Spaces:
Running on Zero
Running on Zero
File size: 11,066 Bytes
4417ac0 | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229 230 231 232 233 234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 293 294 295 296 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 322 323 324 325 326 327 328 329 330 331 332 333 334 335 336 337 338 339 340 341 342 343 344 345 346 347 348 349 350 351 352 353 354 355 356 357 358 359 360 | # Copyright (c) 2018-2022, NVIDIA Corporation
# All rights reserved.
#
# Redistribution and use in source and binary forms, with or without
# modification, are permitted provided that the following conditions are met:
#
# 1. Redistributions of source code must retain the above copyright notice, this
# list of conditions and the following disclaimer.
#
# 2. Redistributions in binary form must reproduce the above copyright notice,
# this list of conditions and the following disclaimer in the documentation
# and/or other materials provided with the distribution.
#
# 3. Neither the name of the copyright holder nor the names of its
# contributors may be used to endorse or promote products derived from
# this software without specific prior written permission.
#
# THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS"
# AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE
# IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE
# DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE
# FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL
# DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR
# SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
# CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY,
# OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE
# OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
from typing import Tuple
import torch
from torch import Tensor
def euler_from_quaternion(quat_angle):
"""
Convert a quaternion into euler angles (roll, pitch, yaw)
roll is rotation around x in radians (counterclockwise)
pitch is rotation around y in radians (counterclockwise)
yaw is rotation around z in radians (counterclockwise)
"""
x = quat_angle[:,0]; y = quat_angle[:,1]; z = quat_angle[:,2]; w = quat_angle[:,3]
t0 = +2.0 * (w * x + y * z)
t1 = +1.0 - 2.0 * (x * x + y * y)
roll_x = torch.atan2(t0, t1)
t2 = +2.0 * (w * y - z * x)
t2 = torch.clip(t2, -1, 1)
pitch_y = torch.asin(t2)
t3 = +2.0 * (w * z + x * y)
t4 = +1.0 - 2.0 * (y * y + z * z)
yaw_z = torch.atan2(t3, t4)
return roll_x, pitch_y, yaw_z # in radians
@torch.jit.script
def normalize(x, eps: float = 1e-9):
return x / x.norm(p=2, dim=-1).clamp(min=eps, max=None).unsqueeze(-1)
@torch.jit.script
def normalize_angle(x):
return torch.atan2(torch.sin(x), torch.cos(x))
@torch.jit.script
def quat_rotate(q, v):
shape = q.shape
q_w = q[:, -1]
q_vec = q[:, :3]
a = v * (2.0 * q_w ** 2 - 1.0).unsqueeze(-1)
b = torch.cross(q_vec, v, dim=-1) * q_w.unsqueeze(-1) * 2.0
c = q_vec * \
torch.bmm(q_vec.view(shape[0], 1, 3), v.view(
shape[0], 3, 1)).squeeze(-1) * 2.0
return a + b + c
@torch.jit.script
def quat_rotate_inverse(q, v):
shape = q.shape
q_w = q[:, -1]
q_vec = q[:, :3]
a = v * (2.0 * q_w ** 2 - 1.0).unsqueeze(-1)
b = torch.cross(q_vec, v, dim=-1) * q_w.unsqueeze(-1) * 2.0
c = q_vec * \
torch.bmm(q_vec.view(shape[0], 1, 3), v.view(
shape[0], 3, 1)).squeeze(-1) * 2.0
return a - b + c
@torch.jit.script
def quat_from_euler_xyz(roll, pitch, yaw):
cy = torch.cos(yaw * 0.5)
