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transforms2d.py
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1201 lines (952 loc) · 35.8 KB
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# Part of Spatial Math Toolbox for Python
# Copyright (c) 2000 Peter Corke
# MIT Licence, see details in top-level file: LICENCE
"""
These functions create and manipulate 2D rotation matrices and rigid-body
transformations as 2x2 SO(2) matrices and 3x3 SE(2) matrices respectively.
These matrices are represented as 2D NumPy arrays.
Vector arguments are what numpy refers to as ``array_like`` and can be a list,
tuple, numpy array, numpy row vector or numpy column vector.
"""
# pylint: disable=invalid-name
import sys
import math
import numpy as np
import scipy.linalg
from spatialmath import base
_eps = np.finfo(np.float64).eps
try: # pragma: no cover
# print('Using SymPy')
import sympy
_symbolics = True
except ImportError: # pragma: no cover
_symbolics = False
# ---------------------------------------------------------------------------------------#
def rot2(theta, unit="rad"):
"""
Create SO(2) rotation
:param theta: rotation angle
:type theta: float
:param unit: angular units: 'rad' [default], or 'deg'
:type unit: str
:return: SO(2) rotation matrix
:rtype: ndarray(2,2)
- ``rot2(θ)`` is an SO(2) rotation matrix (2x2) representing a rotation of θ radians.
- ``rot2(θ, 'deg')`` as above but θ is in degrees.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> rot2(0.3)
>>> rot2(45, 'deg')
"""
theta = base.getunit(theta, unit)
ct = base.sym.cos(theta)
st = base.sym.sin(theta)
# fmt: off
R = np.array([
[ct, -st],
[st, ct]])
# fmt: on
return R
# ---------------------------------------------------------------------------------------#
def trot2(theta, unit="rad", t=None):
"""
Create SE(2) pure rotation
:param theta: rotation angle about X-axis
:type θ: float
:param unit: angular units: 'rad' [default], or 'deg'
:type unit: str
:param t: 2D translation vector, defaults to [0,0]
:type t: array_like(2)
:return: 3x3 homogeneous transformation matrix
:rtype: ndarray(3,3)
- ``trot2(θ)`` is a homogeneous transformation (3x3) representing a rotation of
θ radians.
- ``trot2(θ, 'deg')`` as above but θ is in degrees.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> trot2(0.3)
>>> trot2(45, 'deg', t=[1,2])
.. note:: By default, the translational component is zero but it can be
set to a non-zero value.
:seealso: xyt2tr
"""
T = np.pad(rot2(theta, unit), (0, 1), mode="constant")
if t is not None:
T[:2, 2] = base.getvector(t, 2, "array")
T[2, 2] = 1 # integer to be symbolic friendly
return T
def xyt2tr(xyt, unit="rad"):
"""
Create SE(2) pure rotation
:param xyt: 2d translation and rotation
:type xyt: array_like(3)
:param unit: angular units: 'rad' [default], or 'deg'
:type unit: str
:return: SE(2) matrix
:rtype: ndarray(3,3)
- ``xyt2tr([x,y,θ])`` is a homogeneous transformation (3x3) representing a rotation of
θ radians and a translation of (x,y).
.. runblock:: pycon
>>> from spatialmath.base import *
>>> xyt2tr([1,2,0.3])
>>> xyt2tr([1,2,45], 'deg')
:seealso: tr2xyt
"""
xyt = base.getvector(xyt, 3)
T = np.pad(rot2(xyt[2], unit), (0, 1), mode="constant")
T[:2, 2] = xyt[0:2]
T[2, 2] = 1.0
return T
def tr2xyt(T, unit="rad"):
"""
Convert SE(2) to x, y, theta
:param T: SE(2) matrix
:type T: ndarray(3,3)
:param unit: angular units: 'rad' [default], or 'deg'
:type unit: str
:return: [x, y, θ]
:rtype: ndarray(3)
- ``tr2xyt(T)`` is a vector giving the equivalent 2D translation and
rotation for this SO(2) matrix.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> T = xyt2tr([1, 2, 0.3])
>>> T
>>> tr2xyt(T)
:seealso: trot2
"""
if T.dtype == "O" and _symbolics:
angle = sympy.atan2(T[1, 0], T[0, 0])
else:
angle = math.atan2(T[1, 0], T[0, 0])
return np.r_[T[0, 2], T[1, 2], angle]
# ---------------------------------------------------------------------------------------#
def transl2(x, y=None):
"""
Create SE(2) pure translation, or extract translation from SE(2) matrix
**Create a translational SE(2) matrix**
:param x: translation along X-axis
:type x: float
:param y: translation along Y-axis
:type y: float
:return: SE(2) matrix
:rtype: ndarray(3,3)
- ``T = transl2([X, Y])`` is an SE(2) homogeneous transform (3x3)
representing a pure translation.
