activation_type_promotion_mapping = { + {aten::sigmoid, true}, + {aten::tanh, true}, + {aten::celu, false}, + {aten::elu, false}, + {aten::gelu, false}, + {aten::glu, false}, + {aten::hardshrink, false}, + {aten::hardsigmoid, false}, + {aten::hardswish, false}, + {aten::hardtanh, false}, + {aten::leaky_relu, false}, + {aten::prelu, false}, + {aten::relu6, false}, + {aten::relu, false}, + {aten::rrelu, false}, + {aten::selu, false}, + {aten::silu, false}}; + +class FunctionalToInplaceRewriter { + public: + FunctionalToInplaceRewriter(std::shared_ptr graph); + + bool FunctionalToInplace(Block* block); + + private: + AliasDb* getOrCreateAliasDb() { + if (!aliasDb_) { + aliasDb_ = std::make_unique(graph_); + } + return aliasDb_.get(); + } + + bool CanBeInplace(Node* node); + + std::unique_ptr aliasDb_ = nullptr; + std::shared_ptr graph_; +}; + +// A common application scenario is to apply InplaceToFunctionalActivation +// before some JIT optimization passes, so that those passes are less +// constrained by in-place ops. After those passes are done, we can call +// FunctionalToInplaceActivation to recover in-place activation ops, +// so that we won't lose the performance benefit coming from memory reduction. + +// Replaces functional aten activation ops with their in-place equivalents +TORCH_API bool FunctionalToInplaceActivation( + const std::shared_ptr& graph); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/shape_analysis.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/shape_analysis.h new file mode 100644 index 0000000000000000000000000000000000000000..670072a0b09b45337cd8bd80eb5bd9e12ee7f0dc --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/shape_analysis.h @@ -0,0 +1,43 @@ +#pragma once + +#include +#include +#include + +namespace torch { +namespace jit { + +struct Graph; + +struct propagation_error : std::exception {}; + +class PropertyPropBase { + // Used for both Shape Propagation and Dtype/Device Propagation + public: + explicit PropertyPropBase(std::shared_ptr graph) + : graph_(std::move(graph)) {} + virtual ~PropertyPropBase() = default; + + void propagateBlock(Block* block, bool insert_expands = true); + // insert_expands is used for shape inference + + void processIf(Node* node); + void processLoop(Node* node); + + protected: + virtual void propagateNode(Node* node, bool insert_expands = true) = 0; + void setUnshapedType(Value* o); + void setUnshapedType(Node* node); + std::shared_ptr graph_; +}; + +TORCH_API void EraseShapeInformation(const std::shared_ptr& graph); +TORCH_API void PropagateInputShapes(const std::shared_ptr& graph); + +TORCH_API bool mergeTypes( + ArrayRef lhs, + ArrayRef rhs, + ArrayRef outputs); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/symbolic_shape_analysis.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/symbolic_shape_analysis.h new file mode 100644 index 0000000000000000000000000000000000000000..942fc887f2f938f5f1b50906ed8e1b55cc15239f --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/symbolic_shape_analysis.h @@ -0,0 +1,58 @@ +#pragma once + +#include +#include +#include +#include +#include + +namespace torch { +namespace jit { + +// CAUTION NOT TO BE USED, STILL A WIP, NOT STABLE + +TORCH_API void PropagateShapesOnGraph(std::shared_ptr& graph); + +// CAUTION NOT TO BE USED, STILL A WIP, NOT STABLE +// From [beg, end) attempt to propagate shapes and +// build up a graph that will compute all remaining symbolic +// shapes in [beg, end) that can be executed before beg + +struct ShapeComputeGraphMapping { + ShapeComputeGraphMapping( + std::shared_ptr partial_eval_shape_graph, + std::unordered_map + enclosing_graph_value_to_shape_graph_input, + std::unordered_map graph_output_to_symbolic_shape_dim) + : partial_eval_shape_graph(std::move(partial_eval_shape_graph)), + enclosing_graph_value_to_shape_graph_input_( + std::move(enclosing_graph_value_to_shape_graph_input)), + graph_output_to_symbolic_shape_dim_( + std::move(graph_output_to_symbolic_shape_dim)){}; + + std::shared_ptr partial_eval_shape_graph; + std::unordered_map + enclosing_graph_value_to_shape_graph_input_; + std::unordered_map graph_output_to_symbolic_shape_dim_; +}; + +TORCH_API c10::optional +PropagateShapesAndBuildLargeShapeComputeGraph( + std::shared_ptr& graph, + Node* beg, + Node* end); + +// don't insert complete tensor shapes in shape compute graphs and instead +// rely on our partial evaluation pipeline to propagate information. +// this is a good proxy for our ability to propagate non-complete shape +// information. +TORCH_API bool setSymbolicShapeAnalysisTestMode(bool value); +TORCH_API bool symbolicShapeAnalysisTestModeEnabled(); + +using SSAInput = c10::variant; +TORCH_API c10::optional> +calculateSymbolicShapesOnOp( + const FunctionSchema* schema, + const std::vector& inputs); +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/symbolic_shape_runtime_fusion.