Superclasses
Robot
The various models ERobot models all subclass this class.
@author: Jesse Haviland @author: Peter Corke
- class roboticstoolbox.robot.Robot.Robot(arg, gripper_links=None, name='', manufacturer='', comment='', base=None, tool=None, gravity=[0, 0, -9.81], keywords=[], symbolic=False, configs=None, check_jindex=True, urdf_string=None, urdf_filepath=None)[source]
Bases:
BaseRobot
[Link
],RobotKinematicsMixin
- static URDF_read(file_path, tld=None, xacro_tld=None)[source]
Read a URDF file as Links
File should be specified relative to
RTBDATA/URDF/xacro
- Parameters:
file_path – File path relative to the xacro folder
tld – A custom top-level directory which holds the xacro data, defaults to None
xacro_tld – A custom top-level within the xacro data, defaults to None
- Return type:
- Returns:
links – a list of links
name – the name of the robot
urdf – a string representing the URDF
file_path – a path to the original file
Notes
If
tld
is not supplied, filepath pointing to xacro data should be directly underRTBDATA/URDF/xacro
OR under./xacro
relative to the model file calling this method. Iftld
is supplied, then`file_path`
needs to be relative totld
- property reach: float
Reach of the robot
A conservative estimate of the reach of the robot. It is computed as the sum of the translational ETs that define the link transform.
Note
Computed on the first access. If kinematic parameters subsequently change this will not be reflected.
- Returns:
Maximum reach of the robot
- Return type:
reach
Notes
Probably an overestimate of reach
Used by numerical inverse kinematics to scale translational error.
For a prismatic joint, uses
qlim
if it is set
- fkine_all(q)[source]
Compute the pose of every link frame
T = robot.fkine_all(q)
is an SE3 instance withrobot.nlinks + 1
values:T[0]
is the base transformT[i]
is the pose of link whosenumber
isi
- Parameters:
q (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – The joint configuration- Returns:
Pose of all links
- Return type:
fkine_all
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
- manipulability(q=None, J=None, end=None, start=None, method='yoshikawa', axes='all', **kwargs)[source]
Manipulability measure
manipulability(q)
is the scalar manipulability index for the robot at the joint configurationq
. It indicates dexterity, that is, how well conditioned the robot is for motion with respect to the 6 degrees of Cartesian motion. The values is zero if the robot is at a singularity.- Parameters:
q – Joint coordinates, one of J or q required
J – Jacobian in base frame if already computed, one of J or q required
method (
Literal
['yoshikawa'
,'asada'
,'minsingular'
,'invcondition'
]) – method to use, “yoshikawa” (default), “invcondition”, “minsingular” or “asada”axes (
Union
[Literal
['all'
,'trans'
,'rot'
],List
[bool
]]) – Task space axes to consider: “all” [default], “trans”, or “rot”
- Return type:
manipulability
Synopsis
Various measures are supported:
Measure | Description ||-------------------|————————————————-| |
"yoshikawa"
| Volume of the velocity ellipsoid, distance | | | from singularity [Yoshikawa85] | |"invcondition"``| Inverse condition number of Jacobian, isotropy | | | of the velocity ellipsoid [Klein87]_ | | ``"minsingular"
| Minimum singular value of the Jacobian, | | | distance from singularity [Klein87] | |"asada"
| Isotropy of the task-space acceleration | | | ellipsoid which is a function of the Cartesian | | | inertia matrix which depends on the inertial | | | parameters [Asada83] |Trajectory operation:
If
q
is a matrix (m,n) then the result (m,) is a vector of manipulability indices for each joint configuration specified by a row ofq
.Notes
Invokes the
jacob0
method of the robot ifJ
is not passed- The “all” option includes rotational and translational
dexterity, but this involves adding different units. It can be more useful to look at the translational and rotational manipulability separately.
- Examples in the RVC book (1st edition) can be replicated by
using the “all” option
- Asada’s measure requires inertial a robot model with inertial
parameters.
References
[Yoshikawa85]Manipulability of Robotic Mechanisms. Yoshikawa T., The International Journal of Robotics Research. 1985;4(2):3-9. doi:10.1177/027836498500400201
[Asada83]A geometrical representation of manipulator dynamics and its application to arm design, H. Asada, Journal of Dynamic Systems, Measurement, and Control, vol. 105, p. 131, 1983.
[Klein87]Dexterity Measures for the Design and Control of Kinematically Redundant Manipulators. Klein CA, Blaho BE. The International Journal of Robotics Research. 1987;6(2):72-83. doi:10.1177/027836498700600206
Robotics, Vision & Control, Chap 8, P. Corke, Springer 2011.
Changed in version 1.0.3: Removed ‘both’ option for axes, added a custom list option.
- jtraj(T1, T2, t, **kwargs)[source]
Joint-space trajectory between SE(3) poses
The initial and final poses are mapped to joint space using inverse kinematics:
if the object has an analytic solution
ikine_a
that will be used,otherwise the general numerical algorithm
ikine_lm
will be used.
traj = obot.jtraj(T1, T2, t)
is a trajectory object whose attributetraj.q
is a row-wise joint-space trajectory.
- jacob0_dot(q, qd, J0=None, representation=None)[source]
Derivative of Jacobian
robot.jacob_dot(q, qd)
computes the rate of change of the Jacobian elements\[\dmat{J} = \frac{d \mat{J}}{d \vec{q}} \frac{d \vec{q}}{dt}\]where the first term is the rank-3 Hessian.
- Parameters:
- Returns:
The derivative of the manipulator Jacobian
- Return type:
jdot
Synopsis
If
J0
is already calculated for the joint coordinatesq
it can be passed in to to save computation time.It is computed as the mode-3 product of the Hessian tensor and the velocity vector.
The derivative of an analytical Jacobian can be obtained by setting
representation
as|``representation`` | Rotational representation | |---------------------|————————————-| |
'rpy/xyz'
| RPY angular rates in XYZ order | |'rpy/zyx'
| RPY angular rates in XYZ order | |'eul'
| Euler angular rates in ZYZ order | |'exp'
| exponential coordinate rates |References
- Kinematic Derivatives using the Elementary Transform
Sequence, J. Haviland and P. Corke
See also
- jacobm(q=None, J=None, H=None, end=None, start=None, axes='all')[source]
The manipulability Jacobian
This measure relates the rate of change of the manipulability to the joint velocities of the robot. One of J or q is required. Supply J and H if already calculated to save computation time
- Parameters:
q – The joint angles/configuration of the robot (Optional, if not supplied will use the stored q values).
J – The manipulator Jacobian in any frame
H – The manipulator Hessian in any frame
end (
Union
[str
,Link
,Gripper
,None
]) – the final link or Gripper which the Hessian representsstart (
Union
[str
,Link
,Gripper
,None
]) – the first link which the Hessian represents
- Returns:
The manipulability Jacobian
- Return type:
jacobm
Synopsis
Yoshikawa’s manipulability measure
\[m(\vec{q}) = \sqrt{\mat{J}(\vec{q}) \mat{J}(\vec{q})^T}\]This method returns its Jacobian with respect to configuration
\[\frac{\partial m(\vec{q})}{\partial \vec{q}}\]References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- closest_point(q, shape, inf_dist=1.0, skip=False)[source]
Find the closest point between robot and shape
closest_point(shape, inf_dist)
returns the minimum euclidean distance between this robot and shape, provided it is less than inf_dist. It will also return the points on self and shape in the world frame which connect the line of length distance between the shapes. If the distance is negative then the shapes are collided.- shape
The shape to compare distance to
- inf_dist
The minimum distance within which to consider the shape
- skip
Skip setting all shape transforms based on q, use this option if using this method in conjuction with Swift to save time
- iscollided(q, shape, skip=False)[source]
Check if the robot is in collision with a shape
iscollided(shape)
checks if this robot and shape have collided- shape
The shape to compare distance to
- skip
Skip setting all shape transforms based on q, use this option if using this method in conjuction with Swift to save time
- Returns:
True if shapes have collided
- Return type:
iscollided
- collided(q, shape, skip=False)[source]
Check if the robot is in collision with a shape
collided(shape)
checks if this robot and shape have collided- shape
The shape to compare distance to
- skip
Skip setting all shape transforms based on q, use this option if using this method in conjuction with Swift to save time
- Returns:
True if shapes have collided
- Return type:
collided
- joint_velocity_damper(ps=0.05, pi=0.1, n=None, gain=1.0)[source]
Compute the joint velocity damper for QP motion control
Formulates an inequality contraint which, when optimised for will make it impossible for the robot to run into joint limits. Requires the joint limits of the robot to be specified. See examples/mmc.py for use case
- ps
The minimum angle (in radians) in which the joint is allowed to approach to its limit
- pi
The influence angle (in radians) in which the velocity damper becomes active
- n
The number of joints to consider. Defaults to all joints
- gain
The gain for the velocity damper
- link_collision_damper(shape, q, di=0.3, ds=0.05, xi=1.0, end=None, start=None, collision_list=None)[source]
Compute a collision constrain for QP motion control
Formulates an inequality contraint which, when optimised for will make it impossible for the robot to run into a collision. Requires See examples/neo.py for use case
- ds
The minimum distance in which a joint is allowed to approach the collision object shape
- di
The influence distance in which the velocity damper becomes active
- xi
The gain for the velocity damper
- end
The end link of the robot to consider
- start
The start link of the robot to consider
- collision_list
A list of shapes to consider for collision
- Returns:
Ain – A (6,) vector inequality contraint for an optisator
Bin – b (6,) vector inequality contraint for an optisator
- vision_collision_damper(shape, camera=None, camera_n=0, q=None, di=0.3, ds=0.05, xi=1.0, end=None, start=None, collision_list=None)[source]
Compute a vision collision constrain for QP motion control
Formulates an inequality contraint which, when optimised for will make it impossible for the robot to run into a line of sight. See examples/fetch_vision.py for use case
- camera
The camera link, either as a robotic link or SE3 pose
- camera_n
Degrees of freedom of the camera link
- ds
The minimum distance in which a joint is allowed to approach the collision object shape
- di
The influence distance in which the velocity damper becomes active
- xi
The gain for the velocity damper
- end
The end link of the robot to consider
- start
The start link of the robot to consider
- collision_list
A list of shapes to consider for collision
- Returns:
Ain – A (6,) vector inequality contraint for an optisator
Bin – b (6,) vector inequality contraint for an optisator
- rne(q, qd, qdd, symbolic=False, gravity=None)[source]
Compute inverse dynamics via recursive Newton-Euler formulation
rne_dh(q, qd, qdd)
where the arguments have shape (n,) where n is the number of robot joints. The result has shape (n,).rne_dh(q, qd, qdd)
where the arguments have shape (m,n) where n is the number of robot joints and where m is the number of steps in the joint trajectory. The result has shape (m,n).rne_dh(p)
where the input is a 1D arrayp
= [q, qd, qdd] with shape (3n,), and the result has shape (n,).rne_dh(p)
where the input is a 2D arrayp
= [q, qd, qdd] with shape (m,3n) and the result has shape (m,n).- Parameters:
- Returns:
Joint force/torques
- Return type:
tau
Notes
This version supports symbolic model parameters
Verified against MATLAB code
- __getitem__(i)
Get link
This also supports iterating over each link in the robot object, from the base to the tool.
- Parameters:
- Returns:
i’th link or named link
- Return type:
link
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> print(robot[1]) # print the 2nd link RevoluteDH: θ=q, d=0, a=0.4318, ⍺=0.0 >>> print([link.a for link in robot]) # print all the a_j values [0, 0.4318, 0.0203, 0, 0, 0]
Notes
Robot
supports link lookup by name,eg.
robot['link1']
- __str__()
Pretty prints the ETS Model of the robot.
- Returns:
Pretty print of the robot model
- Return type:
Notes
Constant links are shown in blue.
End-effector links are prefixed with an @
Angles in degrees
- The robot base frame is denoted as
BASE
and is equal to the robot’s
base
attribute.
- The robot base frame is denoted as
- accel(q, qd, torque, gravity=None)
Compute acceleration due to applied torque
qdd = accel(q, qd, torque)
calculates a vector (n) of joint accelerations that result from applying the actuator force/torque (n) to the manipulator in state q (n) and qd (n), andn
is the number of robot joints.\[\ddot{q} = \mathbf{M}^{-1} \left(\tau - \mathbf{C}(q)\dot{q} - \mathbf{g}(q)\right)\]Trajectory operation
If q, qd, torque are matrices (m,n) then
qdd
is a matrix (m,n) where each row is the acceleration corresponding to the equivalent rows of q, qd, torque.- Parameters:
q – Joint coordinates
qd – Joint velocity
torque – Joint torques of the robot
gravity – Gravitational acceleration (Optional, if not supplied will use the
gravity
attribute of self).
- Return type:
ndarray(n)
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.accel(puma.qz, 0.5 * np.ones(6), np.zeros(6)) array([ -7.5544, -12.22 , -6.4022, -5.4303, -4.9518, -2.1178])
Notes
- Useful for simulation of manipulator dynamics, in
conjunction with a numerical integration function.
- Uses the method 1 of Walker and Orin to compute the forward
dynamics.
- Featherstone’s method is more efficient for robots with large
numbers of joints.
Joint friction is considered.
References
- Efficient dynamic computer simulation of robotic mechanisms,
M. W. Walker and D. E. Orin, ASME Journa of Dynamic Systems, Measurement and Control, vol. 104, no. 3, pp. 205-211, 1982.
- accel_x(q, xd, wrench, gravity=None, pinv=False, representation='rpy/xyz')
Operational space acceleration due to applied wrench
xdd = accel_x(q, qd, wrench)
is the operational space acceleration due towrench
applied to the end-effector of a robot in joint configurationq
and joint velocityqd
.\[\ddot{x} = \mathbf{J}(q) \mathbf{M}(q)^{-1} \left( \mathbf{J}(q)^T w - \mathbf{C}(q)\dot{q} - \mathbf{g}(q) \right)\]Trajectory operation
If q, qd, torque are matrices (m,n) then
qdd
is a matrix (m,n) where each row is the acceleration corresponding to the equivalent rows of q, qd, wrench.- Parameters:
q – Joint coordinates
qd – Joint velocity
wrench – Wrench applied to the end-effector
gravity – Gravitational acceleration (Optional, if not supplied will use the
gravity
attribute of self).pinv – use pseudo inverse rather than inverse
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
xd –
representation – (Default value = “rpy/xyz”)
- Returns:
Operational space accelerations of the end-effector
- Return type:
accel
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
- Useful for simulation of manipulator dynamics, in
conjunction with a numerical integration function.
- Uses the method 1 of Walker and Orin to compute the forward
dynamics.
- Featherstone’s method is more efficient for robots with large
numbers of joints.
Joint friction is considered.
See also
- addconfiguration(name, q)
Add a named joint configuration
Add a named configuration to the robot instance’s dictionary of named configurations.
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.addconfiguration_attr("mypos", [0.1, 0.2, 0.3, 0.4, 0.5, 0.6]) >>> robot.configs["mypos"] array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6])
See also
- addconfiguration_attr(name, q, unit='rad')
Add a named joint configuration as an attribute
- Parameters:
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.addconfiguration_attr("mypos", [0.1, 0.2, 0.3, 0.4, 0.5, 0.6]) >>> robot.mypos array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6]) >>> robot.configs["mypos"] array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6])
Notes
Used in robot model init method to store the
qr
configuration- Dynamically adding attributes to objects can cause issues with
Python type checking.
- Configuration is also added to the robot instance’s dictionary of
named configurations.
See also
- attach(object)
- attach_to(object)
- property base: SE3
Get/set robot base transform
robot.base
is the robot base transformrobot.base = ...
checks and sets the robot base transform
- Parameters:
base – the new robot base transform
- Returns:
the current robot base transform
- Return type:
base
- property base_link: LinkType
Get the robot base link
robot.base_link
is the robot base link
- Returns:
the first link in the robot tree
- Return type:
base_link
- cinertia(q)
Deprecated, use
inertia_x
- property comment: str
Get/set robot comment
robot.comment
is the robot commentrobot.comment = ...
checks and sets the robot comment
- Parameters:
name – the new robot comment
- Returns:
robot comment
- Return type:
comment
- configurations_str(border='thin')
- property control_mode: str
Get/set robot control mode
robot.control_type
is the robot control moderobot.control_type = ...
checks and sets the robot control mode
- Parameters:
control_mode – the new robot control mode
- Returns:
the current robot control mode
- Return type:
control_mode
- copy()
- coriolis(q, qd)
Coriolis and centripetal term
coriolis(q, qd)
calculates the Coriolis/centripetal matrix (n,n) for the robot in configurationq
and velocityqd
, wheren
is the number of joints.The product \(\mathbf{C} \dot{q}\) is the vector of joint force/torque due to velocity coupling. The diagonal elements are due to centripetal effects and the off-diagonal elements are due to Coriolis effects. This matrix is also known as the velocity coupling matrix, since it describes the disturbance forces on any joint due to velocity of all other joints.
Trajectory operation
If
q
and qd are matrices (m,n), each row is interpretted as a joint configuration, and the result (n,n,m) is a 3d-matrix where each plane corresponds to a row ofq
andqd
.- Parameters:
q – Joint coordinates
qd – Joint velocity
- Returns:
Velocity matrix
- Return type:
coriolis
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.coriolis(puma.qz, 0.5 * np.ones((6,))) array([[-0.4017, -0.5513, -0.2025, -0.0007, -0.0013, 0. ], [ 0.2023, -0.1937, -0.3868, -0. , -0.002 , 0. ], [ 0.1987, 0.193 , -0. , 0. , -0.0001, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ], [ 0.0007, 0.0007, 0.0001, 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ]])
Notes
- Joint viscous friction is also a joint force proportional to
velocity but it is eliminated in the computation of this value.