- ``T = transl2( V )`` as above but the translation is given by a 2-element
list, dict, or a numpy array, row or column vector.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> import numpy as np
>>> transl2(3, 4)
>>> transl2([3, 4])
>>> transl2(np.array([3, 4]))
**Extract the translational part of an SE(2) matrix**
:param x: SE(2) transform matrix
:type x: ndarray(3,3)
:return: translation elements of SE(2) matrix
:rtype: ndarray(2)
- ``t = transl2(T)`` is the translational part of the SE(3) matrix ``T`` as a
2-element NumPy array.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> import numpy as np
>>> T = np.array([[1, 0, 3], [0, 1, 4], [0, 0, 1]])
>>> transl2(T)
.. note:: This function is compatible with the MATLAB version of the Toolbox. It
is unusual/weird in doing two completely different things inside the one
function.
"""
if base.isscalar(x) and base.isscalar(y):
# (x, y) -> SE(2)
t = np.r_[x, y]
elif base.isvector(x, 2):
# R2 -> SE(2)
t = base.getvector(x, 2)
elif base.ismatrix(x, (3, 3)):
# SE(2) -> R2
return x[:2, 2]
else:
raise ValueError("bad argument")
if t.dtype != "O":
t = t.astype("float64")
T = np.identity(3, dtype=t.dtype)
T[:2, 2] = t
return T
def ishom2(T, check=False):
"""
Test if matrix belongs to SE(2)
:param T: SE(2) matrix to test
:type T: ndarray(3,3)
:param check: check validity of rotation submatrix
:type check: bool
:return: whether matrix is an SE(2) homogeneous transformation matrix
:rtype: bool
- ``ishom2(T)`` is True if the argument ``T`` is of dimension 3x3
- ``ishom2(T, check=True)`` as above, but also checks orthogonality of the
rotation sub-matrix and validitity of the bottom row.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> import numpy as np
>>> T = np.array([[1, 0, 3], [0, 1, 4], [0, 0, 1]])
>>> ishom2(T)
>>> T = np.array([[1, 1, 3], [0, 1, 4], [0, 0, 1]]) # invalid SE(2)
>>> ishom2(T) # a quick check says it is an SE(2)
>>> ishom2(T, check=True) # but if we check more carefully...
>>> R = np.array([[1, 0], [0, 1]])
>>> ishom2(R)
:seealso: isR, isrot2, ishom, isvec
"""
return (
isinstance(T, np.ndarray)
and T.shape == (3, 3)
and (
not check
or (base.isR(T[:2, :2]) and np.all(T[2, :] == np.array([0, 0, 1])))
)
)
def isrot2(R, check=False):
"""
Test if matrix belongs to SO(2)
:param R: SO(2) matrix to test
:type R: ndarray(3,3)
:param check: check validity of rotation submatrix
:type check: bool
:return: whether matrix is an SO(2) rotation matrix
:rtype: bool
- ``isrot2(R)`` is True if the argument ``R`` is of dimension 2x2
- ``isrot2(R, check=True)`` as above, but also checks orthogonality of the rotation matrix.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> import numpy as np
>>> T = np.array([[1, 0, 3], [0, 1, 4], [0, 0, 1]])
>>> isrot2(T)
>>> R = np.array([[1, 0], [0, 1]])
>>> isrot2(R)
>>> R = np.array([[1, 1], [0, 1]]) # invalid SO(2)
>>> isrot2(R) # a quick check says it is an SO(2)
>>> isrot2(R, check=True) # but if we check more carefully...