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/symbolic_shape_runtime_fusion.h new file mode 100644 index 0000000000000000000000000000000000000000..0c88e11d44848e418f265ad3a5a2d249be7aa725 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/symbolic_shape_runtime_fusion.h @@ -0,0 +1,55 @@ +#pragma once + +#include +#include +#include + +#include + +namespace torch { +namespace jit { + +// Takes in a TensorExprGraph of static shapes and generalizes the input shapes +// to symbolic dimensions. Dimensions of value 1 will be preserved, otherwise +// dimensions with the same value will be bucketed to the same symbolic shape. +// E.g. Tensor(5, 3), Tensor(3, 1) -> Tensor(SS(-1), SS(-2)), Tensor(SS(-2), 1) +// From there, runs symbolic shape inference on the graph, and creates a +// versionining if in the graph with prim::TensorExprDynamicGuard checking if +// the inputs at runtime match the Generalized Symbolic Shapes that are inputs +// to the TE Kernel. The computate to calculate all symbolic dimensions is +// inlined in to the if block with the TE Kernel. All Sym Dim Value* are +// appended to the end of the TE Kernel Graph/Node inputs, and the Node is +// augmented with a integer list attr `symbolic_shape_inputs` that gives the +// mapping from Value * -> Symbolic Shape int64_t value. For more lengthy IR +// examples and walkthrough look at ShapeAnalysisTest.DynamicShapesFusion in +// `test_shape_analysis` Returns True on Success, False on Failure, can fail if +// shape propagation fails to propagate # of dims or if complete shapes on +// inputs not set + +TORCH_API bool GenerateGuard( + Node* tensorexpr_graph_node, + bool add_composed_op = false); + +TORCH_API void runTensorExprDynamicGroup(const Code& code, Stack& stack); + +enum class StrideInput { + // Tensors natively store whether they are contiguous or not as a property + // this makes it faster to query `is_contiguous` or + // `is_contiguous(memory_format=channels_last)` + // than looping through the sizes/strides yourself + // For tensors with these properties, we only store one value: + TENSOR_CONT, + TENSOR_CONT_CHANNELS_LAST, + // now, we describe other cases, where there is one stride enum + // per dimension + S_ONE, // STRIDE_ONE: packed + S_CONT, // STRIDE_CONTIGUOUS: stride[i + 1] * sizes[i + 1] + S_TRAN_CONT, // STRIDE_TRANSPOSED_CONTIGUOUS: stride[i-1] * sizes[i-1] + S_AS_ARG, // STRIDE_AS_ARG: stride passed in as runtime value +}; + +TORCH_API std::string toString(StrideInput si); +TORCH_API StrideInput strideInputFromString(const std::string& si); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/update_differentiable_graph_requires_grad.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/update_differentiable_graph_requires_grad.h new file mode 100644 index 0000000000000000000000000000000000000000..eb51ba00c4c9f8d2ca07dd96def6f5e168160e35 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/update_differentiable_graph_requires_grad.h @@ -0,0 +1,20 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Because differentiable graphs detach the gradients of input Tensors, +// creating and inlining differentiable graphs changes the requires_grad +// property of tensors in the graph. This pass updates prim::profiles +// requires_grad to keep profiled properties up to date, it does not update +// grad properties of other nodes like graph inputs bc the only downstream +// user of the grad property is the profiling executor, which just uses +// the types of prim::profiles +TORCH_API void UpdateDifferentiableGraphRequiresGrad( + std::shared_ptr& diff_forward_graph, + c10::optional new_requires_grad); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/xnnpack_rewrite.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/xnnpack_rewrite.h new file mode 100644 index 0000000000000000000000000000000000000000..d1a64c52c9230ad85a3c3540e120b48532abd707 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/passes/xnnpack_rewrite.h @@ -0,0 +1,21 @@ +#pragma once + +#include +#include +#include + +namespace torch { +namespace jit { + +TORCH_API void transformConv1dToConv2d(std::shared_ptr& graph); +TORCH_API void transformConv1dToConv2d(script::Module& module); +TORCH_API void insertPrePackedOps(std::shared_ptr& graph); +TORCH_API void insertPrePackedOps(script::Module& module); +TORCH_API void fusePrePackedLinearConvWithClamp(script::Module& module); +TORCH_API void FoldPrePackingOps(script::Module& module); +TORCH_API script::Module optimizeForMobile( + const script::Module& module, + const std::set& optimization_blocklist = {}, + const std::vector& preserved_methods = {}); +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import.h new