Computationally slow, involves \(n^2/2\) invocations of RNE.
- coriolis_x(q, qd, pinv=False, representation='rpy/xyz', J=None, Ji=None, Jd=None, C=None, Mx=None)
Operational space Coriolis and centripetal term
coriolis_x(q, qd)
is the Coriolis/centripetal matrix (m,m) in operational space for the robot in configurationq
and velocityqd
, wheren
is the number of joints.\[\mathbf{C}_x = \mathbf{J}(q)^{-T} \left( \mathbf{C}(q) - \mathbf{M}_x(q) \mathbf{J})(q) \right) \mathbf{J}(q)^{-1}\]The product \(\mathbf{C} \dot{x}\) is the operational space wrench due to joint velocity coupling. This matrix is also known as the velocity coupling matrix, since it describes the disturbance forces on any joint due to velocity of all other joints.
The transformation to operational space requires an analytical, rather than geometric, Jacobian.
analytical
can be one of:Value
Rotational representation
'rpy/xyz'
RPY angular rates in XYZ order (default)
'rpy/zyx'
RPY angular rates in XYZ order
'eul'
Euler angular rates in ZYZ order
'exp'
exponential coordinate rates
Trajectory operation
If
q
and qd are matrices (m,n), each row is interpretted as a joint configuration, and the result (n,n,m) is a 3d-matrix where each plane corresponds to a row ofq
andqd
.- Parameters:
q – Joint coordinates
qd – Joint velocity
pinv – use pseudo inverse rather than inverse (Default value = False)
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
representation – (Default value = “rpy/xyz”)
J –
Ji –
Jd –
C –
Mx –
- Returns:
Operational space velocity matrix
- Return type:
ndarray(6,6) or ndarray(m,6,6)
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
- Joint viscous friction is also a joint force proportional to
velocity but it is eliminated in the computation of this value.
Computationally slow, involves \(n^2/2\) invocations of RNE.
If the robot is not 6 DOF the
pinv
option is set True.pinv()
is around 5x slower thaninv()
Warning
Assumes that the operational space has 6 DOF.
See also
- property default_backend
Get default graphical backend
robot.default_backend
Get the default graphical backend, used whenno explicit backend is passed to
Robot.plot
.
robot.default_backend = ...
Set the default graphical backend, used whenno explicit backend is passed to
Robot.plot
. The default set here will be overridden if the particularRobot
subclass cannot support it.
- Returns:
backend name
- Return type:
default_backend
- dfs_links(start, func=None)
A link search method
Visit all links from start in depth-first order and will apply func to each visited link
- dotfile(filename, etsbox=False, ets='full', jtype=False, static=True)
Write a link transform graph as a GraphViz dot file
- The file can be processed using dot:
% dot -Tpng -o out.png dotfile.dot
- The nodes are:
Base is shown as a grey square. This is the world frame origin, but can be changed using the
base
attribute of the robot.Link frames are indicated by circles
ETS transforms are indicated by rounded boxes
- The edges are:
an arrow if jtype is False or the joint is fixed
an arrow with a round head if jtype is True and the joint is revolute
an arrow with a box head if jtype is True and the joint is prismatic
Edge labels or nodes in blue have a fixed transformation to the preceding link.
Note
- If
filename
is a file object then the file will not be closed after the GraphViz model is written.
- Parameters:
file – Name of file to write to
etsbox (
bool
) – Put the link ETS in a box, otherwise an edge labelets (
Literal
['full'
,'brief'
]) – Display the full ets with “full” or a brief version with “brief”jtype (
bool
) – Arrowhead to node indicates revolute or prismatic typestatic (
bool
) – Show static joints in blue and bold
See also
- dynamics()
Pretty print the dynamic parameters (Robot superclass)
The dynamic parameters (inertial and friction) are printed in a table, with one row per link.
Examples
- dynamics_list()
Print dynamic parameters (Robot superclass)
Display the kinematic and dynamic parameters to the console in reable format
- dynchanged(what=None)
Dynamic parameters have changed
Called from a property setter to inform the robot that the cache of dynamic parameters is invalid.
See also
roboticstoolbox.Link._listen_dyn()
- ets(start=None, end=None)
Robot to ETS
robot.ets()
is an ETS representing the kinematics from base to end-effector.robot.ets(end=link)
is an ETS representing the kinematics from base to the linklink
specified as a Link reference or a name.robot.ets(start=l1, end=l2)
is an ETS representing the kinematics from linkl1
to linkl2
.:param : :type : param start: start of path, defaults to
base_link
:param : :type : param end: end of path, defaults to end-effector- Raises:
ValueError – a link does not belong to this ERobot
TypeError – a bad link argument
- Returns:
elementary transform sequence
- Return type:
ets
Examples
>>> import roboticstoolbox as rtb >>> panda = rtb.models.ETS.Panda() >>> panda.ets() [ET.tz(eta=0.333), ET.Rz(jindex=0), ET.Rx(eta=-1.5707963267948966), ET.Rz(jindex=1), ET.Rx(eta=1.5707963267948966), ET.tz(eta=0.316), ET.Rz(jindex=2), ET.tx(eta=0.0825), ET.Rx(eta=1.5707963267948966), ET.Rz(jindex=3), ET.tx(eta=-0.0825), ET.Rx(eta=-1.5707963267948966), ET.tz(eta=0.384), ET.Rz(jindex=4), ET.Rx(eta=1.5707963267948966), ET.Rz(jindex=5), ET.tx(eta=0.088), ET.Rx(eta=1.5707963267948966), ET.tz(eta=0.107), ET.Rz(jindex=6), ET.tz(eta=0.10300000000000001), ET.Rz(eta=-0.7853981633974483)]
- fdyn(T, q0, Q=None, Q_args={}, qd0=None, solver='RK45', solver_args={}, dt=None, progress=False)
Integrate forward dynamics
tg = R.fdyn(T, q)
integrates the dynamics of the robot with zero input torques over the time interval 0 toT
and returns the trajectory as a namedtuple with elements:t
the time vector (M,)q
the joint coordinates (M,n)qd
the joint velocities (M,n)
tg = R.fdyn(T, q, torqfun)
as above but the torque applied to the joints is given by the provided function:tau = function(robot, t, q, qd, **args)
where the inputs are:
the robot object
current time
current joint coordinates (n,)
current joint velocity (n,)
args, optional keyword arguments can be specified, these are
passed in from the
targs
kewyword argument.The function must return a Numpy array (n,) of joint forces/torques.
- Parameters:
T (
float
) – integration timeq0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – initial joint coordinatesqd0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – initial joint velocities, assumed zero if not givenQ (
Optional
[Callable
[[Any
,float
,ndarray
,ndarray
],ndarray
]]) – a function that computes generalized joint force as a function of time and/or stateQ_args (
Dict
) – positional arguments passed totorque
solver (
str
) – strsolver_args (
Dict
) – dictprogress (
bool
) – show progress bar, default False
- Returns:
robot trajectory
- Return type:
trajectory
Examples
To apply zero joint torque to the robot without Coulomb friction:
>>> def myfunc(robot, t, q, qd): >>> return np.zeros((robot.n,))
>>> tg = robot.nofriction().fdyn(5, q0, myfunc)
>>> plt.figure() >>> plt.plot(tg.t, tg.q) >>> plt.show()
We could also use a lambda function:
>>> tg = robot.nofriction().fdyn( >>> 5, q0, lambda r, t, q, qd: np.zeros((r.n,)))
The robot is controlled by a PD controller. We first define a function to compute the control which has additional parameters for the setpoint and control gains (qstar, P, D):
>>> def myfunc(robot, t, q, qd, qstar, P, D): >>> return (qstar - q) * P + qd * D # P, D are (6,)
>>> tg = robot.fdyn(10, q0, myfunc, torque_args=(qstar, P, D)) )
Many integrators have variable step length which is problematic if we want to animate the result. If
dt
is specified then the solver results are interpolated in time steps ofdt
.Notes
- This function performs poorly with non-linear joint friction,
such as Coulomb friction. The R.nofriction() method can be used to set this friction to zero.
- If the function is not specified then zero force/torque is
applied to the manipulator joints.
- Interpolation is performed using `ScipY integrate.ode
<https://docs.scipy.org/doc/scipy/reference/generated/scipy.integrate.ode.html>`
The SciPy RK45 integrator is used by default
- Interpolation is performed using `SciPy interp1
<https://docs.scipy.org/doc/scipy/reference/generated/scipy.interpolate.interp1d.html>`
See also
DHRobot.accel()
,DHRobot.nofriction()
,DHRobot.rne()
- fellipse(q, opt='trans', unit='rad', centre=[0, 0, 0])
Create a force ellipsoid object for plotting with PyPlot
robot.fellipse(q)
creates a force ellipsoid for the robot at poseq
. The ellipsoid is centered at the origin.- q
The joint configuration of the robot.
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational force ellipsoid
- unit
‘rad’ or ‘deg’ will plot the ellipsoid in radians or degrees
- centre
The centre of the ellipsoid, either ‘ee’ for the end-effector or a 3-vector [x, y, z] in the world frame
- Returns:
An EllipsePlot object
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- fkine(q, end=None, start=None, tool=None, include_base=True)
Forward kinematics
T = robot.fkine(q)
evaluates forward kinematics for the robot at joint configurationq
.Trajectory operation: If
q
has multiple rows (mxn), it is considered a trajectory and the result is anSE3
instance withm
values.- q
Joint coordinates
- end
end-effector or gripper to compute forward kinematics to
- start
the link to compute forward kinematics from
- tool
tool transform, optional
- Return type:
SE3
- Returns:
The transformation matrix representing the pose of the end-effector
Examples
The following example makes a
panda
robot object, and solves for the forward kinematics at the listed configuration.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) SE3(array([[ 0.995 , -0. , 0.0998, 0.484 ], [-0. , -1. , 0. , 0. ], [ 0.0998, -0. , -0.995 , 0.4126], [ 0. , 0. , 0. , 1. ]]))
Notes
- For a robot with a single end-effector there is no need to
specify
end
- For a robot with multiple end-effectors, the
end
must be specified.
- For a robot with multiple end-effectors, the
- The robot’s base tool transform, if set, is incorporated
into the result.
A tool transform, if provided, is incorporated into the result.
Works from the end-effector link to the base
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- friction(qd)
Manipulator joint friction (Robot superclass)
robot.friction(qd)
is a vector of joint friction forces/torques for the robot moving with joint velocitiesqd
.The friction model includes:
Viscous friction which is a linear function of velocity.
Coulomb friction which is proportional to sign(qd).
\[\begin{split}\tau_j = G^2 B \dot{q}_j + |G_j| \left\{ \begin{array}{ll} \tau_{C,j}^+ & \mbox{if $\dot{q}_j > 0$} \\ \tau_{C,j}^- & \mbox{if $\dot{q}_j < 0$} \end{array} \right.\end{split}\]- Parameters:
qd (
ndarray
) – The joint velocities of the robot- Returns:
The joint friction forces/torques for the robot
- Return type:
friction
Notes
- The friction value should be added to the motor output torque to
determine the nett torque. It has a negative value when qd > 0.
- The returned friction value is referred to the output of the
gearbox.
- The friction parameters in the Link object are referred to the
motor.
Motor viscous friction is scaled up by \(G^2\).
Motor Coulomb friction is scaled up by math:G.
- The appropriate Coulomb friction value to use in the
non-symmetric case depends on the sign of the joint velocity, not the motor velocity.
- Coulomb friction is zero for zero joint velocity, stiction is
not modeled.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 robot has negative gear ratio for joints 1 and 3.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 has negative gear ratio for joints 1 and 3.
See also
Robot.nofriction()
,Link.friction()
- get_path(end=None, start=None)
Find a path from start to end
- Parameters:
- Raises:
ValueError – link not known or ambiguous
- Return type:
- Returns:
path – the path from start to end
n – the number of joints in the path
T – the tool transform present after end
- property gravity: ndarray
Get/set default gravitational acceleration (Robot superclass)
robot.name
is the default gravitational accelerationrobot.name = ...
checks and sets default gravitationalacceleration
- Parameters:
gravity – the new gravitational acceleration for this robot
- Returns:
gravitational acceleration
- Return type:
gravity
Notes
If the z-axis is upward, out of the Earth, this should be a positive number.
- gravload(q=None, gravity=None)
Compute gravity load
robot.gravload(q)
calculates the joint gravity loading (n) for the robot in the joint configurationq
and using the default gravitational acceleration specified in the DHRobot object.robot.gravload(q, gravity=g)
as above except the gravitational acceleration is explicitly specified asg
.Trajectory operation
If q is a matrix (nxm) each column is interpreted as a joint configuration vector, and the result is a matrix (nxm) each column being the corresponding joint torques.
- Parameters:
- Returns:
The generalised joint force/torques due to gravity
- Return type:
gravload
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.gravload(puma.qz) array([ 0. , 37.4837, 0.2489, 0. , 0. , 0. ])
- gravload_x(q=None, gravity=None, pinv=False, representation='rpy/xyz', Ji=None)
Operational space gravity load
robot.gravload_x(q)
calculates the gravity wrench for the robot in the joint configurationq
and using the default gravitational acceleration specified in the robot object.robot.gravload_x(q, gravity=g)
as above except the gravitational acceleration is explicitly specified asg
.\[\mathbf{G}_x = \mathbf{J}(q)^{-T} \mathbf{G}(q)\]The transformation to operational space requires an analytical, rather than geometric, Jacobian.
analytical
can be one of:Value
Rotational representation
'rpy/xyz'
RPY angular rates in XYZ order (default)
'rpy/zyx'
RPY angular rates in XYZ order
'eul'
Euler angular rates in ZYZ order
'exp'
exponential coordinate rates
Trajectory operation
If q is a matrix (nxm) each column is interpreted as a joint configuration vector, and the result is a matrix (nxm) each column being the corresponding joint torques.
- Parameters:
q – Joint coordinates
gravity – Gravitational acceleration (Optional, if not supplied will use the
gravity
attribute of self).pinv – use pseudo inverse rather than inverse (Default value = False)
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
representation – (Default value = “rpy/xyz”)
Ji –
- Returns:
The operational space gravity wrench
- Return type:
gravload
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
If the robot is not 6 DOF the
pinv
option is set True.pinv()
is around 5x slower thaninv()
Warning
Assumes that the operational space has 6 DOF.
See also
- property grippers: List[Gripper]
Grippers attached to the robot
- Returns:
A list of grippers
- Return type:
grippers
- property hascollision
Robot has collision model
- Returns:
hascollision – Robot has collision model
At least one link has associated collision model.
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.hascollision False
See also
- property hasdynamics
Robot has dynamic parameters
- Returns:
hasdynamics – Robot has dynamic parameters
At least one link has associated dynamic parameters.
Examples
- property hasgeometry
Robot has geometry model
At least one link has associated mesh to describe its shape.
- Returns:
Robot has geometry model
- Return type:
hasgeometry
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.hasgeometry True
See also
- hessian0(q=None, end=None, start=None, J0=None, tool=None)
Manipulator Hessian
The manipulator Hessian tensor maps joint acceleration to end-effector spatial acceleration, expressed in the
start
frame. This function calulcates this based on the ETS of the robot. One of J0 or q is required. Supply J0 if already calculated to save computation time- Parameters:
q – The joint angles/configuration of the robot (Optional, if not supplied will use the stored q values).
end (
Union
[str
,Link
,Gripper
,None
]) – the final link/Gripper which the Hessian representsstart (
Union
[str
,Link
,Gripper
,None
]) – the first link which the Hessian representsJ0 – The manipulator Jacobian in the
start
frametool (
Union
[ndarray
,SE3
,None
]) – a static tool transformation matrix to apply to the end of end, defaults to None
- Returns:
The manipulator Hessian in the
start
frame- Return type:
h0
Synopsis
This method computes the manipulator Hessian in the
start
frame. If we take the time derivative of the differential kinematic relationship .. math:\nu &= \mat{J}(\vec{q}) \dvec{q} \\ \alpha &= \dmat{J} \dvec{q} + \mat{J} \ddvec{q}
where .. math:
\dmat{J} = \mat{H} \dvec{q}
and \(\mat{H} \in \mathbb{R}^{6\times n \times n}\) is the Hessian tensor.
The elements of the Hessian are .. math:
\mat{H}_{i,j,k} = \frac{d^2 u_i}{d q_j d q_k}
where \(u = \{t_x, t_y, t_z, r_x, r_y, r_z\}\) are the elements of the spatial velocity vector.