:seealso: isR, ishom2, isrot
"""
return (
isinstance(R, np.ndarray) and R.shape == (2, 2) and (not check or base.isR(R))
)
# ---------------------------------------------------------------------------------------#
def trinv2(T):
r"""
Invert an SE(2) matrix
:param T: SE(2) matrix
:type T: ndarray(3,3)
:return: inverse of SE(2) matrix
:rtype: ndarray(3,3)
:raises ValueError: bad arguments
Computes an efficient inverse of an SE(2) matrix:
:math:`\begin{pmatrix} {\bf R} & t \\ 0\,0 & 1 \end{pmatrix}^{-1} = \begin{pmatrix} {\bf R}^T & -{\bf R}^T t \\ 0\, 0 & 1 \end{pmatrix}`
.. runblock:: pycon
>>> from spatialmath.base import *
>>> T = trot2(0.3, t=[4,5])
>>> trinv2(T)
>>> T @ trinv2(T)
:SymPy: supported
"""
if not ishom2(T):
raise ValueError("expecting SE(2) matrix")
# inline this code for speed, don't use tr2rt and rt2tr
R = T[:2, :2]
t = T[:2, 2]
Ti = np.zeros((3, 3), dtype=T.dtype)
Ti[:2, :2] = R.T
Ti[:2, 2] = -R.T @ t
Ti[2, 2] = 1
return Ti
def trlog2(T, check=True, twist=False):
"""
Logarithm of SO(2) or SE(2) matrix
:param T: SE(2) or SO(2) matrix
:type T: ndarray(3,3) or ndarray(2,2)
:param check: check that matrix is valid
:type check: bool
:param twist: return a twist vector instead of matrix [default]
:type twist: bool
:return: logarithm
:rtype: ndarray(3,3) or ndarray(3); or ndarray(2,2) or ndarray(1)
:raises ValueError: bad argument
An efficient closed-form solution of the matrix logarithm for arguments that
are SO(2) or SE(2).
- ``trlog2(R)`` is the logarithm of the passed rotation matrix ``R`` which
will be 2x2 skew-symmetric matrix. The equivalent vector from ``vex()``
is parallel to rotation axis and its norm is the amount of rotation about
that axis.
- ``trlog(T)`` is the logarithm of the passed homogeneous transformation
matrix ``T`` which will be 3x3 augumented skew-symmetric matrix. The
equivalent vector from ``vexa()`` is the twist vector (6x1) comprising [v
w].
.. runblock:: pycon
>>> from spatialmath.base import *
>>> trlog2(trot2(0.3))
>>> trlog2(trot2(0.3), twist=True)
>>> trlog2(rot2(0.3))
>>> trlog2(rot2(0.3), twist=True)
:seealso: :func:`~trexp`, :func:`~spatialmath.base.transformsNd.vex`,
:func:`~spatialmath.base.transformsNd.vexa`
"""
if ishom2(T, check=check):
# SE(2) matrix
if base.iseye(T):
# is identity matrix
if twist:
return np.zeros((3,))
else:
return np.zeros((3, 3))
else:
if twist:
return base.vexa(scipy.linalg.logm(T))
else:
return scipy.linalg.logm(T)
elif isrot2(T, check=check):
# SO(2) rotation matrix
if twist:
return base.vex(scipy.linalg.logm(T))
else:
return scipy.linalg.logm(T)
else:
raise ValueError("Expect SO(2) or SE(2) matrix")
# ---------------------------------------------------------------------------------------#
def trexp2(S, theta=None, check=True):
"""
Exponential of so(2) or se(2) matrix
:param S: se(2), so(2) matrix or equivalent velctor
:type T: ndarray(3,3) or ndarray(2,2)
:param theta: motion
:type theta: float
:return: matrix exponential in SE(2) or SO(2)
:rtype: ndarray(3,3) or ndarray(2,2)
:raises ValueError: bad argument
An efficient closed-form solution of the matrix exponential for arguments
that are se(2) or so(2).
For se(2) the results is an SE(2) homogeneous transformation matrix:
- ``trexp2(Σ)`` is the matrix exponential of the se(2) element ``Σ`` which is
a 3x3 augmented skew-symmetric matrix.
- ``trexp2(Σ, θ)`` as above but for an se(3) motion of Σθ, where ``Σ``
must represent a unit-twist, ie. the rotational component is a unit-norm skew-symmetric
matrix.
- ``trexp2(S)`` is the matrix exponential of the se(3) element ``S`` represented as
a 3-vector which can be considered a screw motion.