file mode 100644 index 0000000000000000000000000000000000000000..61b96222f6f77abfebefeb7f8fbaa5c52e915c9b --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import.h @@ -0,0 +1,152 @@ +#pragma once + +#include +#include +#include +#include +#include + +#include + +namespace caffe2 { +namespace serialize { +class ReadAdapterInterface; +} // namespace serialize +} // namespace caffe2 + +namespace torch { +namespace jit { + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + const std::string& filename, + c10::optional device = c10::nullopt, + bool load_debug_files = true); + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + std::istream& in, + c10::optional device = c10::nullopt, + bool load_debug_files = true); + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + std::unique_ptr rai, + c10::optional device = c10::nullopt, + bool load_debug_files = true); + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + const std::string& filename, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true, + bool restore_shapes = false); + +// For reading unified serialization format from torch.Package +TORCH_API Module import_ir_module( + std::shared_ptr cu, + std::shared_ptr reader, + std::shared_ptr storage_context, + c10::optional device, + std::string ts_id /* torchscript identifier inside package */); + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + std::istream& in, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true, + bool restore_shapes = false); + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + std::unique_ptr rai, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true); + +TORCH_API Module import_ir_module( + std::shared_ptr cu, + std::shared_ptr rai, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true); + +/// Loads a serialized `Module` from the given `istream`. +/// +/// The istream must contain a serialized `Module`, exported via +/// `torch::jit::ExportModule` in C++. +TORCH_API Module load( + std::istream& in, + c10::optional device = c10::nullopt, + bool load_debug_files = true); + +TORCH_API Module load( + std::istream& in, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true); + +/// Loads a serialized `Module` from the given `filename`. +/// +/// The file stored at the location given in `filename` must contain a +/// serialized `Module`, exported either via `ScriptModule.save()` in +/// Python or `torch::jit::ExportModule` in C++. +TORCH_API Module load( + const std::string& filename, + c10::optional device = c10::nullopt, + bool load_debug_files = true); + +TORCH_API Module load( + const std::string& filename, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true); + +/// Loads a serialized `Module` from the given shared_ptr `rai`. +/// +/// The reader adapter, which is for customized input stream, must contain a +/// serialized `Module`, exported either via `ScriptModule.save()` in +/// Python or `torch::jit::ExportModule` in C++. +TORCH_API Module load( + std::shared_ptr rai, + c10::optional device = c10::nullopt, + bool load_debug_files = true); + +TORCH_API Module load( + std::shared_ptr rai, + c10::optional device, + ExtraFilesMap& extra_files, + bool load_debug_files = true); + +TORCH_API Module jitModuleFromSourceAndConstants( + const IValue& ivalue, + const ExtraFilesMap& source, + const std::vector& constants, + int32_t version); + +TORCH_API Module parse_and_initialize_jit_module( + std::shared_ptr data, + size_t size, + ExtraFilesMap& extra_files, + c10::optional device = c10::nullopt); + +TORCH_API Module load_jit_module_from_file( + const std::string& filename, + ExtraFilesMap& extra_files, + c10::optional device = c10::nullopt); + +TORCH_API Module load_jit_module_from_stream( + std::istream& in, + ExtraFilesMap& extra_files, + c10::optional device = c10::nullopt); + +TORCH_API Module parse_and_initialize_jit_module( + std::shared_ptr data, + size_t size, + ExtraFilesMap& extra_files, + c10::optional device); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import_export_functions.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import_export_functions.h new file mode 100644 index 0000000000000000000000000000000000000000..0de156bfb753c4aa78c7a0f62d9a167acb205ab9 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import_export_functions.h @@ -0,0 +1,16 @@ +#pragma once +#include + +// Functions that are used in both import and export processes +namespace torch { +namespace jit { +using c10::IValue; +IValue expect_field( + c10::ivalue::TupleElements& elements, + const std::string& expected_name, + size_t entry); +std::string operator_str( + const std::string& name, + const std::string& overloadname); +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import_source.