sy = torch.sin(yaw * 0.5)
cr = torch.cos(roll * 0.5)
sr = torch.sin(roll * 0.5)
cp = torch.cos(pitch * 0.5)
sp = torch.sin(pitch * 0.5)
qw = cy * cr * cp + sy * sr * sp
qx = cy * sr * cp - sy * cr * sp
qy = cy * cr * sp + sy * sr * cp
qz = sy * cr * cp - cy * sr * sp
return torch.stack([qx, qy, qz, qw], dim=-1)
@torch.jit.script
def quat_unit(a):
return normalize(a)
@torch.jit.script
def quat_from_angle_axis(angle, axis):
theta = (angle / 2).unsqueeze(-1)
xyz = normalize(axis) * theta.sin()
w = theta.cos()
return quat_unit(torch.cat([xyz, w], dim=-1))
@torch.jit.script
def quat_mul(a, b):
assert a.shape == b.shape
shape = a.shape
a = a.reshape(-1, 4)
b = b.reshape(-1, 4)
x1, y1, z1, w1 = a[:, 0], a[:, 1], a[:, 2], a[:, 3]
x2, y2, z2, w2 = b[:, 0], b[:, 1], b[:, 2], b[:, 3]
ww = (z1 + x1) * (x2 + y2)
yy = (w1 - y1) * (w2 + z2)
zz = (w1 + y1) * (w2 - z2)
xx = ww + yy + zz
qq = 0.5 * (xx + (z1 - x1) * (x2 - y2))
w = qq - ww + (z1 - y1) * (y2 - z2)
x = qq - xx + (x1 + w1) * (x2 + w2)
y = qq - yy + (w1 - x1) * (y2 + z2)
z = qq - zz + (z1 + y1) * (w2 - x2)
quat = torch.stack([x, y, z, w], dim=-1).view(shape)
return quat
@torch.jit.script
def quat_conjugate(a):
shape = a.shape
a = a.reshape(-1, 4)
return torch.cat((-a[:, :3], a[:, -1:]), dim=-1).view(shape)
@torch.jit.script
def quat_to_angle_axis(q):
# computes axis-angle representation from quaternion q
# q must be normalized
min_theta = 1e-5
qx, qy, qz, qw = 0, 1, 2, 3
sin_theta = torch.sqrt(1 - q[..., qw] * q[..., qw])
angle = 2 * torch.acos(q[..., qw])
angle = normalize_angle(angle)
sin_theta_expand = sin_theta.unsqueeze(-1)
axis = q[..., qx:qw] / sin_theta_expand
mask = torch.abs(sin_theta) > min_theta
default_axis = torch.zeros_like(axis)
default_axis[..., -1] = 1
angle = torch.where(mask, angle, torch.zeros_like(angle))
mask_expand = mask.unsqueeze(-1)
axis = torch.where(mask_expand, axis, default_axis)
return angle, axis
@torch.jit.script
def angle_axis_to_exp_map(angle, axis):
# compute exponential map from axis-angle
angle_expand = angle.unsqueeze(-1)
exp_map = angle_expand * axis
return exp_map
@torch.jit.script
def quat_to_exp_map(q):
# compute exponential map from quaternion
# q must be normalized
angle, axis = quat_to_angle_axis(q)
exp_map = angle_axis_to_exp_map(angle, axis)
return exp_map
@torch.jit.script
def quat_to_tan_norm(q):
# represents a rotation using the tangent and normal vectors
ref_tan = torch.zeros_like(q[..., 0:3])
ref_tan[..., 0] = 1
tan = quat_rotate(q, ref_tan)
ref_norm = torch.zeros_like(q[..., 0:3])
ref_norm[..., -1] = 1
norm = quat_rotate(q, ref_norm)
norm_tan = torch.cat([tan, norm], dim=len(tan.shape) - 1)
return norm_tan
@torch.jit.script
def euler_xyz_to_exp_map(roll, pitch, yaw):
q = quat_from_euler_xyz(roll, pitch, yaw)
exp_map = quat_to_exp_map(q)
return exp_map
@torch.jit.script
def exp_map_to_angle_axis(exp_map):
min_theta = 1e-5
angle = torch.norm(exp_map, dim=-1)
angle_exp = torch.unsqueeze(angle, dim=-1)
axis = exp_map / angle_exp
angle = normalize_angle(angle)
default_axis = torch.zeros_like(exp_map)
default_axis[..., -1] = 1
mask = torch.abs(angle) > min_theta
angle = torch.where(mask, angle, torch.zeros_like(angle))
mask_expand = mask.unsqueeze(-1)
axis = torch.where(mask_expand, axis, default_axis)
return angle, axis
@torch.jit.script
def exp_map_to_quat(exp_map):
angle, axis = exp_map_to_angle_axis(exp_map)
q = quat_from_angle_axis(angle, axis)
return q