- ``trexp2(S, θ)`` as above but for an se(2) motion of Sθ, where ``S``
must represent a unit-twist, ie. the rotational component is a unit-norm skew-symmetric
matrix.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> trexp2(skew(1))
>>> trexp2(skew(1), 2) # revolute unit twist
>>> trexp2(1)
>>> trexp2(1, 2) # revolute unit twist
For so(2) the results is an SO(2) rotation matrix:
- ``trexp2(Ω)`` is the matrix exponential of the so(3) element ``Ω`` which is a 2x2
skew-symmetric matrix.
- ``trexp2(Ω, θ)`` as above but for an so(3) motion of Ωθ, where ``Ω`` is
unit-norm skew-symmetric matrix representing a rotation axis and a rotation magnitude
given by ``θ``.
- ``trexp2(ω)`` is the matrix exponential of the so(2) element ``ω`` expressed as
a 1-vector.
- ``trexp2(ω, θ)`` as above but for an so(3) motion of ωθ where ``ω`` is a
unit-norm vector representing a rotation axis and a rotation magnitude
given by ``θ``. ``ω`` is expressed as a 1-vector.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> trexp2(skewa([1, 2, 3]))
>>> trexp2(skewa([1, 0, 0]), 2) # prismatic unit twist
>>> trexp2([1, 2, 3])
>>> trexp2([1, 0, 0], 2)
:seealso: trlog, trexp2
"""
if base.ismatrix(S, (3, 3)) or base.isvector(S, 3):
# se(2) case
if base.ismatrix(S, (3, 3)):
# augmentented skew matrix
if check and not base.isskewa(S):
raise ValueError("argument must be a valid se(2) element")
tw = base.vexa(S)
else:
# 3 vector
tw = base.getvector(S)
if base.iszerovec(tw):
return np.eye(3)
if theta is None:
(tw, theta) = base.unittwist2_norm(tw)
elif not base.isunittwist2(tw):
raise ValueError("If theta is specified S must be a unit twist")
t = tw[0:2]
w = tw[2]
R = base.rodrigues(w, theta)
skw = base.skew(w)
V = (
np.eye(2) * theta
+ (1.0 - math.cos(theta)) * skw
+ (theta - math.sin(theta)) * skw @ skw
)
return base.rt2tr(R, V @ t)
elif base.ismatrix(S, (2, 2)) or base.isvector(S, 1):
# so(2) case
if base.ismatrix(S, (2, 2)):
# skew symmetric matrix
if check and not base.isskew(S):
raise ValueError("argument must be a valid so(2) element")
w = base.vex(S)
else:
# 1 vector
w = base.getvector(S)
if theta is not None and not base.isunitvec(w):
raise ValueError("If theta is specified S must be a unit twist")
# do Rodrigues' formula for rotation
return base.rodrigues(w, theta)
else:
raise ValueError(" First argument must be SO(2), 1-vector, SE(2) or 3-vector")
def adjoint2(T):
# http://ethaneade.com/lie.pdf
if T.shape == (3, 3):
# SO(2) adjoint
return np.identity(2)
elif T.shape == (3, 3):
# SE(2) adjoint
(R, t) = base.tr2rt(T)
# fmt: off
return np.block([
[R, np.c_[t[1], -t[0]].T],
[0, 0, 1]
])
# fmt: on
else:
raise ValueError("bad argument")
def tr2jac2(T):
r"""
SE(2) Jacobian matrix
:param T: SE(2) matrix
:type T: ndarray(3,3)
:return: Jacobian matrix
:rtype: ndarray(3,3)
Computes an Jacobian matrix that maps spatial velocity between two frames defined by
an SE(2) matrix.
``tr2jac2(T)`` is a Jacobian matrix (3x3) that maps spatial velocity or
differential motion from frame {B} to frame {A} where the pose of {B}
elative to {A} is represented by the homogeneous transform T = :math:`{}^A {\bf T}_B`.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> T = trot2(0.3, t=[4,5])
>>> tr2jac2(T)
:Reference: Robotics, Vision & Control: Second Edition, P. Corke, Springer 2016; p65.
