spatialmath-python 0.6.1

Provides spatial maths capability for Python.

Spatial Maths for Python

This is a Python implementation of the Spatial Math Toolbox for MATLAB^®, which is a standalone component of the Robotics Toolbox for MATLAB^®.

Spatial mathematics capability underpins all of robotics and robotic vision where we need to describe the position, orientation or pose of objects in 2D or 3D spaces.

• GitHub repository https://github.com/petercorke/spatialmath-python
• Documentation https://petercorke.github.io/spatialmath-python
• Dependencies: numpy, scipy, matplotlib, ffmpeg (if rendering animations as a movie)

What it does

Provides a set of classes:

• SO2 for orientation in 2-dimensions
• SE2 for position and orientation (pose) in 2-dimensions
• SO3 for orientation in 3-dimensions
• SE3 for position and orientation (pose) in 3-dimensions
• UnitQuaternion for orientation in 3-dimensions

which provide convenience and type safety. These classes have methods and overloaded operators to support:

• composition, using the * operator
• point transformation, using the * operator
• exponent, using the ** operator
• normalization
• inversion
• connection to the Lie algebra via matrix exponential and logarithm operations
• conversion of orientation to/from Euler angles, roll-pitch-yaw angles and angle-axis forms.
• list operations such as append, insert and get

These are layered over a set of base functions that perform many of the same operations but represent data explicitly in terms of numpy arrays.

The class, method and functions names largely mirror those of the MATLAB toolboxes, and the semantics are quite similar.

Examples

High-level classes

These classes abstract the low-level numpy arrays into objects that obey the rules associated with the mathematical groups SO(2), SE(2), SO(3), SE(3) as well as twists and quaternions.

Using classes ensures type safety, for example it stops us mixing a 2D homogeneous transformation with a 3D rotation matrix -- both of which are 3x3 matrices. It also ensures that the internal matrix representation is always a valid member of the relevant group.

For example, to create an object representing a rotation of 0.3 radians about the x-axis is simply

>>> R1 = SO3.Rx(0.3)
>>> R1
   1         0         0          
   0         0.955336 -0.29552    
   0         0.29552   0.955336         

while a rotation of 30 deg about the z-axis is

>>> R2 = SO3.Rz(30, 'deg')
>>> R2
   0.866025 -0.5       0          
   0.5       0.866025  0          
   0         0         1    

and the composition of these two rotations is

>>> R = R1 *R2
   0.866025 -0.5       0          
   0.433013  0.75     -0.5        
   0.25      0.433013  0.866025 

We can find the corresponding Euler angles

>> R.eul
array([-1.57079633,  0.52359878,  2.0943951 ])

Frequently in robotics we want a sequence, a trajectory, of rotation matrices or poses. These pose classes inherit capability from the list class

>>> R = SO3()   # the identity
>>> R.append(R1)
>>> R.append(R2)
>>> len(R)
 3
>>> R[1]
   1         0         0          
   0         0.955336 -0.29552    
   0         0.29552   0.955336             

and this can be used in for loops and list comprehensions.

An alternative way of constructing this would be

>>> R = SO3( [ SO3(), R1, R2 ] )       
>>> len(R)
 3

Many of the constructors such as .Rx, .Ry and .Rz support vectorization

>>> R = SO3.Rx( np.arange(0, 2*np.pi, 0.2))
>>> len(R)
 32

which has created, in a single line, a list of rotation matrices.

Vectorization also applies to the operators, for instance

>>> A = R * SO3.Ry(0.5)
>>> len(R)
 32

will produce a result where each element is the product of each element of the left-hand side with the right-hand side, ie. R[i] * SO3.Ry(0.5).

Similarly

>>> A = SO3.Ry(0.5) * R 
>>> len(R)
 32

will produce a result where each element is the product of the left-hand side with each element of the right-hand side , ie. SO3.Ry(0.5) * R[i] .

Finally

>>> A = R * R 
>>> len(R)
 32

will produce a result where each element is the product of each element of the left-hand side with each element of the right-hand side , ie. R[i] * R[i] .