Similarly, we can write .. math:
\mat{J}_{i,j} = \frac{d u_i}{d q_j}
Examples
The following example makes a
Panda
robot object, and solves for the base frame Hessian at the given joint angle configuration>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> panda.hessian0([0, -0.3, 0, -2.2, 0, 2, 0.7854]) array([[[-0.484 , -0. , -0.486 , -0. , -0.1547, 0. , -0. ], [ 0. , 0.0796, 0. , 0.2466, 0. , 0.2006, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , -1. , -0. , 1. , 0. , 1. , 0. ], [ 0. , -0. , -0.2955, -0. , 0.9463, -0. , 0.0998], [ 0. , 0. , -0. , -0. , 0. , -0. , 0. ]], [[-0. , -0.484 , -0. , 0.4986, -0. , 0.1086, 0. ], [ 0.0796, 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , -0.0796, -0. , -0.2466, -0. , -0.2006, -0. ], [ 0. , 0. , 0.9553, 0. , -0.3233, 0. , -0.995 ], [ 0. , 0. , -0. , -0. , 0. , -0. , 0. ], [ 0. , 0. , 0.2955, 0. , -0.9463, 0. , -0.0998]], [[-0.486 , -0. , -0.4643, -0. , -0.1478, 0. , 0. ], [ 0. , 0. , 0. , 0.383 , 0. , 0.2237, 0. ], [ 0. , -0. , -0.1436, -0. , -0.0457, -0. , -0. ], [ 0. , 0. , 0. , 0.9553, 0. , 0.9553, 0. ], [ 0. , 0. , 0. , -0. , 0.8085, -0. , -0.1987], [ 0. , 0. , 0. , 0.2955, 0. , 0.2955, 0. ]], [[-0. , 0.4986, -0. , -0.4986, 0. , -0.1086, -0. ], [ 0.2466, 0. , 0.383 , 0. , 0. , 0. , 0. ], [ 0. , -0.2466, -0. , 0.2466, 0. , 0.2006, 0. ], [ 0. , 0. , 0. , 0. , 0.3233, 0. , 0.995 ], [ 0. , 0. , 0. , 0. , 0. , 0. , -0. ], [ 0. , 0. , 0. , 0. , 0.9463, 0. , 0.0998]], [[-0.1547, -0. , -0.1478, 0. , 0.05 , -0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , -0.1676, -0. ], [ 0. , -0. , -0.0457, 0. , 0.1464, 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , -0.3233, 0. ], [ 0. , 0. , 0. , 0. , 0. , -0. , 0.9093], [ 0. , 0. , 0. , 0. , 0. , -0.9463, -0. ]], [[ 0. , 0.1086, 0. , -0.1086, -0. , -0.1086, -0. ], [ 0.2006, 0. , 0.2237, 0. , -0.1676, 0. , 0. ], [ 0. , -0.2006, -0. , 0.2006, 0. , 0.2006, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0.995 ], [ 0. , 0. , 0. , 0. , 0. , 0. , -0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0.0998]], [[-0. , 0. , 0. , -0. , 0. , -0. , 0. ], [ 0. , 0. , 0. , 0. , -0. , 0. , -0. ], [ 0. , -0. , -0. , 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ]]])
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- hessiane(q=None, end=None, start=None, Je=None, tool=None)
Manipulator Hessian
The manipulator Hessian tensor maps joint acceleration to end-effector spatial acceleration, expressed in the
end
coordinate frame. This function calulcates this based on the ETS of the robot. One of J0 or q is required. Supply J0 if already calculated to save computation time- Parameters:
q – The joint angles/configuration of the robot (Optional, if not supplied will use the stored q values).
end (
Union
[str
,Link
,Gripper
,None
]) – the final link/Gripper which the Hessian representsstart (
Union
[str
,Link
,Gripper
,None
]) – the first link which the Hessian representsJ0 – The manipulator Jacobian in the
end
frametool (
Union
[ndarray
,SE3
,None
]) – a static tool transformation matrix to apply to the end of end, defaults to None
- Returns:
The manipulator Hessian in
end
frame- Return type:
he
Synopsis
This method computes the manipulator Hessian in the
end
frame. If we take the time derivative of the differential kinematic relationship .. math:\nu &= \mat{J}(\vec{q}) \dvec{q} \\ \alpha &= \dmat{J} \dvec{q} + \mat{J} \ddvec{q}
where .. math:
\dmat{J} = \mat{H} \dvec{q}
and \(\mat{H} \in \mathbb{R}^{6\times n \times n}\) is the Hessian tensor.
The elements of the Hessian are .. math:
\mat{H}_{i,j,k} = \frac{d^2 u_i}{d q_j d q_k}
where \(u = \{t_x, t_y, t_z, r_x, r_y, r_z\}\) are the elements of the spatial velocity vector.
Similarly, we can write .. math:
\mat{J}_{i,j} = \frac{d u_i}{d q_j}
Examples
The following example makes a
Panda
robot object, and solves for the end-effector frame Hessian at the given joint angle configuration>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> panda.hessiane([0, -0.3, 0, -2.2, 0, 2, 0.7854]) array([[[-0.4816, -0. , -0.4835, -0. , -0.1539, -0. , 0. ], [ 0. , -0.0796, 0. , -0.2466, 0. , -0.2006, 0. ], [-0.0483, -0. , -0.0485, -0. , -0.0154, -0. , 0. ], [ 0. , -0.995 , 0. , 0.995 , -0. , 0.995 , -0. ], [ 0. , 0. , 0.2955, -0. , -0.9463, -0. , -0.0998], [ 0. , -0.0998, 0. , 0.0998, -0. , 0.0998, 0. ]], [[-0. , -0.4896, -0. , 0.4715, -0. , 0.088 , 0. ], [-0.0796, 0. , 0. , -0. , 0. , -0. , 0. ], [-0. , 0.0309, 0. , 0.2952, 0. , 0.2104, -0. ], [ 0. , 0. , 0.9801, 0. , -0.4161, 0. , -1. ], [ 0. , 0. , -0. , -0. , 0. , -0. , 0. ], [ 0. , 0. , -0.1987, -0. , 0.9093, -0. , 0. ]], [[-0.4835, -0. , -0.4763, -0. , -0.1516, -0. , 0. ], [ 0. , 0. , 0. , -0.383 , 0. , -0.2237, 0. ], [-0.0485, 0. , 0.0965, -0. , 0.0307, -0. , 0. ], [ 0. , 0. , 0. , 0.9801, -0. , 0.9801, 0. ], [ 0. , 0. , 0. , -0. , -0.8085, -0. , 0.1987], [ 0. , 0. , 0. , -0.1987, -0. , -0.1987, -0. ]], [[-0. , 0.4715, -0. , -0.4715, 0. , -0.088 , 0. ], [-0.2466, -0. , -0.383 , 0. , -0. , 0. , -0. ], [-0. , 0.2952, -0. , -0.2952, -0. , -0.2104, 0. ], [ 0. , 0. , 0. , 0. , 0.4161, 0. , 1. ], [ 0. , 0. , 0. , 0. , -0. , 0. , -0. ], [ 0. , 0. , 0. , 0. , -0.9093, 0. , 0. ]], [[-0.1539, -0. , -0.1516, 0. , 0.0644, 0. , -0. ], [ 0. , 0. , 0. , -0. , -0. , 0.1676, -0. ], [-0.0154, 0. , 0.0307, -0. , -0.1407, -0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , -0.4161, -0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , -0.9093], [ 0. , 0. , 0. , 0. , 0. , 0.9093, 0. ]], [[-0. , 0.088 , -0. , -0.088 , 0. , -0.088 , 0. ], [-0.2006, -0. , -0.2237, 0. , 0.1676, 0. , -0. ], [-0. , 0.2104, -0. , -0.2104, -0. , -0.2104, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 1. ], [ 0. , 0. , 0. , 0. , 0. , 0. , -0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ]], [[ 0. , 0. , 0. , 0. , -0. , 0. , 0. ], [ 0. , 0. , 0. , -0. , -0. , -0. , -0. ], [ 0. , -0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. , 0. ]]])
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- hierarchy()
Pretty print the robot link hierachy
- Return type:
Pretty print of the robot model
Examples
Makes a robot and prints the heirachy
>>> import roboticstoolbox as rtb >>> robot = rtb.models.URDF.Panda() >>> robot.hierarchy() panda_link0 panda_link1 panda_link2 panda_link3 panda_link4 panda_link5 panda_link6 panda_link7 panda_link8 panda_hand panda_leftfinger panda_rightfinger
- ik_GN(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, pinv=True, pinv_damping=0.0)
Fast numerical inverse kinematics by Gauss-Newton optimization
sol = ets.ik_GN(Tep)
are the joint coordinates (n) corresponding to the robot end-effector poseTep
which is anSE3
orndarray
object. This method can be used for robots with any number of degrees of freedom. This is a fast solver implemented in C++.See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
Note
When using this method with redundant robots (>6 DoF),
pinv
must be set toTrue
- Parameters:
Tep (
Union
[ndarray
,SE3
]) – The desired end-effector pose or pose trajectoryend (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Optional
[ndarray
]) – initial joint configuration (default to random valid joint configuration contrained by the joint limits of the robot)ilimit (
int
) – maximum number of iterations per searchslimit (
int
) – maximum number of search attemptstol (
float
) – final error tolerancemask (
Optional
[ndarray
]) – a mask vector which weights the end-effector error priority. Corresponds to translation in X, Y and Z and rotation about X, Y and Z respectivelyjoint_limits (
bool
) – constrain the solution to being within the joint limits of the robot (reject solution with invalid joint configurations and perfrom another search up to the slimit)pinv (
int
) – Use the psuedo-inverse instad of the normal matrix inversepinv_damping (
float
) – Damping factor for the psuedo-inverse
- Return type:
- Returns:
sol – tuple (q, success, iterations, searches, residual)
The return value
sol
is a tuple with elements============ ========== ===============================================
Element Type Description
============ ========== ===============================================
q
ndarray(n) joint coordinates in units of radians or metressuccess
int whether a solution was founditerations
int total number of iterationssearches
int total number of searchesresidual
float final value of cost function============ ========== ===============================================
If
success == 0
theq
values will be valid numbers, but thesolution will be in error. The amount of error is indicated by
the
residual
.
Synopsis
Each iteration uses the Gauss-Newton optimisation method
\[\begin{split}\vec{q}_{k+1} &= \vec{q}_k + \left( {\mat{J}(\vec{q}_k)}^\top \mat{W}_e \ {\mat{J}(\vec{q}_k)} \right)^{-1} \bf{g}_k \\ \bf{g}_k &= {\mat{J}(\vec{q}_k)}^\top \mat{W}_e \vec{e}_k\end{split}\]where \(\mat{J} = {^0\mat{J}}\) is the base-frame manipulator Jacobian. If \(\mat{J}(\vec{q}_k)\) is non-singular, and \(\mat{W}_e = \mat{1}_n\), then the above provides the pseudoinverse solution. However, if \(\mat{J}(\vec{q}_k)\) is singular, the above can not be computed and the GN solution is infeasible.
Examples
The following example gets a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_GN method.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> Tep = panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) >>> panda.ik_GN(Tep) (array([-1.0805, -0.5328, 0.9086, -2.1781, 0.4612, 1.9018, 0.4239]), 1, 510, 32, 2.803306327008683e-09)
Notes
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- ik_LM(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, k=1.0, method='chan')
Fast levenberg-Marquadt Numerical Inverse Kinematics Solver
A method which provides functionality to perform numerical inverse kinematics (IK) using the Levemberg-Marquadt method. This is a fast solver implemented in C++.
See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
- Parameters:
end (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Optional
[ndarray
]) – The initial joint coordinate vectorilimit (
int
) – How many iterations are allowed within a search before a new search is startedslimit (
int
) – How many searches are allowed before being deemed unsuccessfultol (
float
) – Maximum allowed residual error Emask (
Optional
[ndarray
]) – A 6 vector which assigns weights to Cartesian degrees-of-freedom error priorityjoint_limits (
bool
) – Reject solutions with joint limit violationsseed – A seed for the private RNG used to generate random joint coordinate vectors
k (
float
) – Sets the gain value for the damping matrix Wn in the next iteration. See synopsismethod (
Literal
['chan'
,'wampler'
,'sugihara'
]) – One of “chan”, “sugihara” or “wampler”. Defines which method is used to calculate the damping matrix Wn in thestep
method
- Return type:
Synopsis
The operation is defined by the choice of the
method
kwarg.The step is deined as
\[\begin{split}\vec{q}_{k+1} &= \vec{q}_k + \left( \mat{A}_k \right)^{-1} \bf{g}_k \\ % \mat{A}_k &= {\mat{J}(\vec{q}_k)}^\top \mat{W}_e \ {\mat{J}(\vec{q}_k)} + \mat{W}_n\end{split}\]where \(\mat{W}_n = \text{diag}(\vec{w_n})(\vec{w_n} \in \mathbb{R}^n_{>0})\) is a diagonal damping matrix. The damping matrix ensures that \(\mat{A}_k\) is non-singular and positive definite. The performance of the LM method largely depends on the choice of \(\mat{W}_n\).
Chan’s Method
Chan proposed
\[\mat{W}_n = λ E_k \mat{1}_n\]where λ is a constant which reportedly does not have much influence on performance. Use the kwarg k to adjust the weighting term λ.
Sugihara’s Method
Sugihara proposed
\[\mat{W}_n = E_k \mat{1}_n + \text{diag}(\hat{\vec{w}}_n)\]where \(\hat{\vec{w}}_n \in \mathbb{R}^n\), \(\hat{w}_{n_i} = l^2 \sim 0.01 l^2\), and \(l\) is the length of a typical link within the manipulator. We provide the variable k as a kwarg to adjust the value of \(w_n\).
Wampler’s Method
Wampler proposed \(\vec{w_n}\) to be a constant. This is set through the k kwarg.
Examples
The following example makes a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_LM method.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> Tep = panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) >>> panda.ikine_LM(Tep) IKSolution(q=array([-0.3834, -0.3202, 0.3427, -2.1984, 0.1219, 1.9934, 0.6892]), success=True, iterations=27, searches=2, residual=3.829062192451652e-09, reason='Success')
Notes
The value for the
k
kwarg will depend on themethod
chosen and the arm you are using. Use the following as a rough guidechan, k = 1.0 - 0.01
,wampler, k = 0.01 - 0.0001
, andsugihara, k = 0.1 - 0.0001
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
This class supports null-space motion to assist with maximising manipulability and avoiding joint limits. These are enabled by setting kq and km to non-zero values.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
See also
Changed in version 1.0.4: Merged the Levemberg-Marquadt IK solvers into the ik_LM method
- ik_NR(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, pinv=True, pinv_damping=0.0)
Fast numerical inverse kinematics using Newton-Raphson optimization
sol = ets.ik_NR(Tep)
are the joint coordinates (n) corresponding to the robot end-effector poseTep
which is anSE3
orndarray
object. This method can be used for robots with any number of degrees of freedom. This is a fast solver implemented in C++.See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
Note
When using this method with redundant robots (>6 DoF),
pinv
must be set toTrue
- Parameters:
Tep (
Union
[ndarray
,SE3
]) – The desired end-effector pose or pose trajectoryend (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Optional
[ndarray
]) – initial joint configuration (default to random valid joint configuration contrained by the joint limits of the robot)ilimit (
int
) – maximum number of iterations per searchslimit (
int
) – maximum number of search attemptstol (
float
) – final error tolerancemask (
Optional
[ndarray
]) – a mask vector which weights the end-effector error priority. Corresponds to translation in X, Y and Z and rotation about X, Y and Z respectivelyjoint_limits (
bool
) – constrain the solution to being within the joint limits of the robot (reject solution with invalid joint configurations and perfrom another search up to the slimit)pinv (
int
) – Use the psuedo-inverse instad of the normal matrix inversepinv_damping (
float
) – Damping factor for the psuedo-inverse
- Return type:
- Returns:
sol – tuple (q, success, iterations, searches, residual)
The return value
sol
is a tuple with elements============ ========== ===============================================
Element Type Description
============ ========== ===============================================
q
ndarray(n) joint coordinates in units of radians or metressuccess
int whether a solution was founditerations
int total number of iterationssearches
int total number of searchesresidual
float final value of cost function============ ========== ===============================================
If
success == 0
theq
values will be valid numbers, but thesolution will be in error. The amount of error is indicated by
the
residual
.
Synopsis
Each iteration uses the Newton-Raphson optimisation method
\[\vec{q}_{k+1} = \vec{q}_k + {^0\mat{J}(\vec{q}_k)}^{-1} \vec{e}_k\]Examples
The following example gets a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_GN method.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> Tep = panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) >>> panda.ik_NR(Tep) (array([-1.0805, -0.5328, 0.9086, -2.1781, 0.4612, 1.9018, 0.4239]), 1, 489, 32, 2.8033063270234757e-09)
Notes
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- ikine_GN(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, seed=None, pinv=False, kq=0.0, km=0.0, ps=0.0, pi=0.3, **kwargs)
Gauss-Newton Numerical Inverse Kinematics Solver
A method which provides functionality to perform numerical inverse kinematics (IK) using the Gauss-Newton method.