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import_source.h new file mode 100644 index 0000000000000000000000000000000000000000..9a720a81bcbb2085a4f3f21ff5e73d45d9afaf1b --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/import_source.h @@ -0,0 +1,103 @@ +#pragma once + +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include +#include + +namespace torch { +namespace jit { + +using SourceLoader = std::function(const std::string&)>; + +struct SourceImporterImpl : public Resolver, + std::enable_shared_from_this { + SourceImporterImpl( + std::shared_ptr cu, + const std::vector* constant_table, + SourceLoader source_loader, + size_t version); + TypePtr findNamedType(const QualifiedName& name); + Function* findFunction(const QualifiedName& name); + void parseSourceIfNeeded(const std::string& qualifier); + void LEGACY_import_methods( + const Module& mod, + const std::shared_ptr& src); + + std::shared_ptr resolveValue( + const std::string& name, + GraphFunction& m, + const SourceRange& loc) override; + TypePtr resolveType(const std::string& name, const SourceRange& loc) override; + + private: + void importFunction(const std::string& qualifier, const Def& def); + void importNamedType(const std::string& qualifier, const ClassDef& class_def); + c10::optional attributeAssignmentSpecialHandlingHack( + const QualifiedName& qualified_classname, + const Assign& assign); + void importClass( + const QualifiedName& qualified_classname, + const ClassDef& class_def, + bool is_module); + void importEnum( + const QualifiedName& qualified_name, + const ClassDef& enum_def); + void importNamedTuple( + const QualifiedName& qualified_name, + const ClassDef& named_tuple_def); + + void parsePossibleVersionNumber(Lexer& L); + + void parseImports(Lexer& L); + + std::shared_ptr cu_; + std::unordered_map> env_; + SourceLoader source_loader_; + c10::optional version_ = c10::nullopt; + std::unordered_set loaded_sources_; + // named types and functions loaded from a file but not yet defined because + // their type has not been requested yet. + std::unordered_map to_be_defined_; +}; + +// Given a directory of serialized TorchScript sources, +// This class allows the loading of individual named types in source. +// Resolves the dependencies between source files and parses +// the source files as necessary. + +struct TORCH_API SourceImporter { + SourceImporter( + // The compilation unit that will own the imported source + std::shared_ptr cu, + const std::vector* constant_table, + SourceLoader loader, + size_t version); + + TypePtr loadType(const QualifiedName& name) const; + + // Add the methods defined in `src` to the module `mod`, using SourceImporter + // to resolve any classes via loadType + void LEGACY_import_methods( + const Module& mod, + const std::shared_ptr& src); + ~SourceImporter(); + + private: + std::shared_ptr pImpl; +}; + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/pickle.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/pickle.h new file mode 100644 index 0000000000000000000000000000000000000000..11e741740e022b8bec74598022e35094ae792447 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/pickle.h @@ -0,0 +1,91 @@ +#pragma once + +#include +#include +#include +#include +#include +#include + +namespace torch { +namespace jit { + +/// Pickle an IValue by calling a function to handle writing the data. +/// +/// `writer` is a function that takes in a pointer to a chunk of memory and its +/// size and consumes it. +/// +/// See `jit::pickle` for more details. +TORCH_API void pickle( + std::function writer, + const IValue& ivalue, + std::vector* tensor_table = nullptr); + +/// Save a `torch::IValue` in a format compatible with Python's `pickle` module +/// +/// If present, `tensor_table` is a pointer to a table in which tensors that +/// are contained within `ivalue` are stored, and the bytes returned by the +/// pickler will only include references to these tensors in the table. This can +/// be used to keep the binary blob size small. +/// If not provided, tensors are stored in the same byte stream as the pickle +/// data, similar to `torch.save()` in eager Python. +/// +/// Pickled values can be loaded in Python and C++: +/// \rst +/// .. code-block:: cpp +/// +/// torch::IValue float_value(2.3); +/// +/// // TODO: when tensors are stored in the pickle, delete this +/// std::vector tensor_table; +/// auto data = torch::jit::pickle(float_value, &tensor_table); +/// +/// std::vector ivalues = +/// torch::jit::unpickle(data.data(), data.size()); +/// +/// .. code-block:: python +/// +/// values = torch.load('data.pkl') +/// print(values) +/// +/// \endrst +TORCH_API std::vector pickle( + const IValue& ivalue, + std::vector* tensor_table = nullptr); + +/// Save a `torch::IValue` in a format that can be loaded by both +/// `torch::pickle_load` in C++ and `torch.load` in