@torch.jit.script
def slerp(q0, q1, t):
assert(len(t.shape) == len(q0.shape) - 1)
cos_half_theta = torch.sum(q0 * q1, dim=-1)
neg_mask = cos_half_theta < 0
q1 = torch.where(neg_mask.unsqueeze(-1), -q1, q1)
cos_half_theta = torch.abs(cos_half_theta)
cos_half_theta = torch.unsqueeze(cos_half_theta, dim=-1)
half_theta = torch.acos(cos_half_theta)
sin_half_theta = torch.sqrt(1.0 - cos_half_theta * cos_half_theta)
t = t.unsqueeze(-1)
ratioA = torch.sin((1 - t) * half_theta) / sin_half_theta
ratioB = torch.sin(t * half_theta) / sin_half_theta
new_q = ratioA * q0 + ratioB * q1
new_q = torch.where(torch.abs(sin_half_theta) < 0.001, 0.5 * q0 + 0.5 * q1, new_q)
new_q = torch.where(torch.abs(cos_half_theta) >= 1, q0, new_q)
return new_q
@torch.jit.script
def slerp2(q0, q1, t):
cos_half_theta = torch.sum(q0 * q1, dim=-1)
neg_mask = cos_half_theta < 0
q1 = q1.clone()
q1[neg_mask] = -q1[neg_mask]
cos_half_theta = torch.abs(cos_half_theta)
cos_half_theta = torch.unsqueeze(cos_half_theta, dim=-1)
half_theta = torch.acos(cos_half_theta);
sin_half_theta = torch.sqrt(1.0 - cos_half_theta * cos_half_theta);
ratioA = torch.sin((1 - t) * half_theta) / sin_half_theta;
ratioB = torch.sin(t * half_theta) / sin_half_theta;
new_q = ratioA * q0 + ratioB * q1
new_q = torch.where(torch.abs(sin_half_theta) < 0.001, 0.5 * q0 + 0.5 * q1, new_q)
new_q = torch.where(torch.abs(cos_half_theta) >= 1, q0, new_q)
return new_q
@torch.jit.script
def calc_heading(q):
# calculate heading direction from quaternion
# the heading is the direction on the xy plane
# q must be normalized
ref_dir = torch.zeros_like(q[..., 0:3])
ref_dir[..., 0] = 1
rot_dir = quat_rotate(q, ref_dir)
heading = torch.atan2(rot_dir[..., 1], rot_dir[..., 0])
return heading
@torch.jit.script
def calc_heading_quat(q):
# calculate heading rotation from quaternion
# the heading is the direction on the xy plane
# q must be normalized
heading = calc_heading(q)
axis = torch.zeros_like(q[..., 0:3])
axis[..., 2] = 1
heading_q = quat_from_angle_axis(heading, axis)
return heading_q
@torch.jit.script
def calc_heading_quat_inv(q):
# calculate heading rotation from quaternion
# the heading is the direction on the xy plane
# q must be normalized
heading = calc_heading(q)
axis = torch.zeros_like(q[..., 0:3])
axis[..., 2] = 1
heading_q = quat_from_angle_axis(-heading, axis)
return heading_q
@torch.jit.script
def quat_pos(x):
q = x
z = (q[..., 3:] < 0).float()
q = (1 - 2 * z) * q
return q
@torch.jit.script
def quat_to_axis_angle(q):
eps = 1e-5
qx, qy, qz, qw = 0, 1, 2, 3
# need to make sure w is not negative to calculate geodesic distance
q = quat_pos(q)
length = torch.norm(q[..., 0:3], dim=-1, p=2)
angle = 2.0 * torch.atan2(length, q[..., qw])
axis = q[..., qx:qw] / length.unsqueeze(-1)
default_axis = torch.zeros_like(axis)
default_axis[..., -1] = 1
mask = length > eps
angle = torch.where(mask, angle, torch.zeros_like(angle))
mask_expand = mask.unsqueeze(-1)
axis = torch.where(mask_expand, axis, default_axis)
return axis, angle
@torch.jit.script
def quat_diff(q0, q1):
dq = quat_mul(q1, quat_conjugate(q0))
return dq
@torch.jit.script
def quat_diff_angle(q0, q1):
dq = quat_diff(q0, q1)
_, angle = quat_to_axis_angle(dq)
return angle
@torch.jit.script
def axis_angle_to_quat(axis, angle):
# type: (Tensor, Tensor) -> Tensor
theta = (angle / 2).unsqueeze(-1)
xyz = normalize(axis) * theta.sin()
w = theta.cos()
return quat_unit(torch.cat([xyz, w], dim=-1))
|