See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
Note
When using this method with redundant robots (>6 DoF),
pinv
must be set toTrue
- Parameters:
end (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – The initial joint coordinate vectorilimit (
int
) – How many iterations are allowed within a search before a new search is startedslimit (
int
) – How many searches are allowed before being deemed unsuccessfultol (
float
) – Maximum allowed residual error Emask (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – A 6 vector which assigns weights to Cartesian degrees-of-freedom error priorityjoint_limits (
bool
) – Reject solutions with joint limit violationsseed (
Optional
[int
]) – A seed for the private RNG used to generate random joint coordinate vectorspinv (
bool
) – If True, will use the psuedoinverse in the step method instead of the normal inversekq (
float
) – The gain for joint limit avoidance. Setting to 0.0 will remove this completely from the solutionkm (
float
) – The gain for maximisation. Setting to 0.0 will remove this completely from the solutionps (
float
) – The minimum angle/distance (in radians or metres) in which the joint is allowed to approach to its limitpi (
Union
[ndarray
,float
]) – The influence angle/distance (in radians or metres) in null space motion becomes active
Synopsis
Each iteration uses the Gauss-Newton optimisation method
\[\begin{split}\vec{q}_{k+1} &= \vec{q}_k + \left( {\mat{J}(\vec{q}_k)}^\top \mat{W}_e \ {\mat{J}(\vec{q}_k)} \right)^{-1} \bf{g}_k \\ \bf{g}_k &= {\mat{J}(\vec{q}_k)}^\top \mat{W}_e \vec{e}_k\end{split}\]where \(\mat{J} = {^0\mat{J}}\) is the base-frame manipulator Jacobian. If \(\mat{J}(\vec{q}_k)\) is non-singular, and \(\mat{W}_e = \mat{1}_n\), then the above provides the pseudoinverse solution. However, if \(\mat{J}(\vec{q}_k)\) is singular, the above can not be computed and the GN solution is infeasible.
Examples
The following example gets a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_GN method.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> Tep = panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) >>> panda.ikine_GN(Tep) IKSolution(q=array([ 2.0377, -0.5789, -1.7111, -2.1663, -0.9973, 1.8724, 2.0736]), success=False, iterations=100, searches=100, residual=0.0, reason='iteration and search limit reached, 100 numpy.LinAlgError encountered')
Notes
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
This class supports null-space motion to assist with maximising manipulability and avoiding joint limits. These are enabled by setting kq and km to non-zero values.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
See also
Changed in version 1.0.4: Added the Gauss-Newton IK solver method on the Robot class
- ikine_LM(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, seed=None, k=1.0, method='chan', kq=0.0, km=0.0, ps=0.0, pi=0.3, **kwargs)
Levenberg-Marquadt Numerical Inverse Kinematics Solver
A method which provides functionality to perform numerical inverse kinematics (IK) using the Levemberg-Marquadt method.
See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
- Parameters:
end (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – The initial joint coordinate vectorilimit (
int
) – How many iterations are allowed within a search before a new search is startedslimit (
int
) – How many searches are allowed before being deemed unsuccessfultol (
float
) – Maximum allowed residual error Emask (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – A 6 vector which assigns weights to Cartesian degrees-of-freedom error priorityjoint_limits (
bool
) – Reject solutions with joint limit violationsseed (
Optional
[int
]) – A seed for the private RNG used to generate random joint coordinate vectorsk (
float
) – Sets the gain value for the damping matrix Wn in the next iteration. See synopsismethod (
Literal
['chan'
,'wampler'
,'sugihara'
]) – One of “chan”, “sugihara” or “wampler”. Defines which method is used to calculate the damping matrix Wn in thestep
methodkq (
float
) – The gain for joint limit avoidance. Setting to 0.0 will remove this completely from the solutionkm (
float
) – The gain for maximisation. Setting to 0.0 will remove this completely from the solutionps (
float
) – The minimum angle/distance (in radians or metres) in which the joint is allowed to approach to its limitpi (
Union
[ndarray
,float
]) – The influence angle/distance (in radians or metres) in null space motion becomes active
Synopsis
The operation is defined by the choice of the
method
kwarg.The step is deined as
\[\begin{split}\vec{q}_{k+1} &= \vec{q}_k + \left( \mat{A}_k \right)^{-1} \bf{g}_k \\ % \mat{A}_k &= {\mat{J}(\vec{q}_k)}^\top \mat{W}_e \ {\mat{J}(\vec{q}_k)} + \mat{W}_n\end{split}\]where \(\mat{W}_n = \text{diag}(\vec{w_n})(\vec{w_n} \in \mathbb{R}^n_{>0})\) is a diagonal damping matrix. The damping matrix ensures that \(\mat{A}_k\) is non-singular and positive definite. The performance of the LM method largely depends on the choice of \(\mat{W}_n\).
Chan’s Method
Chan proposed
\[\mat{W}_n = λ E_k \mat{1}_n\]where λ is a constant which reportedly does not have much influence on performance. Use the kwarg k to adjust the weighting term λ.
Sugihara’s Method
Sugihara proposed
\[\mat{W}_n = E_k \mat{1}_n + \text{diag}(\hat{\vec{w}}_n)\]where \(\hat{\vec{w}}_n \in \mathbb{R}^n\), \(\hat{w}_{n_i} = l^2 \sim 0.01 l^2\), and \(l\) is the length of a typical link within the manipulator. We provide the variable k as a kwarg to adjust the value of \(w_n\).
Wampler’s Method
Wampler proposed \(\vec{w_n}\) to be a constant. This is set through the k kwarg.
Examples
The following example makes a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_LM method.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> Tep = panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) >>> panda.ikine_LM(Tep) IKSolution(q=array([ 0.076 , -0.3008, -0.0683, -2.1999, -0.0233, 1.9998, 0.8038]), success=True, iterations=31, searches=2, residual=6.103979291931972e-11, reason='Success')
Notes
The value for the
k
kwarg will depend on themethod
chosen and the arm you are using. Use the following as a rough guidechan, k = 1.0 - 0.01
,wampler, k = 0.01 - 0.0001
, andsugihara, k = 0.1 - 0.0001
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
This class supports null-space motion to assist with maximising manipulability and avoiding joint limits. These are enabled by setting kq and km to non-zero values.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
See also
Changed in version 1.0.4: Added the Levemberg-Marquadt IK solver method on the Robot class
- ikine_NR(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, seed=None, pinv=False, kq=0.0, km=0.0, ps=0.0, pi=0.3, **kwargs)
Newton-Raphson Numerical Inverse Kinematics Solver
A method which provides functionality to perform numerical inverse kinematics (IK) using the Newton-Raphson method.
See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
Note
When using this method with redundant robots (>6 DoF),
pinv
must be set toTrue
- Parameters:
end (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – The initial joint coordinate vectorilimit (
int
) – How many iterations are allowed within a search before a new search is startedslimit (
int
) – How many searches are allowed before being deemed unsuccessfultol (
float
) – Maximum allowed residual error Emask (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – A 6 vector which assigns weights to Cartesian degrees-of-freedom error priorityjoint_limits (
bool
) – Reject solutions with joint limit violationsseed (
Optional
[int
]) – A seed for the private RNG used to generate random joint coordinate vectorspinv (
bool
) – If True, will use the psuedoinverse in the step method instead of the normal inversekq (
float
) – The gain for joint limit avoidance. Setting to 0.0 will remove this completely from the solutionkm (
float
) – The gain for maximisation. Setting to 0.0 will remove this completely from the solutionps (
float
) – The minimum angle/distance (in radians or metres) in which the joint is allowed to approach to its limitpi (
Union
[ndarray
,float
]) – The influence angle/distance (in radians or metres) in null space motion becomes active
Synopsis
Each iteration uses the Newton-Raphson optimisation method
\[\vec{q}_{k+1} = \vec{q}_k + {^0\mat{J}(\vec{q}_k)}^{-1} \vec{e}_k\]Examples
The following example gets a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_NR method.>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> Tep = panda.fkine([0, -0.3, 0, -2.2, 0, 2, 0.7854]) >>> panda.ikine_NR(Tep) IKSolution(q=array([-0.9478, -1.036 , -0.5051, -2.1583, -0.0992, 1.8519, 0.0562]), success=False, iterations=100, searches=100, residual=0.0, reason='iteration and search limit reached, 100 numpy.LinAlgError encountered')
Notes
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
This class supports null-space motion to assist with maximising manipulability and avoiding joint limits. These are enabled by setting kq and km to non-zero values.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
See also
Changed in version 1.0.4: Added the Newton-Raphson IK solver method on the Robot class
- ikine_QP(Tep, end=None, start=None, q0=None, ilimit=30, slimit=100, tol=1e-06, mask=None, joint_limits=True, seed=None, kj=1.0, ks=1.0, kq=0.0, km=0.0, ps=0.0, pi=0.3, **kwargs)
Quadratic Programming Numerical Inverse Kinematics Solver
A method that provides functionality to perform numerical inverse kinematics (IK) using a quadratic progamming approach.
See the Inverse Kinematics Docs Page for more details and for a tutorial on numerical IK, see here.
- Parameters:
end (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effectorstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frameq0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – The initial joint coordinate vectorilimit (
int
) – How many iterations are allowed within a search before a new search is startedslimit (
int
) – How many searches are allowed before being deemed unsuccessfultol (
float
) – Maximum allowed residual error Emask (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – A 6 vector which assigns weights to Cartesian degrees-of-freedom error priorityjoint_limits (
bool
) – Reject solutions with joint limit violationsseed (
Optional
[int
]) – A seed for the private RNG used to generate random joint coordinate vectorskj – A gain for joint velocity norm minimisation
ks – A gain which adjusts the cost of slack (intentional error)
kq (
float
) – The gain for joint limit avoidance. Setting to 0.0 will remove this completely from the solutionkm (
float
) – The gain for maximisation. Setting to 0.0 will remove this completely from the solutionps (
float
) – The minimum angle/distance (in radians or metres) in which the joint is allowed to approach to its limitpi (
Union
[ndarray
,float
]) – The influence angle/distance (in radians or metres) in null space motion becomes active
- Raises:
ImportError – If the package
qpsolvers
is not installed
Synopsis
Each iteration uses the following approach
\[\vec{q}_{k+1} = \vec{q}_{k} + \dot{\vec{q}}.\]where the QP is defined as
\[\begin{split}\min_x \quad f_o(\vec{x}) &= \frac{1}{2} \vec{x}^\top \mathcal{Q} \vec{x}+ \mathcal{C}^\top \vec{x}, \\ \text{subject to} \quad \mathcal{J} \vec{x} &= \vec{\nu}, \\ \mathcal{A} \vec{x} &\leq \mathcal{B}, \\ \vec{x}^- &\leq \vec{x} \leq \vec{x}^+\end{split}\]with
\[\begin{split}\vec{x} &= \begin{pmatrix} \dvec{q} \\ \vec{\delta} \end{pmatrix} \in \mathbb{R}^{(n+6)} \\ \mathcal{Q} &= \begin{pmatrix} \lambda_q \mat{1}_{n} & \mathbf{0}_{6 \times 6} \\ \mathbf{0}_{n \times n} & \lambda_\delta \mat{1}_{6} \end{pmatrix} \in \mathbb{R}^{(n+6) \times (n+6)} \\ \mathcal{J} &= \begin{pmatrix} \mat{J}(\vec{q}) & \mat{1}_{6} \end{pmatrix} \in \mathbb{R}^{6 \times (n+6)} \\ \mathcal{C} &= \begin{pmatrix} \mat{J}_m \\ \bf{0}_{6 \times 1} \end{pmatrix} \in \mathbb{R}^{(n + 6)} \\ \mathcal{A} &= \begin{pmatrix} \mat{1}_{n \times n + 6} \\ \end{pmatrix} \in \mathbb{R}^{(l + n) \times (n + 6)} \\ \mathcal{B} &= \eta \begin{pmatrix} \frac{\rho_0 - \rho_s} {\rho_i - \rho_s} \\ \vdots \\ \frac{\rho_n - \rho_s} {\rho_i - \rho_s} \end{pmatrix} \in \mathbb{R}^{n} \\ \vec{x}^{-, +} &= \begin{pmatrix} \dvec{q}^{-, +} \\ \vec{\delta}^{-, +} \end{pmatrix} \in \mathbb{R}^{(n+6)},\end{split}\]where \(\vec{\delta} \in \mathbb{R}^6\) is the slack vector, \(\lambda_\delta \in \mathbb{R}^+\) is a gain term which adjusts the cost of the norm of the slack vector in the optimiser, \(\dvec{q}^{-,+}\) are the minimum and maximum joint velocities, and \(\dvec{\delta}^{-,+}\) are the minimum and maximum slack velocities.
Examples
The following example gets a
panda
robot object, makes a goal poseTep
, and then solves for the joint coordinates which result in the poseTep
using the ikine_QP method.File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/roboticstoolbox/robot/IK.py", line 1331, in __init__ "the package qpsolvers is required for this class. \nInstall using 'pip" ImportError: the package qpsolvers is required for this class. Install using 'pip install qpsolvers'
Notes
When using the this method, the initial joint coordinates \(q_0\), should correspond to a non-singular manipulator pose, since it uses the manipulator Jacobian.
This class supports null-space motion to assist with maximising manipulability and avoiding joint limits. These are enabled by setting kq and km to non-zero values.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
See also
Changed in version 1.0.4: Added the Quadratic Programming IK solver method on the Robot class
- inertia(q)
Manipulator inertia matrix
inertia(q)
is the symmetric joint inertia matrix (n,n) which relates joint torque to joint acceleration for the robot at joint configuration q.Trajectory operation
If
q
is a matrix (m,n), each row is interpretted as a joint state vector, and the result is a 3d-matrix (nxnxk) where each plane corresponds to the inertia for the corresponding row of q.- Parameters:
q (
ndarray
) – Joint coordinates- Returns:
The inertia matrix
- Return type:
inertia
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.inertia(puma.qz) array([[ 3.9611, -0.1627, -0.1389, 0.0016, -0.0004, 0. ], [-0.1627, 4.4566, 0.3727, 0. , 0.0019, 0. ], [-0.1389, 0.3727, 0.9387, 0. , 0.0019, 0. ], [ 0.0016, 0. , 0. , 0.1924, 0. , 0. ], [-0.0004, 0.0019, 0.0019, 0. , 0.1713, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0.1941]])
Notes
- The diagonal elements
M[j,j]
are the inertia seen by joint actuator
j
.
- The diagonal elements
- The off-diagonal elements
M[j,k]
are coupling inertias that relate acceleration on joint
j
to force/torque on jointk
.
- The off-diagonal elements
- The diagonal terms include the motor inertia reflected through
the gear ratio.
See also
- inertia_x(q=None, pinv=False, representation='rpy/xyz', Ji=None)
Operational space inertia matrix
robot.inertia_x(q)
is the operational space (Cartesian) inertia matrix which relates Cartesian force/torque to Cartesian acceleration at the joint configuration q.\[\mathbf{M}_x = \mathbf{J}(q)^{-T} \mathbf{M}(q) \mathbf{J}(q)^{-1}\]The transformation to operational space requires an analytical, rather than geometric, Jacobian.
analytical
can be one of:Value
Rotational representation
'rpy/xyz'
RPY angular rates in XYZ order (default)
'rpy/zyx'
RPY angular rates in XYZ order
'eul'
Euler angular rates in ZYZ order
'exp'
exponential coordinate rates
Trajectory operation
If
q
is a matrix (m,n), each row is interpretted as a joint state vector, and the result is a 3d-matrix (m,n,n) where each plane corresponds to the Cartesian inertia for the corresponding row ofq
.- Parameters:
q – Joint coordinates
pinv – use pseudo inverse rather than inverse (Default value = False)
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
representation – (Default value = “rpy/xyz”)
Ji – The inverse analytical Jacobian (base-frame)
- Returns:
The operational space inertia matrix
- Return type:
inertia_x
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
If the robot is not 6 DOF the
pinv
option is set True.pinv()
is around 5x slower thaninv()
Warning
Assumes that the operational space has 6 DOF.
See also
- isprismatic(j)
Check if joint is prismatic
- Returns:
True if prismatic
- Return type:
j
Examples
See also
Link.isprismatic()
,prismaticjoints()
- isrevolute(j)
Check if joint is revolute
- Returns:
True if revolute
- Return type:
j
Examples
See also
Link.isrevolute()
,revolutejoints()
- itorque(q, qdd)
Inertia torque
itorque(q, qdd)
is the inertia force/torque vector (n) at the specified joint configuration q (n) and acceleration qdd (n), andn
is the number of robot joints. It is \(\mathbf{I}(q) \ddot{q}\).Trajectory operation
If
q
andqdd
are matrices (m,n), each row is interpretted as a joint configuration, and the result is a matrix (m,n) where each row is the corresponding joint torques.- Parameters:
q – Joint coordinates
qdd – Joint acceleration
- Returns:
The inertia torque vector
- Return type:
itorque
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.itorque(puma.qz, 0.5 * np.ones((6,))) array([1.8304, 2.3343, 0.5872, 0.0971, 0.0873, 0.0971])
Notes
- If the robot model contains non-zero motor inertia then this
will be included in the result.
See also
- jacob0(q, end=None, start=None, tool=None)
Manipulator geometric Jacobian in the
start
framerobot.jacobo(q)
is the manipulator Jacobian matrix which maps joint velocity to end-effector spatial velocity expressed in the base frame.End-effector spatial velocity \(\nu = (v_x, v_y, v_z, \omega_x, \omega_y, \omega_z)^T\) is related to joint velocity by \({}^{E}\!\nu = \mathbf{J}_m(q) \dot{q}\).