:SymPy: supported
"""
if not ishom2(T):
raise ValueError("expecting an SE(2) matrix")
J = np.eye(3, dtype=T.dtype)
J[:2, :2] = base.t2r(T)
return J
def trinterp2(start, end, s=None):
"""
Interpolate SE(2) or SO(2) matrices
:param start: initial SE(2) or SO(2) matrix value when s=0, if None then identity is used
:type start: ndarray(3,3) or ndarray(2,2) or None
:param end: final SE(2) or SO(2) matrix, value when s=1
:type end: ndarray(3,3) or ndarray(2,2)
:param s: interpolation coefficient, range 0 to 1
:type s: float
:return: interpolated SE(2) or SO(2) matrix value
:rtype: ndarray(3,3) or ndarray(2,2)
:raises ValueError: bad arguments
- ``trinterp2(None, T, S)`` is an SE(2) matrix interpolated
between identity when `S`=0 and `T` when `S`=1.
- ``trinterp2(T0, T1, S)`` as above but interpolated
between `T0` when `S`=0 and `T1` when `S`=1.
- ``trinterp2(None, R, S)`` is an SO(2) matrix interpolated
between identity when `S`=0 and `R` when `S`=1.
- ``trinterp2(R0, R1, S)`` as above but interpolated
between `R0` when `S`=0 and `R1` when `S`=1.
.. note:: Rotation angle is linearly interpolated.
.. runblock:: pycon
>>> from spatialmath.base import *
>>> T1 = transl2(1, 2)
>>> T2 = transl2(3, 4)
>>> trinterp2(T1, T2, 0)
>>> trinterp2(T1, T2, 1)
>>> trinterp2(T1, T2, 0.5)
>>> trinterp2(None, T2, 0)
>>> trinterp2(None, T2, 1)
>>> trinterp2(None, T2, 0.5)
:seealso: :func:`~spatialmath.base.transforms3d.trinterp`
"""
if base.ismatrix(end, (2, 2)):
# SO(2) case
if start is None:
# TRINTERP2(T, s)
th0 = math.atan2(end[1, 0], end[0, 0])
th = s * th0
else:
# TRINTERP2(T1, start= s)
if start.shape != end.shape:
raise ValueError("start and end matrices must be same shape")
th0 = math.atan2(start[1, 0], start[0, 0])
th1 = math.atan2(end[1, 0], end[0, 0])
th = th0 * (1 - s) + s * th1
return rot2(th)
elif base.ismatrix(end, (3, 3)):
if start is None:
# TRINTERP2(T, s)
th0 = math.atan2(end[1, 0], end[0, 0])
p0 = transl2(end)
th = s * th0
pr = s * p0
else:
# TRINTERP2(T0, T1, s)
if start.shape != end.shape:
raise ValueError("both matrices must be same shape")
th0 = math.atan2(start[1, 0], start[0, 0])
th1 = math.atan2(end[1, 0], end[0, 0])
p0 = transl2(start)
p1 = transl2(end)
pr = p0 * (1 - s) + s * p1
th = th0 * (1 - s) + s * th1
return base.rt2tr(rot2(th), pr)
else:
return ValueError("Argument must be SO(2) or SE(2)")
def trprint2(T, label=None, file=sys.stdout, fmt="{:.3g}", unit="deg"):
"""
Compact display of SE(2) or SO(2) matrices
:param T: matrix to format
:type T: ndarray(3,3) or ndarray(2,2)
:param label: text label to put at start of line
:type label: str
:param file: file to write formatted string to
:type file: file object
:param fmt: conversion format for each number
:type fmt: str
:param unit: angular units: 'rad' [default], or 'deg'
:type unit: str
:return: formatted string
:rtype: str
The matrix is formatted and written to ``file`` and the
string is returned. To suppress writing to a file, set ``file=None``.
