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That is the question.
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The graph is a line.
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So we all think of it as linear, but go ahead.
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STEVEN G. JOHNSON: Yeah.
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So does it satisfy the rules?
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That's the question.
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So if I multiply the input by 2, does it
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multiply the output by 2?
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No.
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So if we do O of 2--
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no, let's do 3.
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3v, that's, what, 6v plus 1.
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And that's very much not equal to 3Ov,
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which that would be 6v plus 3.
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So this one, it does have a name.
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It's related.
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These are sometimes called affine.
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ALAN EDELMAN: Affine, but not linear even if the graph
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is demonstrably aligned?
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STEVEN G. JOHNSON: Yeah.
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ALAN EDELMAN: They're not linear in the sense of linear algebra.
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STEVEN G. JOHNSON: Right?
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So another one is clearly multiplication by a matrix.
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That's why we do matrices in linear algebra.
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Because they're a nice way of writing down a linear operation
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if your vs are column vectors.
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They're not the only way of writing down linear operation.
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So for example, if you take a column vector
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and multiply it by 3, you could write
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that down as a matrix with all 3s along the diagonal.
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But it's a lot easier to write that down as 3,
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I'd say, as a scalar, than to write it down as a matrix.
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So another example, just to be more--
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so another vector space.
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If you took 1806, you learned that we can have a-- whoops,
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I have to get my color scheme.
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Yeah, so my vectors are red.
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Suppose the vector space V is the set of functions f of x
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that take real numbers in and give you real numbers out.
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Those are a perfectly good vector space.
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I can take two functions.
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I can add them or subtract them, get another function.
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I can take a function and multiply by 2,
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get another function.
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ALAN EDELMAN: Wait, how do we get sine plus cosine?
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STEVEN G. JOHNSON: I get sine x plus cosine x.
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It's just got some other function.
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So if you take sine x plus cosine x,
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that's the function f of x equals sine x plus cosine x.
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It's another rule that gives you-- takes
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real numbers to real numbers.
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And so what would be your linear operators on this?
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Well, multiplication by a scalar, that, of course, works.
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So let's think of L on a function f of x is just 2 f
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of x.
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That takes a function in, function out.
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That's linear.
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What about a linear operator on a function of f of x?
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Again, that gives you the derivative, just
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the ordinary 18.01 derivative.
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This is the 18.01 derivative.
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Obviously, that only works if the function is differentiable.
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So maybe we can look at the subspace
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of differentiable functions.
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That's also a vector space.
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Because if I take two differentiable functions
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and add or subtract or multiply by constants,
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they're still differentiable.
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I could also do integration.
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So if f of x that takes a function f of x in
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and gives you the integral from, I don't know,
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0 to x of f prime--
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no, so f of x prime and dx prime if they're integrable.
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Again, we need to restrict what functions
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are allowed if we're taking derivatives or integrals, so
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things where these exist.
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But this is perfectly linear.
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Why?
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Because if I take the function and I double it,
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if I double the integrand, it doubles the integrals.
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If I add two integrands, you add the integrals.
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Integration is a linear operation.
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Derivative is a linear operation.
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Another fun one is suppose we take L of f of x.
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And the output is the function f of x squared.
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So this doesn't look linear.
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I have a square there.
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But why is this linear?
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Why?
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Because, let's see, if I take L of two functions,
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if I have f of x plus g of x, that should be f of x squared
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plus g of x squared.
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I'm squaring the input, not the output.
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So that's equal to L of f plus L of g.
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ALAN EDELMAN: So I'll just comment.
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Leave it to mathematicians to take what most people would
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think of as just a column of numbers
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and abstract it out and say that this finite dimensional column
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of numbers is somehow the same as continuous functions
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or differentiable functions, satisfies the same axioms.