- Parameters:
q (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – Joint coordinate vectorend (
Union
[str
,Link
,Gripper
,None
]) – the particular link or gripper whose velocity the Jacobian describes, defaults to the end-effector if only one is presentstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frametool (
Union
[ndarray
,SE3
,None
]) – a static tool transformation matrix to apply to the end of end, defaults to None
- Returns:
Manipulator Jacobian in the
start
frame- Return type:
J0
Examples
The following example makes a
Puma560
robot object, and solves for the base-frame Jacobian at the zero joint angle configuration>>> import roboticstoolbox as rtb >>> puma = rtb.models.Puma560() >>> puma.jacob0([0, 0, 0, 0, 0, 0]) array([[ 0.1295, -0.4854, -0.4854, -0. , -0.0533, 0. ], [ 0.4318, 0. , 0. , 0. , 0. , 0. ], [-0. , 0.4318, 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , -1. , -1. , 0. , -1. , 0. ], [ 1. , 0. , 0. , 1. , 0. , 1. ]])
Notes
- This is the geometric Jacobian as described in texts by
Corke, Spong etal., Siciliano etal. The end-effector velocity is described in terms of translational and angular velocity, not a velocity twist as per the text by Lynch & Park.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
- jacob0_analytical(q, representation='rpy/xyz', end=None, start=None, tool=None)
Manipulator analytical Jacobian in the
start
framerobot.jacob0_analytical(q)
is the manipulator Jacobian matrix which maps joint velocity to end-effector spatial velocity expressed in thestart
frame.- Parameters:
q (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – Joint coordinate vectorrepresentation (
Literal
['rpy/xyz'
,'rpy/zyx'
,'eul'
,'exp'
]) – angular representationend (
Union
[str
,Link
,Gripper
,None
]) – the particular link or gripper whose velocity the Jacobian describes, defaults to the base linkstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the end-effector, defaults to the robots’s end-effectortool (
Union
[ndarray
,SE3
,None
]) – a static tool transformation matrix to apply to the end of end, defaults to None
- Returns:
Manipulator Jacobian in the
start
frame- Return type:
jacob0
Synopsis
End-effector spatial velocity \(\nu = (v_x, v_y, v_z, \omega_x, \omega_y, \omega_z)^T\) is related to joint velocity by \({}^{E}\!\nu = \mathbf{J}_m(q) \dot{q}\).
|``representation`` | Rotational representation | |---------------------|————————————-| |
'rpy/xyz'
| RPY angular rates in XYZ order | |'rpy/zyx'
| RPY angular rates in XYZ order | |'eul'
| Euler angular rates in ZYZ order | |'exp'
| exponential coordinate rates |Examples
Makes a robot object and computes the analytic Jacobian for the given joint configuration
>>> import roboticstoolbox as rtb >>> puma = rtb.models.ETS.Puma560() >>> puma.jacob0_analytical([0, 0, 0, 0, 0, 0]) array([[ 0.15 , 0.8636, 0.4318, 0. , 0. , 0. ], [ 0.2203, 0. , 0. , 0.2 , 0. , 0.2 ], [ 0. , -0.2203, -0.2 , 0. , -0.2 , 0. ], [ 1. , 0. , 0. , 1. , 0. , 1. ], [ 0. , 1. , 1. , 0. , 1. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ]])
- jacobe(q, end=None, start=None, tool=None)
Manipulator geometric Jacobian in the end-effector frame
robot.jacobe(q)
is the manipulator Jacobian matrix which maps joint velocity to end-effector spatial velocity expressed in theend
frame.End-effector spatial velocity \(\nu = (v_x, v_y, v_z, \omega_x, \omega_y, \omega_z)^T\) is related to joint velocity by \({}^{E}\!\nu = \mathbf{J}_m(q) \dot{q}\).
- Parameters:
q (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – Joint coordinate vectorend (
Union
[str
,Link
,Gripper
,None
]) – the particular link or gripper whose velocity the Jacobian describes, defaults to the end-effector if only one is presentstart (
Union
[str
,Link
,Gripper
,None
]) – the link considered as the base frame, defaults to the robots’s base frametool (
Union
[ndarray
,SE3
,None
]) – a static tool transformation matrix to apply to the end of end, defaults to None
- Returns:
Manipulator Jacobian in the
end
frame- Return type:
Je
Examples
The following example makes a
Puma560
robot object, and solves for the end-effector frame Jacobian at the zero joint angle configuration>>> import roboticstoolbox as rtb >>> puma = rtb.models.Puma560() >>> puma.jacobe([0, 0, 0, 0, 0, 0]) array([[ 0.1295, -0.4854, -0.4854, -0. , -0.0533, 0. ], [ 0.4318, 0. , 0. , 0. , 0. , 0. ], [-0. , 0.4318, 0. , 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ], [ 0. , -1. , -1. , 0. , -1. , 0. ], [ 1. , 0. , 0. , 1. , 0. , 1. ]])
Notes
- This is the geometric Jacobian as described in texts by
Corke, Spong etal., Siciliano etal. The end-effector velocity is described in terms of translational and angular velocity, not a velocity twist as per the text by Lynch & Park.
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
- jointdynamics(q, qd=None)
Transfer function of joint actuator
tf = jointdynamics(qd, q)
calculates a vector of n continuous-time transfer functions that represent the transfer function 1/(Js+B) for each joint based on the dynamic parameters of the robot and the configuration q (n). n is the number of robot joints. The result is a list of tuples (J, B) for each joint.tf = jointdynamics(q, qd)
as above but include the linearized effects of Coulomb friction when operating at joint velocity QD (1xN).- Parameters:
q – Joint coordinates
qd – Joint velocity
- Returns:
transfer function denominators
- Return type:
list of 2-tuples
- linkcolormap(linkcolors='viridis')
Create a colormap for robot joints
cm = robot.linkcolormap()
is an n-element colormap that gives a unique color for every link. The RGBA colors for linkj
arecm(j)
.cm = robot.linkcolormap(cmap)
as above butcmap
is the name of a valid matplotlib colormap. The default, example above, is theviridis
colormap.cm = robot.linkcolormap(list of colors)
as above but a colormap is created from a list of n color names given as strings, tuples or hexstrings.
- Parameters:
linkcolors (
Union
[List
[Any
],str
]) – list of colors or colormap, defaults to “viridis”- Returns:
the color map
- Return type:
color map
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> cm = robot.linkcolormap("inferno") >>> print(cm(range(6))) # cm(i) is 3rd color in colormap [[0.0015 0.0005 0.0139 1. ] [0.2582 0.0386 0.4065 1. ] [0.5783 0.148 0.4044 1. ] [0.865 0.3168 0.2261 1. ] [0.9876 0.6453 0.0399 1. ] [0.9884 0.9984 0.6449 1. ]] >>> cm = robot.linkcolormap( ... ['red', 'g', (0,0.5,0), '#0f8040', 'yellow', 'cyan']) >>> print(cm(range(6))) [[1. 0. 0. 1. ] [0. 0.5 0. 1. ] [0. 0.5 0. 1. ] [0.0588 0.502 0.251 1. ] [1. 1. 0. 1. ] [0. 1. 1. 1. ]]
Notes
Colormaps have 4-elements: red, green, blue, alpha (RGBA)
Names of supported colors and colormaps are defined in the matplotlib documentation.
- property links: List[LinkType]
Robot links
- Returns:
A list of link objects
- Return type:
links
Notes
It is probably more concise to index the robot object rather than the list of links, ie. the following are equivalent: -
robot.links[i]
-robot[i]
- property manufacturer
Get/set robot manufacturer’s name
robot.manufacturer
is the robot manufacturer’s namerobot.manufacturer = ...
checks and sets the manufacturer’s name
- Returns:
robot manufacturer’s name
- Return type:
manufacturer
- property n: int
Number of joints
- Returns:
Number of joints
- Return type:
n
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.n 6
See also
- property name: str
Get/set robot name
robot.name
is the robot namerobot.name = ...
checks and sets the robot name
- Parameters:
name – the new robot name
- Returns:
the current robot name
- Return type:
name
- property nbranches: int
Number of branches
Number of branches in this robot. Computed as the number of links with zero children
- Returns:
number of branches in the robot’s kinematic tree
- Return type:
nbranches
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.ETS.Panda() >>> robot.nbranches 1
- property nlinks
Number of links
The returned number is the total of both variable joints and static links
- Returns:
Number of links
- Return type:
nlinks
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.nlinks 6
See also
- nofriction(coulomb=True, viscous=False)
Remove manipulator joint friction
nofriction()
copies the robot and returns a robot with the same link parameters except the Coulomb and/or viscous friction parameter are set to zero.- Parameters:
- Returns:
A copy of the robot with dynamic parameters perturbed
- Return type:
robot
See also
Robot.friction()
,Link.nofriction()
- partial_fkine0(q, n=3, end=None, start=None)
Manipulator Forward Kinematics nth Partial Derivative
This method computes the nth derivative of the forward kinematics where
n
is greater than or equal to 3. This is an extension of the differential kinematics where the Jacobian is the first partial derivative and the Hessian is the second.- Parameters:
q (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – The joint angles/configuration of the robot (Optional, if not supplied will use the stored q values).end (
Union
[str
,Link
,Gripper
,None
]) – the final link/Gripper which the Hessian representsstart (
Union
[str
,Link
,Gripper
,None
]) – the first link which the Hessian representstool – a static tool transformation matrix to apply to the end of end, defaults to None
- Returns:
The nth Partial Derivative of the forward kinematics
- Return type:
A
Examples
The following example makes a
Panda
robot object, and solves for the base-effector frame 4th defivative of the forward kinematics at the given joint angle configuration>>> import roboticstoolbox as rtb >>> panda = rtb.models.Panda() >>> panda.partial_fkine0([0, -0.3, 0, -2.2, 0, 2, 0.7854], n=4) array([[[[[ 0.484 , 0. , 0.486 , ..., 0.1547, -0. , 0. ], [-0. , -0.0796, -0. , ..., -0. , -0.2006, 0. ], [-0. , -0. , -0. , ..., -0. , -0. , 0. ], [ 0. , 1. , 0. , ..., -0. , -1. , -0. ], [ 0. , 0. , 0.2955, ..., -0.9463, 0. , -0.0998], [ 0. , -0. , 0. , ..., -0. , 0. , -0. ]], [[ 0. , 0.484 , 0. , ..., 0. , -0.1086, 0. ], [-0. , -0. , -0. , ..., -0. , -0. , 0. ], [ 0. , -0. , -0. , ..., -0. , 0. , 0. ], [-1. , 0. , -0.9553, ..., 0.3233, -0. , 0.995 ], [-0. , 0. , 0. , ..., -0. , 0. , -0. ], [ 0. , 0. , 0. , ..., 0. , 0. , -0. ]], [[ 0.4624, 0. , 0.4643, ..., 0.1478, -0. , 0. ], [-0. , 0.067 , -0. , ..., -0. , -0.2237, 0. ], [-0. , 0. , -0. , ..., -0. , -0. , 0. ], [-0. , 0.9553, 0. , ..., -0. , -0.9553, -0. ], [-0.2955, -0. , 0. , ..., -0.8085, 0. , 0.1987], [-0. , -0. , 0. , ..., -0. , 0. , 0. ]], ..., [[-0.1565, -0. , -0.1571, ..., -0.05 , 0. , 0. ], [ 0. , -0.4323, 0. , ..., -0. , 0.1676, 0. ], [ 0. , -0. , 0. , ..., 0. , 0. , 0. ], [ 0. , -0.3233, 0. , ..., 0. , 0.3233, -0. ], [ 0.9463, 0. , 0.8085, ..., 0. , 0. , -0.9093], [ 0. , 0. , 0. , ..., 0. , 0. , -0. ]], [[ 0. , -0.484 , 0. , ..., -0. , 0.1086, 0. ], [-0. , 0. , -0. , ..., -0. , -0. , 0. ], [ 0. , 0. , -0. , ..., 0. , 0. , 0. ], [ 1. , 0. , 0.9553, ..., -0.3233, 0. , -0.995 ], [-0. , -0. , -0. , ..., -0. , 0. , 0. ], [-0. , -0. , -0. , ..., 0. , 0. , 0. ]], [[-0.4816, -0. , -0.4835, ..., -0.1539, 0. , 0. ], [ 0. , 0.0309, 0. , ..., 0. , 0.2104, 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , -0.995 , 0. , ..., 0. , 0.995 , 0. ], [ 0.0998, 0. , -0.1987, ..., 0.9093, -0. , 0. ], [ 0. , 0. , -0. , ..., 0. , -0. , 0. ]]], [[[ 0. , 0. , 0. , ..., 0. , -0. , 0. ], [-0. , -0. , -0. , ..., -0. , -0. , 0. ], [-0. , -0.0796, -0. , ..., -0. , -0.2006, 0. ], [ 0. , 0. , 0. , ..., -0. , -0. , 0. ], [ 0. , 0. , 0. , ..., -0. , 0. , -0. ], [ 0. , -0. , 0.2955, ..., -0.9463, 0. , -0.0998]], [[-0. , 0. , 0. , ..., 0. , -0. , 0. ], [ 0. , -0.0796, -0. , ..., -0. , -0.2006, 0. ], [-0.0796, -0. , 0. , ..., 0. , -0. , 0. ], [-0. , 0. , -0. , ..., 0. , -0. , 0. ], [-0. , 0. , 0.2955, ..., -0.9463, 0. , -0.0998], [ 0. , 0. , 0. , ..., -0. , 0. , -0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [-0.143 , -0. , -0.1436, ..., -0.0457, -0. , 0. ], [-0. , 0. , -0. , ..., -0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , -0. , 0. ], [-0. , -0.2955, 0. , ..., -0. , 0.2955, 0. ], [-0.2955, -0. , 0. , ..., -0. , 0. , 0. ]], ..., [[ 0. , 0. , -0. , ..., -0. , 0. , 0. ], [ 0.4581, 0. , 0.4599, ..., 0.1464, 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , -0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0.9463, 0. , ..., 0. , -0.9463, -0. ], [ 0.9463, 0. , 0. , ..., 0. , -0. , 0. ]], [[ 0. , -0. , 0. , ..., -0. , 0. , 0. ], [-0. , 0.0796, 0. , ..., 0. , 0.2006, 0. ], 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, ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], ..., [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 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, 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]]], [[[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], ..., [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]]], ..., [[[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], ..., [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]]], [[[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], ..., [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]]], [[[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], ..., [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]], [[ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ], [ 0. , 0. , 0. , ..., 0. , 0. , 0. ]]]]])
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part II: Acceleration and Advanced Applications.” arXiv preprint arXiv:2207.01794 (2022).
- pay(W, q=None, J=None, frame=1)
Generalised joint force/torque due to a payload wrench
tau = pay(W, J) Returns the generalised joint force/torques due to a payload wrench W applied to the end-effector. Where the manipulator Jacobian is J (6xn), and n is the number of robot joints.
tau = pay(W, q, frame) as above but the Jacobian is calculated at pose q in the frame given by frame which is 0 for base frame, 1 for end-effector frame.
Uses the formula tau = J’W, where W is a wrench vector applied at the end effector, W = [Fx Fy Fz Mx My Mz]’.
- Trajectory operation:
In the case q is nxm or J is 6xnxm then tau is nxm where each row is the generalised force/torque at the pose given by corresponding row of q.
- Parameters:
W (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – A wrench vector applied at the end effector, W = [Fx Fy Fz Mx My Mz]J (
Optional
[ndarray
]) – The manipulator Jacobian (Optional, if not supplied will use the q value).frame (
int
) – The frame in which to torques are expressed in when J is not supplied. 0 means base frame of the robot, 1 means end- effector frame
- Returns:
Joint forces/torques due to w
- Return type:
t
Notes
- Wrench vector and Jacobian must be from the same reference
frame.
Tool transforms are taken into consideration when frame=1.
- Must have a constant wrench - no trajectory support for this
yet.
- paycap(w, tauR, frame=1, q=None)
Static payload capacity of a robot
wmax, joint = paycap(q, w, f, tauR)
returns the maximum permissible payload wrenchwmax
(6) applied at the end-effector, and the index of the joint (zero indexed) which hits its force/torque limit at that wrench.q
(n) is the manipulator pose,w
the payload wrench (6),f
the wrench reference frame and tauR (nx2) is a matrix of joint forces/torques (first col is maximum, second col minimum).Trajectory operation:
In the case q is nxm then wmax is Mx6 and J is Mx1 where the rows are the results at the pose given by corresponding row of q.
- Parameters:
w (
ndarray
) – The payload wrenchtauR (
ndarray
) – Joint torque matrix minimum and maximumsframe (
int
) – The frame in which to torques are expressed in when J is not supplied. ‘base’ means base frame of the robot, ‘ee’ means end-effector frameq (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – Joint coordinates
- Returns:
The maximum permissible payload wrench
- Return type:
ndarray(6)
Notes
Wrench vector and Jacobian must be from the same reference frame
Tool transforms are taken into consideration for frame=1.
- payload(m, p=array([0.0, 0.0, 0.0]))
Add a payload to the end-effector
payload(m, p) adds payload mass adds a payload with point mass m at position p in the end-effector coordinate frame.
payload(m) adds payload mass adds a payload with point mass m at in the end-effector coordinate frame.
payload(0) removes added payload.
- Parameters:
m (
float
) – mass (kg)p – position in end-effector frame
- perturb(p=0.1)
Perturb robot parameters
rp = perturb(p) is a new robot object in which the dynamic parameters (link mass and inertia) have been perturbed. The perturbation is multiplicative so that values are multiplied by random numbers in the interval (1-p) to (1+p). The name string of the perturbed robot is prefixed by ‘P/’.