- ``trprint2(R)`` displays the SO(2) rotation matrix in a compact
single-line format and returns the string::
[LABEL:] θ UNIT
- ``trprint2(T)`` displays the SE(2) homogoneous transform in a compact
single-line format and returns the string::
[LABEL:] [t=X, Y;] θ UNIT
.. runblock:: pycon
>>> from spatialmath.base import *
>>> T = transl2(1,2) @ trot2(0.3)
>>> trprint2(T, file=None, label='T')
>>> trprint2(T, file=None, label='T', fmt='{:8.4g}')
.. notes::
- Default formatting is for compact display of data
- For tabular data set ``fmt`` to a fixed width format such as
``fmt='{:.3g}'``
:seealso: trprint
"""
s = ""
if label is not None:
s += "{:s}: ".format(label)
# print the translational part if it exists
if ishom2(T):
s += "t = {};".format(_vec2s(fmt, transl2(T)))
angle = math.atan2(T[1, 0], T[0, 0])
if unit == "deg":
angle *= 180.0 / math.pi
s += " {}°".format(_vec2s(fmt, [angle]))
else:
s += " {} rad".format(_vec2s(fmt, [angle]))
if file:
print(s, file=file)
return s
def _vec2s(fmt, v):
v = [x if np.abs(x) > 100 * _eps else 0.0 for x in v]
return ", ".join([fmt.format(x) for x in v])
def points2tr2(p1, p2):
"""
SE(2) transform from corresponding points
:param p1: first set of points
:type p1: array_like(2,N)
:param p2: second set of points
:type p2: array_like(2,N)
:return: transform from ``p1`` to ``p2``
:rtype: ndarray(3,3)
Compute an SE(2) matrix that transforms the point set ``p1`` to ``p2``.
p1 and p2 must have the same number of columns, and columns correspond
to the same point.
"""
# first find the centroids of both point clouds
p1_centroid = np.mean(p1, axis=0)
p2_centroid = np.mean(p2, axis=0)
# get the point clouds in reference to their centroids
p1_centered = p1 - p1_centroid
p2_centered = p2 - p2_centroid
# compute moment matrix
M = np.dot(p2_centered.T, p1_centered)
# get singular value decomposition of the cross covariance matrix
U, W, VT = np.linalg.svd(M)
# get rotation between the two point clouds
R = U @ VT
# special reflection case
if np.linalg.det(R) < 0:
VT[-1, :] *= -1
R = VT.T @ U.T
# get the translation
t = np.expand_dims(p2_centroid, 0).T - np.dot(R, np.expand_dims(p1_centroid, 0).T)
# assemble translation and rotation into a transformation matrix
T = np.identity(3)
T[:2, 2] = np.squeeze(t)
T[:2, :2] = R
return T
# https://github.com/ClayFlannigan/icp/blob/master/icp.py
# https://github.com/1988kramer/intel_dataset/blob/master/scripts/Align2D.py
# hack below to use points2tr above
# use ClayFlannigan's improved data association
from scipy.spatial import KDTree
import numpy as np
# reference or target 2xN
# source 2xN
# params:
# source_points: numpy array containing points to align to the reference set
# points should be homogeneous, with one point per row
# reference_points: numpy array containing points to which the source points
# are to be aligned, points should be homogeneous with one
# point per row
# initial_T: initial estimate of the transform between reference and source
# def __init__(self, source_points, reference_points, initial_T):
# self.source = source_points
# self.reference = reference_points
# self.init_T = initial_T
# self.reference_tree = KDTree(reference_points[:,:2])
# self.transform = self.AlignICP(30, 1.0e-4)
# uses the iterative closest point algorithm to find the
# transformation between the source and reference point clouds
# that minimizes the sum of squared errors between nearest
# neighbors in the two point clouds
# params:
# max_iter: int, max number of iterations
# min_delta_err: float, minimum change in alignment error
def ICP2d(reference, source, T=None, max_iter=20, min_delta_err=1e-4):
mean_sq_error = 1.0e6 # initialize error as large number
delta_err = 1.0e6 # change in error (used in stopping condition)
num_iter = 0 # number of iterations
if T is None:
T = np.eye(3)
ref_kdtree = KDTree(reference.T)
tf_source = source
source_hom = np.vstack((source, np.ones(source.shape[1])))
while delta_err > min_delta_err and num_iter < max_iter:
# find correspondences via nearest-neighbor search
matched_ref_pts, matched_source, indices = _FindCorrespondences(ref_kdtree, tf_source, reference)
# find alingment between source and corresponding reference points via SVD
# note: svd step doesn't use homogeneous points
new_T = _AlignSVD(matched_source, matched_ref_pts)
# update transformation between point sets
T = T @ new_T
# apply transformation to the source points
tf_source = T @ source_hom
tf_source = tf_source[:2, :]