The underlying representation of these classes is a numpy matrix, but the class ensures that the structure of that matrix is valid for the particular group represented: SO(2), SE(2), SO(3), SE(3). Any operation that is not valid for the group will return a matrix rather than a pose class, for example

>>> SO3.Rx(0.3)*2
array([[ 2.        ,  0.        ,  0.        ],
       [ 0.        ,  1.91067298, -0.59104041],
       [ 0.        ,  0.59104041,  1.91067298]])

>>> SO3.Rx(0.3)-1
array([[ 0.        , -1.        , -1.        ],
       [-1.        , -0.04466351, -1.29552021],
       [-1.        , -0.70447979, -0.04466351]])

We can print and plot these objects as well

>>> T = SE3(1,2,3) * SE3.Rx(30, 'deg')
>>> T.print()
   1         0         0         1          
   0         0.866025 -0.5       2          
   0         0.5       0.866025  3          
   0         0         0         1          

>>> T.printline()
t =        1,        2,        3; rpy/zyx =       30,        0,        0 deg

>>> T.plot()

printline is a compact single line format for tabular listing, whereas print shows the underlying matrix and for consoles that support it, it is colorised, with rotational elements in red and translational elements in blue.

Low-level spatial math

Import the low-level transform functions

>>> import spatialmath.base as tr

We can create a 3D rotation matrix

>>> tr.rotx(0.3)
array([[ 1.        ,  0.        ,  0.        ],
       [ 0.        ,  0.95533649, -0.29552021],
       [ 0.        ,  0.29552021,  0.95533649]])

>>> tr.rotx(30, unit='deg')
array([[ 1.       ,  0.       ,  0.       ],
       [ 0.       ,  0.8660254, -0.5      ],
       [ 0.       ,  0.5      ,  0.8660254]])

The results are numpy arrays so to perform matrix multiplication you need to use the @ operator, for example

rotx(0.3) @ roty(0.2)

We also support multiple ways of passing vector information to functions that require it:

• as separate positional arguments

transl2(1, 2)
array([[1., 0., 1.],
       [0., 1., 2.],
       [0., 0., 1.]])

• as a list or a tuple

transl2( [1,2] )
array([[1., 0., 1.],
       [0., 1., 2.],
       [0., 0., 1.]])

transl2( (1,2) )
Out[444]: 
array([[1., 0., 1.],
       [0., 1., 2.],
       [0., 0., 1.]])

• or as a numpy array

transl2( np.array([1,2]) )
Out[445]: 
array([[1., 0., 1.],
       [0., 1., 2.],
       [0., 0., 1.]])

There is a single module that deals with quaternions, unit or not, and the representation is a numpy array of four elements. As above, functions can accept the numpy array, a list, dict or numpy row or column vectors.

>>> from spatialmath.base.quaternion import *
>>> q = qqmul([1,2,3,4], [5,6,7,8])
>>> q
array([-60,  12,  30,  24])
>>> qprint(q)
-60.000000 < 12.000000, 30.000000, 24.000000 >
>>> qnorm(q)
72.24956747275377

Graphics

The functions support various plotting styles

trplot( transl(1,2,3), frame='A', rviz=True, width=1, dims=[0, 10, 0, 10, 0, 10])
trplot( transl(3,1, 2), color='red', width=3, frame='B')
trplot( transl(4, 3, 1)@trotx(math.pi/3), color='green', frame='c', dims=[0,4,0,4,0,4])

Symbolic support

Some functions have support for symbolic variables, for example

import sympy

theta = sym.symbols('theta')
print(rotx(theta))
[[1 0 0]
 [0 cos(theta) -sin(theta)]
 [0 sin(theta) cos(theta)]]

The resulting numpy array is an array of symbolic objects not numbers – the constants are also symbolic objects. You can read the elements of the matrix

a = T[0,0]

a
Out[258]: 1

type(a)
Out[259]: int

a = T[1,1]
a
Out[256]: 
cos(theta)
type(a)
Out[255]: cos

We see that the symbolic constants are converted back to Python numeric types on read.

Similarly when we assign an element or slice of the symbolic matrix to a numeric value, they are converted to symbolic constants on the way in.