Useful for investigating the robustness of various model-based control schemes. For example to vary parameters in the range +/- 10 percent is: r2 = puma.perturb(0.1)
- Parameters:
p – The percent (+/-) to be perturbed. Default 10%
- Returns:
A copy of the robot with dynamic parameters perturbed
- Return type:
- plot(q, backend=None, block=False, dt=0.05, limits=None, vellipse=False, fellipse=False, fig=None, movie=None, loop=False, **kwargs)
Graphical display and animation
robot.plot(q, 'pyplot')
displays a graphical view of a robot based on the kinematic model and the joint configurationq
. This is a stick figure polyline which joins the origins of the link coordinate frames. The plot will autoscale with an aspect ratio of 1.If
q
(m,n) representing a joint-space trajectory it will create an animation with a pause ofdt
seconds between each frame.- q
The joint configuration of the robot.
- backend
The graphical backend to use, currently ‘swift’ and ‘pyplot’ are implemented. Defaults to ‘swift’ of a
Robot
and ‘pyplot` for aDHRobot
- block
Block operation of the code and keep the figure open
- dt
if q is a trajectory, this describes the delay in seconds between frames
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2] (this option is for ‘pyplot’ only)
- vellipse
(Plot Option) Plot the velocity ellipse at the end-effector (this option is for ‘pyplot’ only)
- fellipse
(Plot Option) Plot the force ellipse at the end-effector (this option is for ‘pyplot’ only)
- fig
(Plot Option) The figure label to plot in (this option is for ‘pyplot’ only)
- movie
(Plot Option) The filename to save the movie to (this option is for ‘pyplot’ only)
- loop
(Plot Option) Loop the movie (this option is for ‘pyplot’ only)
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint) (this option is for ‘pyplot’ only)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes. (this option is for ‘pyplot’ only)
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane. (this option is for ‘pyplot’ only)
- name
(Plot Option) Plot the name of the robot near its base (this option is for ‘pyplot’ only)
- Returns:
A reference to the environment object which controls the figure
- Return type:
env
Notes
- By default this method will block until the figure is dismissed.
To avoid this set
block=False
.
- For PyPlot, the polyline joins the origins of the link frames,
but for some Denavit-Hartenberg models those frames may not actually be on the robot, ie. the lines to not neccessarily represent the links of the robot.
See also
- plot_ellipse(ellipse, block=True, limits=None, jointaxes=True, eeframe=True, shadow=True, name=True)
Plot the an ellipsoid
robot.plot_ellipse(ellipsoid)
displays the ellipsoid.- ellipse
the ellipsoid to plot
- block
Block operation of the code and keep the figure open
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes.
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane
- name
(Plot Option) Plot the name of the robot near its base
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
- plot_fellipse(q, block=True, fellipse=None, limits=None, opt='trans', centre=[0, 0, 0], jointaxes=True, eeframe=True, shadow=True, name=True)
Plot the force ellipsoid for manipulator
robot.plot_fellipse(q)
displays the velocity ellipsoid for the robot at poseq
. The plot will autoscale with an aspect ratio of 1.robot.plot_fellipse(vellipse)
specifies a custon ellipse to plot.- q
The joint configuration of the robot
- block
Block operation of the code and keep the figure open
- fellipse
the vellocity ellipsoid to plot
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational force ellipsoid
- centre
The coordinates to plot the fellipse [x, y, z] or “ee” to plot at the end-effector location
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes.
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane
- name
(Plot Option) Plot the name of the robot near its base
- Raises:
ValueError – q or fellipse must be supplied
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- plot_vellipse(q, block=True, vellipse=None, limits=None, opt='trans', centre=[0, 0, 0], jointaxes=True, eeframe=True, shadow=True, name=True)
Plot the velocity ellipsoid for manipulator
robot.plot_vellipse(q)
displays the velocity ellipsoid for the robot at poseq
. The plot will autoscale with an aspect ratio of 1.robot.plot_vellipse(vellipse)
specifies a custon ellipse to plot.- block
Block operation of the code and keep the figure open
- q
The joint configuration of the robot
- vellipse
the vellocity ellipsoid to plot
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational velocity ellipsoid
- centre
The coordinates to plot the vellipse [x, y, z] or “ee” to plot at the end-effector location
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes.
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane
- name
(Plot Option) Plot the name of the robot near its base
- Raises:
ValueError – q or fellipse must be supplied
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- property prismaticjoints: List[bool]
Revolute joints as bool array
- Returns:
array of joint type, True if prismatic
- Return type:
prismaticjoints
Examples
Notes
Fixed joints, that maintain a constant link relative pose, are not included.
See also
Link.isprismatic()
,revolutejoints()
- property q: ndarray
Get/set robot joint configuration
robot.q
is the robot joint configurationrobot.q = ...
checks and sets the joint configuration
- Parameters:
q – the new robot joint configuration
- Returns:
robot joint configuration
- Return type:
q
- property qd: ndarray
Get/set robot joint velocity
robot.qd
is the robot joint velocityrobot.qd = ...
checks and sets the joint velocity
- Returns:
robot joint velocity
- Return type:
qd
- property qdd: ndarray
Get/set robot joint acceleration
robot.qdd
is the robot joint accelerationrobot.qdd = ...
checks and sets the robot joint acceleration
- Returns:
robot joint acceleration
- Return type:
qdd
- property qlim: ndarray
Joint limits
Limits are extracted from the link objects. If joints limits are not set for:
a revolute joint [-𝜋. 𝜋] is returned
a prismatic joint an exception is raised
- qlim
An array of joints limits (2, n)
- Raises:
ValueError – unset limits for a prismatic joint
- Returns:
Array of joint limit values
- Return type:
qlim
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.qlim array([[-2.7925, -1.9199, -2.3562, -4.6426, -1.7453, -4.6426], [ 2.7925, 1.9199, 2.3562, 4.6426, 1.7453, 4.6426]])
- random_q()
Return a random joint configuration
The value for each joint is uniform randomly distributed between the limits set for the robot.
Note
The joint limit for all joints must be set.
- Returns:
Random joint configuration :rtype: ndarray(n)
- Return type:
q
See also
Robot.qlim()
,Link.qlim()
- property revolutejoints: List[bool]
Revolute joints as bool array
- Returns:
array of joint type, True if revolute
- Return type:
revolutejoints
Examples
Notes
Fixed joints, that maintain a constant link relative pose, are not included.
See also
Link.isrevolute()
,prismaticjoints()
- segments()
Segments of branched robot
For a single-chain robot with structure:
L1 - L2 - L3
the return is
[[None, L1, L2, L3]]
For a robot with structure:
L1 - L2 +- L3 - L4 +- L5 - L6
the return is
[[None, L1, L2], [L2, L3, L4], [L2, L5, L6]]
- Returns:
Segment list
- Return type:
segments
Notes
the length of the list is the number of segments in the robot
- the first segment always starts with
None
which represents the base transform (since there is no base link)
- the first segment always starts with
- the last link of one segment is also the first link of subsequent
segments
- showgraph(display_graph=True, **kwargs)
Display a link transform graph in browser
robot.showgraph()
displays a graph of the robot’s link frames and the ETS between them. It uses GraphViz dot.- The nodes are:
Base is shown as a grey square. This is the world frame origin, but can be changed using the
base
attribute of the robot.Link frames are indicated by circles
ETS transforms are indicated by rounded boxes
- The edges are:
an arrow if jtype is False or the joint is fixed
an arrow with a round head if jtype is True and the joint is revolute
an arrow with a box head if jtype is True and the joint is prismatic
Edge labels or nodes in blue have a fixed transformation to the preceding link.
- Parameters:
display_graph (
bool
) – Open the graph in a browser if True. Otherwise will return the file pathetsbox – Put the link ETS in a box, otherwise an edge label
jtype – Arrowhead to node indicates revolute or prismatic type
static – Show static joints in blue and bold
- Return type:
Examples
>>> import roboticstoolbox as rtb >>> panda = rtb.models.URDF.Panda() >>> panda.showgraph()
See also
- property structure: str
Return the joint structure string
A string with one letter per joint:
R
for a revolute joint, andP
for a prismatic joint.- Returns:
joint configuration string
- Return type:
structure
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.structure 'RRRRRR' >>> stanford = rtb.models.DH.Stanford() >>> stanford.structure 'RRPRRR'
Notes
Fixed joints, that maintain a constant link relative pose, are not included.
len(self.structure) == self.n
.
- teach(q, block=True, limits=None, vellipse=False, fellipse=False, backend=None)
Graphical teach pendant
robot.teach(q)
creates a matplotlib plot which allows the user to “drive” a graphical robot using a graphical slider panel. The robot’s inital joint configuration isq
. The plot will autoscale with an aspect ratio of 1.robot.teach()
as above except the robot’s stored value ofq
is used.- q
The joint configuration of the robot (Optional, if not supplied will use the stored q values).
- block
Block operation of the code and keep the figure open
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- vellipse
(Plot Option) Plot the velocity ellipse at the end-effector (this option is for ‘pyplot’ only)
- fellipse
(Plot Option) Plot the force ellipse at the end-effector (this option is for ‘pyplot’ only)
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
Notes
- Program execution is blocked until the teach window is
dismissed. If
block=False
the method is non-blocking but you need to poll the window manager to ensure that the window remains responsive.
- The slider limits are derived from the joint limit properties.
If not set then: - For revolute joints they are assumed to be [-pi, +pi] - For prismatic joint they are assumed unknown and an error
occurs.
- todegrees(q)
Convert joint angles to degrees
- Parameters:
q – The joint configuration of the robot
- Return type:
- Returns:
q – a vector of joint coordinates in degrees and metres
robot.todegrees(q)
converts joint coordinatesq
to degreestaking into account whether elements of
q
correspond to revoluteor prismatic joints, ie. prismatic joint values are not converted.
If
q
is a matrix, with one column per joint, the conversion isperformed columnwise.
Examples
>>> import roboticstoolbox as rtb >>> from math import pi >>> stanford = rtb.models.DH.Stanford() >>> stanford.todegrees([pi/4, pi/8, 2, -pi/4, pi/6, pi/3]) array([ 45. , 22.5, 2. , -45. , 30. , 60. ])
- property tool: SE3
Get/set robot tool transform
robot.tool
is the robot tool transform as an SE3 objectrobot._tool
is the robot tool transform as a numpy arrayrobot.tool = ...
checks and sets the robot tool transform
- Parameters:
tool – the new robot tool transform (as an SE(3))
- Returns:
robot tool transform
- Return type:
tool
- toradians(q)
Convert joint angles to radians
robot.toradians(q)
converts joint coordinatesq
to radians taking into account whether elements ofq
correspond to revolute or prismatic joints, ie. prismatic joint values are not converted.If
q
is a matrix, with one column per joint, the conversion is performed columnwise.- Parameters:
q – The joint configuration of the robot
- Returns:
a vector of joint coordinates in radians and metres
- Return type:
q
Examples
>>> import roboticstoolbox as rtb >>> stanford = rtb.models.DH.Stanford() >>> stanford.toradians([10, 20, 2, 30, 40, 50]) array([0.1745, 0.3491, 2. , 0.5236, 0.6981, 0.8727])
- vellipse(q, opt='trans', unit='rad', centre=[0, 0, 0], scale=0.1)
Create a velocity ellipsoid object for plotting with PyPlot
robot.vellipse(q)
creates a force ellipsoid for the robot at poseq
. The ellipsoid is centered at the origin.- q
The joint configuration of the robot.
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational force ellipsoid
- unit
‘rad’ or ‘deg’ will plot the ellipsoid in radians or degrees
- centre
The centre of the ellipsoid, either ‘ee’ for the end-effector or a 3-vector [x, y, z] in the world frame
- scale
The scale factor for the ellipsoid
- Returns:
An EllipsePlot object
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- class roboticstoolbox.robot.Robot.Robot2(arg, **kwargs)[source]
Bases:
BaseRobot
[Link2
]- __getitem__(i)
Get link
This also supports iterating over each link in the robot object, from the base to the tool.
- Parameters:
- Returns:
i’th link or named link
- Return type:
link
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> print(robot[1]) # print the 2nd link RevoluteDH: θ=q, d=0, a=0.4318, ⍺=0.0 >>> print([link.a for link in robot]) # print all the a_j values [0, 0.4318, 0.0203, 0, 0, 0]
Notes
Robot
supports link lookup by name,eg.
robot['link1']
- __str__()
Pretty prints the ETS Model of the robot.
- Returns:
Pretty print of the robot model
- Return type:
Notes
Constant links are shown in blue.
End-effector links are prefixed with an @
Angles in degrees
- The robot base frame is denoted as
BASE
and is equal to the robot’s
base
attribute.
- The robot base frame is denoted as
- accel(q, qd, torque, gravity=None)
Compute acceleration due to applied torque
qdd = accel(q, qd, torque)
calculates a vector (n) of joint accelerations that result from applying the actuator force/torque (n) to the manipulator in state q (n) and qd (n), andn
is the number of robot joints.\[\ddot{q} = \mathbf{M}^{-1} \left(\tau - \mathbf{C}(q)\dot{q} - \mathbf{g}(q)\right)\]Trajectory operation
If q, qd, torque are matrices (m,n) then
qdd
is a matrix (m,n) where each row is the acceleration corresponding to the equivalent rows of q, qd, torque.- Parameters:
q – Joint coordinates
qd – Joint velocity
torque – Joint torques of the robot
gravity – Gravitational acceleration (Optional, if not supplied will use the
gravity
attribute of self).
- Return type:
ndarray(n)
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.accel(puma.qz, 0.5 * np.ones(6), np.zeros(6)) array([ -7.5544, -12.22 , -6.4022, -5.4303, -4.9518, -2.1178])
Notes
- Useful for simulation of manipulator dynamics, in
conjunction with a numerical integration function.
- Uses the method 1 of Walker and Orin to compute the forward
dynamics.
- Featherstone’s method is more efficient for robots with large
numbers of joints.
Joint friction is considered.
References
- Efficient dynamic computer simulation of robotic mechanisms,
M. W. Walker and D. E. Orin, ASME Journa of Dynamic Systems, Measurement and Control, vol. 104, no. 3, pp. 205-211, 1982.
- accel_x(q, xd, wrench, gravity=None, pinv=False, representation='rpy/xyz')
Operational space acceleration due to applied wrench
xdd = accel_x(q, qd, wrench)
is the operational space acceleration due towrench
applied to the end-effector of a robot in joint configurationq
and joint velocityqd
.\[\ddot{x} = \mathbf{J}(q) \mathbf{M}(q)^{-1} \left( \mathbf{J}(q)^T w - \mathbf{C}(q)\dot{q} - \mathbf{g}(q) \right)\]Trajectory operation
If q, qd, torque are matrices (m,n) then
qdd
is a matrix (m,n) where each row is the acceleration corresponding to the equivalent rows of q, qd, wrench.- Parameters:
q – Joint coordinates
qd – Joint velocity
wrench – Wrench applied to the end-effector
gravity – Gravitational acceleration (Optional, if not supplied will use the
gravity
attribute of self).pinv – use pseudo inverse rather than inverse
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
xd –
representation – (Default value = “rpy/xyz”)
- Returns:
Operational space accelerations of the end-effector
- Return type:
accel
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
- Useful for simulation of manipulator dynamics, in
conjunction with a numerical integration function.
- Uses the method 1 of Walker and Orin to compute the forward
dynamics.
- Featherstone’s method is more efficient for robots with large
numbers of joints.
Joint friction is considered.
See also
- addconfiguration(name, q)
Add a named joint configuration
Add a named configuration to the robot instance’s dictionary of named configurations.
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.addconfiguration_attr("mypos", [0.1, 0.2, 0.3, 0.4, 0.5, 0.6]) >>> robot.configs["mypos"] array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6])
See also
- addconfiguration_attr(name, q, unit='rad')
Add a named joint configuration as an attribute
- Parameters:
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.addconfiguration_attr("mypos", [0.1, 0.2, 0.3, 0.4, 0.5, 0.6]) >>> robot.mypos array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6]) >>> robot.configs["mypos"] array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6])
Notes
Used in robot model init method to store the
qr
configuration- Dynamically adding attributes to objects can cause issues with
Python type checking.
- Configuration is also added to the robot instance’s dictionary of
named configurations.
See also
- attach(object)
- attach_to(object)
- property base_link: LinkType
Get the robot base link
robot.base_link
is the robot base link
- Returns:
the first link in the robot tree
- Return type:
base_link
- cinertia(q)
Deprecated, use
inertia_x
- property comment: str
Get/set robot comment
robot.comment
is the robot commentrobot.comment = ...
checks and sets the robot comment
- Parameters:
name – the new robot comment
- Returns:
robot comment
- Return type:
comment
- configurations_str(border='thin')
- property control_mode: str
Get/set robot control mode
robot.control_type
is the robot control moderobot.control_type = ...
checks and sets the robot control mode
- Parameters:
control_mode – the new robot control mode
- Returns:
the current robot control mode
- Return type:
control_mode
- copy()
- coriolis(q, qd)
Coriolis and centripetal term
coriolis(q, qd)
calculates the Coriolis/centripetal matrix (n,n) for the robot in configurationq
and velocityqd
, wheren
is the number of joints.The product \(\mathbf{C} \dot{q}\) is the vector of joint force/torque due to velocity coupling. The diagonal elements are due to centripetal effects and the off-diagonal elements are due to Coriolis effects. This matrix is also known as the velocity coupling matrix, since it describes the disturbance forces on any joint due to velocity of all other joints.