# find mean squared error between transformed source points and reference points
# TODO: do this with fancy indexing
new_err = 0
for i in range(len(indices)):
if indices[i] != -1:
diff = tf_source[:, i] - reference[:, indices[i]]
new_err += np.dot(diff,diff.T)
new_err /= float(len(matched_ref_pts))
# update error and calculate delta error
delta_err = abs(mean_sq_error - new_err)
mean_sq_error = new_err
print('ITER', num_iter, delta_err, mean_sq_error)
num_iter += 1
return T
def _FindCorrespondences(tree, source, reference):
# get distances to nearest neighbors and indices of nearest neighbors
dist, indices = tree.query(source.T)
# remove multiple associatons from index list
# only retain closest associations
unique = False
matched_src = source.copy()
while not unique:
unique = True
for i, idxi in enumerate(indices):
if idxi == -1:
continue
# could do this with np.nonzero
for j in range(i+1,len(indices)):
if idxi == indices[j]:
if dist[i] < dist[j]:
indices[j] = -1
else:
indices[i] = -1
break
# build array of nearest neighbor reference points
# and remove unmatched source points
point_list = []
src_idx = 0
for idx in indices:
if idx != -1:
point_list.append(reference[:,idx])
src_idx += 1
else:
matched_src = np.delete(matched_src, src_idx, axis=1)
matched_ref = np.array(point_list).T
return matched_ref, matched_src, indices
# uses singular value decomposition to find the
# transformation from the reference to the source point cloud
# assumes source and reference point clounds are ordered such that
# corresponding points are at the same indices in each array
#
# params:
# source: numpy array representing source pointcloud
# reference: numpy array representing reference pointcloud
# returns:
# T: transformation between the two point clouds
# TODO: replace this func with
def _AlignSVD(source, reference):
# first find the centroids of both point clouds
src_centroid = source.mean(axis=1)
ref_centroid = reference.mean(axis=1)
# get the point clouds in reference to their centroids
source_centered = source - src_centroid[:, np.newaxis]
reference_centered = reference - ref_centroid[:, np.newaxis]
# compute the moment matrix
M = reference_centered @ source_centered.T
# do the singular value decomposition
U, W, V_t = np.linalg.svd(M)
# get rotation between the two point clouds
R = U @ V_t
if np.linalg.det(R) < 0:
raise RuntimeError('bad rotation matrix')
# translation is the difference between the point clound centroids
t = ref_centroid - R @ src_centroid
return base.rt2tr(R, t)
def trplot2(
T,
color="blue",
frame=None,
axislabel=True,
axissubscript=True,
textcolor=None,
labels=("X", "Y"),
length=1,
arrow=True,
rviz=False,
ax=None,
block=False,
dims=None,
wtl=0.2,
width=1,
d1=0.1,
d2=1.15,
**kwargs
):
"""
Plot a 2D coordinate frame
:param T: an SE(3) or SO(3) pose to be displayed as coordinate frame
:type: ndarray(3,3) or ndarray(2,2)
:param color: color of the lines defining the frame
:type color: str
:param textcolor: color of text labels for the frame, default color of lines above
:type textcolor: str
:param frame: label the frame, name is shown below the frame and as subscripts on the frame axis labels
:type frame: str
:param axislabel: display labels on axes, default True
:type axislabel: bool
:param axissubscript: display subscripts on axis labels, default True
:type axissubscript: bool
:param labels: labels for the axes, defaults to X and Y
:type labels: 2-tuple of strings
:param length: length of coordinate frame axes, default 1
:type length: float
:param arrow: show arrow heads, default True
:type arrow: bool
:param ax: the axes to plot into, defaults to current axes
:type ax: Axes3D reference
:param block: run the GUI main loop until all windows are closed, default True
:type block: bool
:param dims: dimension of plot volume as [xmin, xmax, ymin, ymax]
:type dims: array_like(4)
:param wtl: width-to-length ratio for arrows, default 0.2
:type wtl: float
:param rviz: show Rviz style arrows, default False
:type rviz: bool
:param projection: 3D projection: ortho [default] or persp
:type projection: str
:param width: width of lines, default 1
:type width: float
:param d1: distance of frame axis label text from origin, default 0.05
:type d1: float
:param d2: distance of frame label text from origin, default 1.15
:type d2: float
:return: axes containing the frame
:rtype: AxesSubplot
:raises ValueError: bad argument
Adds a 2D coordinate frame represented by the SO(2) or SE(2) matrix to the current axes.