Python. +TORCH_API std::vector pickle_save(const IValue& ivalue); + +/// Deserialize a `torch::IValue` from bytes produced by either +/// `torch::pickle_save` in C++ or `torch.save` in Python +TORCH_API IValue pickle_load(const std::vector& data); + +/// `reader` is a function that takes in a size to read from some pickled +/// binary. `reader` should remember where it last read, and return +/// the number of bytes read. +/// See `torch::pickle` for details. +/// type_resolver is used to resolve any JIT type based on type str +TORCH_API IValue unpickle( + std::function reader, + TypeResolver type_resolver, + c10::ArrayRef tensor_table, + c10::TypePtr (*type_parser)(const std::string&) = + Unpickler::defaultTypeParser); + +/// Decode a chunk of memory containing pickled data into its `torch::IValue`s. +/// +/// If any `torch::IValue`s in the pickled data are `Object`s, then a +/// `class_resolver` function must be provided. +/// +/// See `torch::pickle` for details. +TORCH_API IValue unpickle( + const char* data, + size_t size, + TypeResolver type_resolver = nullptr, + c10::ArrayRef tensor_table = {}, + c10::TypePtr (*type_parser)(const std::string&) = + Unpickler::defaultTypeParser); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/python_print.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/python_print.h new file mode 100644 index 0000000000000000000000000000000000000000..94fb83d7aab774bfa6aa74e626260fb839f316b3 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/python_print.h @@ -0,0 +1,61 @@ +#pragma once +#include +#include +#include +#include +#include + +namespace torch { +namespace jit { + +struct Method; +struct Module; +struct PythonPrintImpl; + +struct PrintDepsTable { + void add(const c10::NamedTypePtr& type); + + size_t size() const { + return table_.size(); + } + + const c10::NamedTypePtr& operator[](size_t index) const { + return table_[index]; + } + + private: + std::vector table_; + std::unordered_set non_unique_; +}; + +struct TORCH_API PythonPrint { + PythonPrint( + std::vector& constant_table, + PrintDepsTable& deps_table, + c10::TypePrinter type_printer = nullptr, + bool enforce_importable = false); + + void printNamedType(const c10::NamedTypePtr& classType); + void printFunction(const Function& callee); + void printMethod(const Function& callee); + + std::string str() const; + const SourceRangeRecords& ranges() const; + uint64_t minVersion() const; + + ~PythonPrint(); + + private: + std::shared_ptr pImpl; +}; + +TORCH_API bool printerHasSpecialCaseFor(c10::Symbol sym); + +TORCH_API void jitModuleToPythonCodeAndConstants( + const Module& module, + ExtraFilesMap* jit_sources, // output + std::vector* constants // output +); + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/source_range_serialization_impl.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/source_range_serialization_impl.h new file mode 100644 index 0000000000000000000000000000000000000000..2b7cd5a14ba9282090b025f23cdf28eb9bf1c5de --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/source_range_serialization_impl.h @@ -0,0 +1,30 @@ +#pragma once + +#include + +namespace torch { +namespace jit { + +// Do this clownyness with virtual functions because of the split +// between ATen core and torch + +class ConcreteSourceRangeUnpickler : public SourceRangeUnpickler { + public: + ConcreteSourceRangeUnpickler(at::DataPtr&& data, size_t size); + + c10::optional findSourceRangeThatGenerated( + const SourceRange& range) override; + + private: + at::DataPtr data; + size_t size; + + void unpickle(); + + std::mutex mutex; + std::shared_ptr deserializer; + std::shared_ptr unpickled_records; +}; + +} // namespace jit +} // namespace torch diff --git a/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/type_name_uniquer.h b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/type_name_uniquer.h new file mode 100644 index 0000000000000000000000000000000000000000..addedc5492cff19673d777887185cc894bf77321 --- /dev/null +++ b/wemm/lib/python3.10/site-packages/torch/include/torch/csrc/jit/serialization/type_name_uniquer.h @@ -0,0 +1,33 @@ +#pragma once + +#include +#include + +namespace torch { +namespace jit { + +/** + * class TypeNameUniquer + * + * Generates a unique name for every type `t` passed in. Types that compare + * equal with EqualType will receive the same unique name. + * + * This is used during Module::save(), to resolve type name collisions during + * serialization. + */ +class TORCH_API TypeNameUniquer { + public: + c10::QualifiedName getUniqueName(c10::ConstNamedTypePtr t); + + private: + NameMangler mangler_; + std::unordered_set used_names_; + std::unordered_map< + c10::ConstNamedTypePtr, + c10::QualifiedName, + HashType, + EqualType> + name_map_; +}; +} // namespace jit +} // namespace torch