Trajectory operation
If
q
and qd are matrices (m,n), each row is interpretted as a joint configuration, and the result (n,n,m) is a 3d-matrix where each plane corresponds to a row ofq
andqd
.- Parameters:
q – Joint coordinates
qd – Joint velocity
- Returns:
Velocity matrix
- Return type:
coriolis
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.coriolis(puma.qz, 0.5 * np.ones((6,))) array([[-0.4017, -0.5513, -0.2025, -0.0007, -0.0013, 0. ], [ 0.2023, -0.1937, -0.3868, -0. , -0.002 , 0. ], [ 0.1987, 0.193 , -0. , 0. , -0.0001, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ], [ 0.0007, 0.0007, 0.0001, 0. , 0. , 0. ], [ 0. , 0. , 0. , 0. , 0. , 0. ]])
Notes
- Joint viscous friction is also a joint force proportional to
velocity but it is eliminated in the computation of this value.
Computationally slow, involves \(n^2/2\) invocations of RNE.
- coriolis_x(q, qd, pinv=False, representation='rpy/xyz', J=None, Ji=None, Jd=None, C=None, Mx=None)
Operational space Coriolis and centripetal term
coriolis_x(q, qd)
is the Coriolis/centripetal matrix (m,m) in operational space for the robot in configurationq
and velocityqd
, wheren
is the number of joints.\[\mathbf{C}_x = \mathbf{J}(q)^{-T} \left( \mathbf{C}(q) - \mathbf{M}_x(q) \mathbf{J})(q) \right) \mathbf{J}(q)^{-1}\]The product \(\mathbf{C} \dot{x}\) is the operational space wrench due to joint velocity coupling. This matrix is also known as the velocity coupling matrix, since it describes the disturbance forces on any joint due to velocity of all other joints.
The transformation to operational space requires an analytical, rather than geometric, Jacobian.
analytical
can be one of:Value
Rotational representation
'rpy/xyz'
RPY angular rates in XYZ order (default)
'rpy/zyx'
RPY angular rates in XYZ order
'eul'
Euler angular rates in ZYZ order
'exp'
exponential coordinate rates
Trajectory operation
If
q
and qd are matrices (m,n), each row is interpretted as a joint configuration, and the result (n,n,m) is a 3d-matrix where each plane corresponds to a row ofq
andqd
.- Parameters:
q – Joint coordinates
qd – Joint velocity
pinv – use pseudo inverse rather than inverse (Default value = False)
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
representation – (Default value = “rpy/xyz”)
J –
Ji –
Jd –
C –
Mx –
- Returns:
Operational space velocity matrix
- Return type:
ndarray(6,6) or ndarray(m,6,6)
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
- Joint viscous friction is also a joint force proportional to
velocity but it is eliminated in the computation of this value.
Computationally slow, involves \(n^2/2\) invocations of RNE.
If the robot is not 6 DOF the
pinv
option is set True.pinv()
is around 5x slower thaninv()
Warning
Assumes that the operational space has 6 DOF.
See also
coriolis()
,inertia_x()
,hessian0()
- property default_backend
Get default graphical backend
robot.default_backend
Get the default graphical backend, used whenno explicit backend is passed to
Robot.plot
.
robot.default_backend = ...
Set the default graphical backend, used whenno explicit backend is passed to
Robot.plot
. The default set here will be overridden if the particularRobot
subclass cannot support it.
- Returns:
backend name
- Return type:
default_backend
- dfs_links(start, func=None)
A link search method
Visit all links from start in depth-first order and will apply func to each visited link
- dotfile(filename, etsbox=False, ets='full', jtype=False, static=True)
Write a link transform graph as a GraphViz dot file
- The file can be processed using dot:
% dot -Tpng -o out.png dotfile.dot
- The nodes are:
Base is shown as a grey square. This is the world frame origin, but can be changed using the
base
attribute of the robot.Link frames are indicated by circles
ETS transforms are indicated by rounded boxes
- The edges are:
an arrow if jtype is False or the joint is fixed
an arrow with a round head if jtype is True and the joint is revolute
an arrow with a box head if jtype is True and the joint is prismatic
Edge labels or nodes in blue have a fixed transformation to the preceding link.
Note
- If
filename
is a file object then the file will not be closed after the GraphViz model is written.
- Parameters:
file – Name of file to write to
etsbox (
bool
) – Put the link ETS in a box, otherwise an edge labelets (
Literal
['full'
,'brief'
]) – Display the full ets with “full” or a brief version with “brief”jtype (
bool
) – Arrowhead to node indicates revolute or prismatic typestatic (
bool
) – Show static joints in blue and bold
See also
- dynamics()
Pretty print the dynamic parameters (Robot superclass)
The dynamic parameters (inertial and friction) are printed in a table, with one row per link.
Examples
- dynamics_list()
Print dynamic parameters (Robot superclass)
Display the kinematic and dynamic parameters to the console in reable format
- dynchanged(what=None)
Dynamic parameters have changed
Called from a property setter to inform the robot that the cache of dynamic parameters is invalid.
See also
roboticstoolbox.Link._listen_dyn()
- ets(start=None, end=None)
Robot to ETS
robot.ets()
is an ETS representing the kinematics from base to end-effector.robot.ets(end=link)
is an ETS representing the kinematics from base to the linklink
specified as a Link reference or a name.robot.ets(start=l1, end=l2)
is an ETS representing the kinematics from linkl1
to linkl2
.:param : :type : param start: start of path, defaults to
base_link
:param : :type : param end: end of path, defaults to end-effector- Raises:
ValueError – a link does not belong to this ERobot
TypeError – a bad link argument
- Returns:
elementary transform sequence
- Return type:
ets
Examples
>>> import roboticstoolbox as rtb >>> panda = rtb.models.ETS.Panda() >>> panda.ets() [ET.tz(eta=0.333), ET.Rz(jindex=0), ET.Rx(eta=-1.5707963267948966), ET.Rz(jindex=1), ET.Rx(eta=1.5707963267948966), ET.tz(eta=0.316), ET.Rz(jindex=2), ET.tx(eta=0.0825), ET.Rx(eta=1.5707963267948966), ET.Rz(jindex=3), ET.tx(eta=-0.0825), ET.Rx(eta=-1.5707963267948966), ET.tz(eta=0.384), ET.Rz(jindex=4), ET.Rx(eta=1.5707963267948966), ET.Rz(jindex=5), ET.tx(eta=0.088), ET.Rx(eta=1.5707963267948966), ET.tz(eta=0.107), ET.Rz(jindex=6), ET.tz(eta=0.10300000000000001), ET.Rz(eta=-0.7853981633974483)]
- fdyn(T, q0, Q=None, Q_args={}, qd0=None, solver='RK45', solver_args={}, dt=None, progress=False)
Integrate forward dynamics
tg = R.fdyn(T, q)
integrates the dynamics of the robot with zero input torques over the time interval 0 toT
and returns the trajectory as a namedtuple with elements:t
the time vector (M,)q
the joint coordinates (M,n)qd
the joint velocities (M,n)
tg = R.fdyn(T, q, torqfun)
as above but the torque applied to the joints is given by the provided function:tau = function(robot, t, q, qd, **args)
where the inputs are:
the robot object
current time
current joint coordinates (n,)
current joint velocity (n,)
args, optional keyword arguments can be specified, these are
passed in from the
targs
kewyword argument.The function must return a Numpy array (n,) of joint forces/torques.
- Parameters:
T (
float
) – integration timeq0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – initial joint coordinatesqd0 (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – initial joint velocities, assumed zero if not givenQ (
Optional
[Callable
[[Any
,float
,ndarray
,ndarray
],ndarray
]]) – a function that computes generalized joint force as a function of time and/or stateQ_args (
Dict
) – positional arguments passed totorque
solver (
str
) – strsolver_args (
Dict
) – dictprogress (
bool
) – show progress bar, default False
- Returns:
robot trajectory
- Return type:
trajectory
Examples
To apply zero joint torque to the robot without Coulomb friction:
>>> def myfunc(robot, t, q, qd): >>> return np.zeros((robot.n,))
>>> tg = robot.nofriction().fdyn(5, q0, myfunc)
>>> plt.figure() >>> plt.plot(tg.t, tg.q) >>> plt.show()
We could also use a lambda function:
>>> tg = robot.nofriction().fdyn( >>> 5, q0, lambda r, t, q, qd: np.zeros((r.n,)))
The robot is controlled by a PD controller. We first define a function to compute the control which has additional parameters for the setpoint and control gains (qstar, P, D):
>>> def myfunc(robot, t, q, qd, qstar, P, D): >>> return (qstar - q) * P + qd * D # P, D are (6,)
>>> tg = robot.fdyn(10, q0, myfunc, torque_args=(qstar, P, D)) )
Many integrators have variable step length which is problematic if we want to animate the result. If
dt
is specified then the solver results are interpolated in time steps ofdt
.Notes
- This function performs poorly with non-linear joint friction,
such as Coulomb friction. The R.nofriction() method can be used to set this friction to zero.
- If the function is not specified then zero force/torque is
applied to the manipulator joints.
- Interpolation is performed using `ScipY integrate.ode
<https://docs.scipy.org/doc/scipy/reference/generated/scipy.integrate.ode.html>`
The SciPy RK45 integrator is used by default
- Interpolation is performed using `SciPy interp1
<https://docs.scipy.org/doc/scipy/reference/generated/scipy.interpolate.interp1d.html>`
See also
DHRobot.accel()
,DHRobot.nofriction()
,DHRobot.rne()
- fellipse(q, opt='trans', unit='rad', centre=[0, 0, 0])
Create a force ellipsoid object for plotting with PyPlot
robot.fellipse(q)
creates a force ellipsoid for the robot at poseq
. The ellipsoid is centered at the origin.- q
The joint configuration of the robot.
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational force ellipsoid
- unit
‘rad’ or ‘deg’ will plot the ellipsoid in radians or degrees
- centre
The centre of the ellipsoid, either ‘ee’ for the end-effector or a 3-vector [x, y, z] in the world frame
- Returns:
An EllipsePlot object
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- friction(qd)
Manipulator joint friction (Robot superclass)
robot.friction(qd)
is a vector of joint friction forces/torques for the robot moving with joint velocitiesqd
.The friction model includes:
Viscous friction which is a linear function of velocity.
Coulomb friction which is proportional to sign(qd).
\[\begin{split}\tau_j = G^2 B \dot{q}_j + |G_j| \left\{ \begin{array}{ll} \tau_{C,j}^+ & \mbox{if $\dot{q}_j > 0$} \\ \tau_{C,j}^- & \mbox{if $\dot{q}_j < 0$} \end{array} \right.\end{split}\]- Parameters:
qd (
ndarray
) – The joint velocities of the robot- Returns:
The joint friction forces/torques for the robot
- Return type:
friction
Notes
- The friction value should be added to the motor output torque to
determine the nett torque. It has a negative value when qd > 0.
- The returned friction value is referred to the output of the
gearbox.
- The friction parameters in the Link object are referred to the
motor.
Motor viscous friction is scaled up by \(G^2\).
Motor Coulomb friction is scaled up by math:G.
- The appropriate Coulomb friction value to use in the
non-symmetric case depends on the sign of the joint velocity, not the motor velocity.
- Coulomb friction is zero for zero joint velocity, stiction is
not modeled.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 robot has negative gear ratio for joints 1 and 3.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 has negative gear ratio for joints 1 and 3.
See also
Robot.nofriction()
,Link.friction()
- get_path(end=None, start=None)
Find a path from start to end
- Parameters:
- Raises:
ValueError – link not known or ambiguous
- Return type:
- Returns:
path – the path from start to end
n – the number of joints in the path
T – the tool transform present after end
- property gravity: ndarray
Get/set default gravitational acceleration (Robot superclass)
robot.name
is the default gravitational accelerationrobot.name = ...
checks and sets default gravitationalacceleration
- Parameters:
gravity – the new gravitational acceleration for this robot
- Returns:
gravitational acceleration
- Return type:
gravity
Notes
If the z-axis is upward, out of the Earth, this should be a positive number.
- gravload(q=None, gravity=None)
Compute gravity load
robot.gravload(q)
calculates the joint gravity loading (n) for the robot in the joint configurationq
and using the default gravitational acceleration specified in the DHRobot object.robot.gravload(q, gravity=g)
as above except the gravitational acceleration is explicitly specified asg
.Trajectory operation
If q is a matrix (nxm) each column is interpreted as a joint configuration vector, and the result is a matrix (nxm) each column being the corresponding joint torques.
- Parameters:
- Returns:
The generalised joint force/torques due to gravity
- Return type:
gravload
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.gravload(puma.qz) array([ 0. , 37.4837, 0.2489, 0. , 0. , 0. ])
- gravload_x(q=None, gravity=None, pinv=False, representation='rpy/xyz', Ji=None)
Operational space gravity load
robot.gravload_x(q)
calculates the gravity wrench for the robot in the joint configurationq
and using the default gravitational acceleration specified in the robot object.robot.gravload_x(q, gravity=g)
as above except the gravitational acceleration is explicitly specified asg
.\[\mathbf{G}_x = \mathbf{J}(q)^{-T} \mathbf{G}(q)\]The transformation to operational space requires an analytical, rather than geometric, Jacobian.
analytical
can be one of:Value
Rotational representation
'rpy/xyz'
RPY angular rates in XYZ order (default)
'rpy/zyx'
RPY angular rates in XYZ order
'eul'
Euler angular rates in ZYZ order
'exp'
exponential coordinate rates
Trajectory operation
If q is a matrix (nxm) each column is interpreted as a joint configuration vector, and the result is a matrix (nxm) each column being the corresponding joint torques.
- Parameters:
q – Joint coordinates
gravity – Gravitational acceleration (Optional, if not supplied will use the
gravity
attribute of self).pinv – use pseudo inverse rather than inverse (Default value = False)
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
representation – (Default value = “rpy/xyz”)
Ji –
- Returns:
The operational space gravity wrench
- Return type:
gravload
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
If the robot is not 6 DOF the
pinv
option is set True.pinv()
is around 5x slower thaninv()
Warning
Assumes that the operational space has 6 DOF.
See also
- property grippers: List[Gripper]
Grippers attached to the robot
- Returns:
A list of grippers
- Return type:
grippers
- property hascollision
Robot has collision model
- Returns:
hascollision – Robot has collision model
At least one link has associated collision model.
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.hascollision False
See also
- property hasdynamics
Robot has dynamic parameters
- Returns:
hasdynamics – Robot has dynamic parameters
At least one link has associated dynamic parameters.
Examples
- property hasgeometry
Robot has geometry model
At least one link has associated mesh to describe its shape.
- Returns:
Robot has geometry model
- Return type:
hasgeometry
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.hasgeometry True
See also
- hierarchy()
Pretty print the robot link hierachy
- Return type:
Pretty print of the robot model
Examples
Makes a robot and prints the heirachy
>>> import roboticstoolbox as rtb >>> robot = rtb.models.URDF.Panda() >>> robot.hierarchy() panda_link0 panda_link1 panda_link2 panda_link3 panda_link4 panda_link5 panda_link6 panda_link7 panda_link8 panda_hand panda_leftfinger panda_rightfinger
- inertia(q)
Manipulator inertia matrix
inertia(q)
is the symmetric joint inertia matrix (n,n) which relates joint torque to joint acceleration for the robot at joint configuration q.Trajectory operation
If
q
is a matrix (m,n), each row is interpretted as a joint state vector, and the result is a 3d-matrix (nxnxk) where each plane corresponds to the inertia for the corresponding row of q.- Parameters:
q (
ndarray
) – Joint coordinates- Returns:
The inertia matrix
- Return type:
inertia
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.inertia(puma.qz) array([[ 3.9611, -0.1627, -0.1389, 0.0016, -0.0004, 0. ], [-0.1627, 4.4566, 0.3727, 0. , 0.0019, 0. ], [-0.1389, 0.3727, 0.9387, 0. , 0.0019, 0. ], [ 0.0016, 0. , 0. , 0.1924, 0. , 0. ], [-0.0004, 0.0019, 0.0019, 0. , 0.1713, 0. ], [ 0. , 0. , 0. , 0. , 0. , 0.1941]])
Notes
- The diagonal elements
M[j,j]
are the inertia seen by joint actuator
j
.
- The diagonal elements
- The off-diagonal elements
M[j,k]
are coupling inertias that relate acceleration on joint
j
to force/torque on jointk
.
- The off-diagonal elements
- The diagonal terms include the motor inertia reflected through
the gear ratio.
See also
- inertia_x(q=None, pinv=False, representation='rpy/xyz', Ji=None)
Operational space inertia matrix
robot.inertia_x(q)
is the operational space (Cartesian) inertia matrix which relates Cartesian force/torque to Cartesian acceleration at the joint configuration q.\[\mathbf{M}_x = \mathbf{J}(q)^{-T} \mathbf{M}(q) \mathbf{J}(q)^{-1}\]The transformation to operational space requires an analytical, rather than geometric, Jacobian.
analytical
can be one of:Value
Rotational representation
'rpy/xyz'
RPY angular rates in XYZ order (default)
'rpy/zyx'
RPY angular rates in XYZ order
'eul'
Euler angular rates in ZYZ order
'exp'
exponential coordinate rates
Trajectory operation
If
q
is a matrix (m,n), each row is interpretted as a joint state vector, and the result is a 3d-matrix (m,n,n) where each plane corresponds to the Cartesian inertia for the corresponding row ofq
.- Parameters:
q – Joint coordinates
pinv – use pseudo inverse rather than inverse (Default value = False)
analytical – the type of analytical Jacobian to use, default is ‘rpy/xyz’
representation – (Default value = “rpy/xyz”)
Ji – The inverse analytical Jacobian (base-frame)
- Returns:
The operational space inertia matrix
- Return type:
inertia_x
Examples
ainv = _umath_linalg.inv(a, signature=signature, extobj=extobj) File "/opt/hostedtoolcache/Python/3.7.17/x64/lib/python3.7/site-packages/numpy/linalg/linalg.py", line 88, in _raise_linalgerror_singular raise LinAlgError("Singular matrix") numpy.linalg.LinAlgError: Singular matrix
Notes
If the robot is not 6 DOF the
pinv
option is set True.pinv()
is around 5x slower thaninv()
Warning
Assumes that the operational space has 6 DOF.
See also
- isprismatic(j)
Check if joint is prismatic
- Returns:
True if prismatic
- Return type:
j
Examples
See also
Link.isprismatic()
,prismaticjoints()
- isrevolute(j)
Check if joint is revolute
- Returns:
True if revolute
- Return type:
j
Examples
See also
Link.isrevolute()
,revolutejoints()
- itorque(q, qdd)
Inertia torque
itorque(q, qdd)
is the inertia force/torque vector (n) at the specified joint configuration q (n) and acceleration qdd (n), andn
is the number of robot joints. It is \(\mathbf{I}(q) \ddot{q}\).Trajectory operation
If
q
andqdd
are matrices (m,n), each row is interpretted as a joint configuration, and the result is a matrix (m,n) where each row is the corresponding joint torques.- Parameters:
q – Joint coordinates
qdd – Joint acceleration
- Returns:
The inertia torque vector
- Return type:
itorque
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.itorque(puma.qz, 0.5 * np.ones((6,))) array([1.8304, 2.3343, 0.5872, 0.0971, 0.0873, 0.0971])
Notes
- If the robot model contains non-zero motor inertia then this
will be included in the result.
See also
- jointdynamics(q, qd=None)
Transfer function of joint actuator
tf = jointdynamics(qd, q)
calculates a vector of n continuous-time transfer functions that represent the transfer function 1/(Js+B) for each joint based on the dynamic parameters of the robot and the configuration q (n). n is the number of robot joints. The result is a list of tuples (J, B) for each joint.tf = jointdynamics(q, qd)
as above but include the linearized effects of Coulomb friction when operating at joint velocity QD (1xN).- Parameters:
q – Joint coordinates
qd – Joint velocity
- Returns:
transfer function denominators
- Return type:
list of 2-tuples
- linkcolormap(linkcolors='viridis')
Create a colormap for robot joints
cm = robot.linkcolormap()
is an n-element colormap that gives a unique color for every link. The RGBA colors for linkj
arecm(j)
.cm = robot.linkcolormap(cmap)
as above butcmap
is the name of a valid matplotlib colormap. The default, example above, is theviridis
colormap.cm = robot.linkcolormap(list of colors)
as above but a colormap is created from a list of n color names given as strings, tuples or hexstrings.
- Parameters:
linkcolors (
Union
[List
[Any
],str
]) – list of colors or colormap, defaults to “viridis”- Returns:
the color map
- Return type:
color map
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> cm = robot.linkcolormap("inferno") >>> print(cm(range(6))) # cm(i) is 3rd color in colormap [[0.0015 0.0005 0.0139 1. ] [0.2582 0.0386 0.4065 1. ] [0.5783 0.148 0.4044 1. ] [0.865 0.3168 0.2261 1. ] [0.9876 0.6453 0.0399 1. ] [0.9884 0.9984 0.6449 1. ]] >>> cm = robot.linkcolormap( ... ['red', 'g', (0,0.5,0), '#0f8040', 'yellow', 'cyan']) >>> print(cm(range(6))) [[1. 0. 0. 1. ] [0. 0.5 0. 1. ] [0. 0.5 0. 1. ] [0.0588 0.502 0.251 1. ] [1. 1. 0. 1. ] [0. 1. 1. 1. ]]
Notes
Colormaps have 4-elements: red, green, blue, alpha (RGBA)
Names of supported colors and colormaps are defined in the matplotlib documentation.
- property links: List[LinkType]
Robot links
- Returns:
A list of link objects
- Return type:
links
Notes
It is probably more concise to index the robot object rather than the list of links, ie. the following are equivalent: -
robot.links[i]
-robot[i]
- property manufacturer
Get/set robot manufacturer’s name
robot.manufacturer
is the robot manufacturer’s namerobot.manufacturer = ...
checks and sets the manufacturer’s name
- Returns:
robot manufacturer’s name
- Return type:
manufacturer
- property n: int
Number of joints
- Returns:
Number of joints
- Return type:
n
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.n 6
See also
- property name: str
Get/set robot name
robot.name
is the robot namerobot.name = ...
checks and sets the robot name
- Parameters:
name – the new robot name
- Returns:
the current robot name
- Return type:
name
- property nbranches: int
Number of branches
Number of branches in this robot. Computed as the number of links with zero children
- Returns:
number of branches in the robot’s kinematic tree
- Return type:
nbranches
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.ETS.Panda() >>> robot.nbranches 1
- property nlinks
Number of links
The returned number is the total of both variable joints and static links
- Returns:
Number of links
- Return type:
nlinks
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.nlinks 6
See also
- nofriction(coulomb=True, viscous=False)
Remove manipulator joint friction
nofriction()
copies the robot and returns a robot with the same link parameters except the Coulomb and/or viscous friction parameter are set to zero.- Parameters:
- Returns:
A copy of the robot with dynamic parameters perturbed
- Return type:
robot
See also
Robot.friction()
,Link.nofriction()
- pay(W, q=None, J=None, frame=1)
Generalised joint force/torque due to a payload wrench
tau = pay(W, J) Returns the generalised joint force/torques due to a payload wrench W applied to the end-effector. Where the manipulator Jacobian is J (6xn), and n is the number of robot joints.
tau = pay(W, q, frame) as above but the Jacobian is calculated at pose q in the frame given by frame which is 0 for base frame, 1 for end-effector frame.
Uses the formula tau = J’W, where W is a wrench vector applied at the end effector, W = [Fx Fy Fz Mx My Mz]’.
- Trajectory operation:
In the case q is nxm or J is 6xnxm then tau is nxm where each row is the generalised force/torque at the pose given by corresponding row of q.
- Parameters:
W (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – A wrench vector applied at the end effector, W = [Fx Fy Fz Mx My Mz]J (
Optional
[ndarray
]) – The manipulator Jacobian (Optional, if not supplied will use the q value).frame (
int
) – The frame in which to torques are expressed in when J is not supplied. 0 means base frame of the robot, 1 means end- effector frame
- Returns:
Joint forces/torques due to w
- Return type:
t
Notes
- Wrench vector and Jacobian must be from the same reference
frame.
Tool transforms are taken into consideration when frame=1.
- Must have a constant wrench - no trajectory support for this
yet.
- paycap(w, tauR, frame=1, q=None)
Static payload capacity of a robot
wmax, joint = paycap(q, w, f, tauR)
returns the maximum permissible payload wrenchwmax
(6) applied at the end-effector, and the index of the joint (zero indexed) which hits its force/torque limit at that wrench.q
(n) is the manipulator pose,w
the payload wrench (6),f
the wrench reference frame and tauR (nx2) is a matrix of joint forces/torques (first col is maximum, second col minimum).Trajectory operation:
In the case q is nxm then wmax is Mx6 and J is Mx1 where the rows are the results at the pose given by corresponding row of q.
- Parameters:
w (
ndarray
) – The payload wrenchtauR (
ndarray
) – Joint torque matrix minimum and maximumsframe (
int
) – The frame in which to torques are expressed in when J is not supplied. ‘base’ means base frame of the robot, ‘ee’ means end-effector frameq (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – Joint coordinates
- Returns:
The maximum permissible payload wrench
- Return type:
ndarray(6)
Notes
Wrench vector and Jacobian must be from the same reference frame
Tool transforms are taken into consideration for frame=1.
- payload(m, p=array([0.0, 0.0, 0.0]))
Add a payload to the end-effector
payload(m, p) adds payload mass adds a payload with point mass m at position p in the end-effector coordinate frame.
payload(m) adds payload mass adds a payload with point mass m at in the end-effector coordinate frame.
payload(0) removes added payload.
- Parameters:
m (
float
) – mass (kg)p – position in end-effector frame
- perturb(p=0.1)
Perturb robot parameters
rp = perturb(p) is a new robot object in which the dynamic parameters (link mass and inertia) have been perturbed. The perturbation is multiplicative so that values are multiplied by random numbers in the interval (1-p) to (1+p). The name string of the perturbed robot is prefixed by ‘P/’.
Useful for investigating the robustness of various model-based control schemes. For example to vary parameters in the range +/- 10 percent is: r2 = puma.perturb(0.1)
- Parameters:
p – The percent (+/-) to be perturbed. Default 10%
- Returns:
A copy of the robot with dynamic parameters perturbed
- Return type:
- plot(q, backend=None, block=False, dt=0.05, limits=None, vellipse=False, fellipse=False, fig=None, movie=None, loop=False, **kwargs)
Graphical display and animation
robot.plot(q, 'pyplot')
displays a graphical view of a robot based on the kinematic model and the joint configurationq
. This is a stick figure polyline which joins the origins of the link coordinate frames. The plot will autoscale with an aspect ratio of 1.If
q
(m,n) representing a joint-space trajectory it will create an animation with a pause ofdt
seconds between each frame.- q
The joint configuration of the robot.
- backend
The graphical backend to use, currently ‘swift’ and ‘pyplot’ are implemented. Defaults to ‘swift’ of a
Robot
and ‘pyplot` for aDHRobot
- block
Block operation of the code and keep the figure open
- dt
if q is a trajectory, this describes the delay in seconds between frames
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2] (this option is for ‘pyplot’ only)
- vellipse
(Plot Option) Plot the velocity ellipse at the end-effector (this option is for ‘pyplot’ only)
- fellipse
(Plot Option) Plot the force ellipse at the end-effector (this option is for ‘pyplot’ only)
- fig
(Plot Option) The figure label to plot in (this option is for ‘pyplot’ only)
- movie
(Plot Option) The filename to save the movie to (this option is for ‘pyplot’ only)
- loop
(Plot Option) Loop the movie (this option is for ‘pyplot’ only)
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint) (this option is for ‘pyplot’ only)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes. (this option is for ‘pyplot’ only)
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane. (this option is for ‘pyplot’ only)
- name
(Plot Option) Plot the name of the robot near its base (this option is for ‘pyplot’ only)
- Returns:
A reference to the environment object which controls the figure
- Return type:
env
Notes
- By default this method will block until the figure is dismissed.
To avoid this set
block=False
.
- For PyPlot, the polyline joins the origins of the link frames,
but for some Denavit-Hartenberg models those frames may not actually be on the robot, ie. the lines to not neccessarily represent the links of the robot.
See also
- plot_ellipse(ellipse, block=True, limits=None, jointaxes=True, eeframe=True, shadow=True, name=True)
Plot the an ellipsoid
robot.plot_ellipse(ellipsoid)
displays the ellipsoid.- ellipse
the ellipsoid to plot
- block
Block operation of the code and keep the figure open
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes.
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane
- name
(Plot Option) Plot the name of the robot near its base
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
- plot_fellipse(q, block=True, fellipse=None, limits=None, opt='trans', centre=[0, 0, 0], jointaxes=True, eeframe=True, shadow=True, name=True)
Plot the force ellipsoid for manipulator
robot.plot_fellipse(q)
displays the velocity ellipsoid for the robot at poseq
. The plot will autoscale with an aspect ratio of 1.robot.plot_fellipse(vellipse)
specifies a custon ellipse to plot.- q
The joint configuration of the robot
- block
Block operation of the code and keep the figure open
- fellipse
the vellocity ellipsoid to plot
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational force ellipsoid
- centre
The coordinates to plot the fellipse [x, y, z] or “ee” to plot at the end-effector location
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes.
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane
- name
(Plot Option) Plot the name of the robot near its base
- Raises:
ValueError – q or fellipse must be supplied
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- plot_vellipse(q, block=True, vellipse=None, limits=None, opt='trans', centre=[0, 0, 0], jointaxes=True, eeframe=True, shadow=True, name=True)
Plot the velocity ellipsoid for manipulator
robot.plot_vellipse(q)
displays the velocity ellipsoid for the robot at poseq
. The plot will autoscale with an aspect ratio of 1.robot.plot_vellipse(vellipse)
specifies a custon ellipse to plot.- block
Block operation of the code and keep the figure open
- q
The joint configuration of the robot
- vellipse
the vellocity ellipsoid to plot
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational velocity ellipsoid
- centre
The coordinates to plot the vellipse [x, y, z] or “ee” to plot at the end-effector location
- jointaxes
(Plot Option) Plot an arrow indicating the axes in which the joint revolves around(revolute joint) or translates along (prosmatic joint)
- eeframe
(Plot Option) Plot the end-effector coordinate frame at the location of the end-effector. Uses three arrows, red, green and blue to indicate the x, y, and z-axes.
- shadow
(Plot Option) Plot a shadow of the robot in the x-y plane
- name
(Plot Option) Plot the name of the robot near its base
- Raises:
ValueError – q or fellipse must be supplied
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- property prismaticjoints: List[bool]
Revolute joints as bool array
- Returns:
array of joint type, True if prismatic
- Return type:
prismaticjoints
Examples
Notes
Fixed joints, that maintain a constant link relative pose, are not included.
See also
Link.isprismatic()
,revolutejoints()
- property q: ndarray
Get/set robot joint configuration
robot.q
is the robot joint configurationrobot.q = ...
checks and sets the joint configuration
- Parameters:
q – the new robot joint configuration
- Returns:
robot joint configuration
- Return type:
q
- property qd: ndarray
Get/set robot joint velocity
robot.qd
is the robot joint velocityrobot.qd = ...
checks and sets the joint velocity
- Returns:
robot joint velocity
- Return type:
qd
- property qdd: ndarray
Get/set robot joint acceleration
robot.qdd
is the robot joint accelerationrobot.qdd = ...
checks and sets the robot joint acceleration
- Returns:
robot joint acceleration
- Return type:
qdd
- property qlim: ndarray
Joint limits
Limits are extracted from the link objects. If joints limits are not set for:
a revolute joint [-𝜋. 𝜋] is returned
a prismatic joint an exception is raised
- qlim
An array of joints limits (2, n)
- Raises:
ValueError – unset limits for a prismatic joint
- Returns:
Array of joint limit values
- Return type:
qlim
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot.qlim array([[-2.7925, -1.9199, -2.3562, -4.6426, -1.7453, -4.6426], [ 2.7925, 1.9199, 2.3562, 4.6426, 1.7453, 4.6426]])
- random_q()
Return a random joint configuration
The value for each joint is uniform randomly distributed between the limits set for the robot.
Note
The joint limit for all joints must be set.
- Returns:
Random joint configuration :rtype: ndarray(n)
- Return type:
q
See also
Robot.qlim()
,Link.qlim()
- property revolutejoints: List[bool]
Revolute joints as bool array
- Returns:
array of joint type, True if revolute
- Return type:
revolutejoints
Examples
Notes
Fixed joints, that maintain a constant link relative pose, are not included.
See also
Link.isrevolute()
,prismaticjoints()
- segments()
Segments of branched robot
For a single-chain robot with structure:
L1 - L2 - L3
the return is
[[None, L1, L2, L3]]
For a robot with structure:
L1 - L2 +- L3 - L4 +- L5 - L6
the return is
[[None, L1, L2], [L2, L3, L4], [L2, L5, L6]]
- Returns:
Segment list
- Return type:
segments
Notes
the length of the list is the number of segments in the robot
- the first segment always starts with
None
which represents the base transform (since there is no base link)
- the first segment always starts with
- the last link of one segment is also the first link of subsequent
segments
- showgraph(display_graph=True, **kwargs)
Display a link transform graph in browser
robot.showgraph()
displays a graph of the robot’s link frames and the ETS between them. It uses GraphViz dot.- The nodes are:
Base is shown as a grey square. This is the world frame origin, but can be changed using the
base
attribute of the robot.Link frames are indicated by circles
ETS transforms are indicated by rounded boxes
- The edges are:
an arrow if jtype is False or the joint is fixed
an arrow with a round head if jtype is True and the joint is revolute
an arrow with a box head if jtype is True and the joint is prismatic
Edge labels or nodes in blue have a fixed transformation to the preceding link.
- Parameters:
display_graph (
bool
) – Open the graph in a browser if True. Otherwise will return the file pathetsbox – Put the link ETS in a box, otherwise an edge label
jtype – Arrowhead to node indicates revolute or prismatic type
static – Show static joints in blue and bold
- Return type:
Examples
>>> import roboticstoolbox as rtb >>> panda = rtb.models.URDF.Panda() >>> panda.showgraph()
See also
- property structure: str
Return the joint structure string
A string with one letter per joint:
R
for a revolute joint, andP
for a prismatic joint.- Returns:
joint configuration string
- Return type:
structure
Examples
>>> import roboticstoolbox as rtb >>> puma = rtb.models.DH.Puma560() >>> puma.structure 'RRRRRR' >>> stanford = rtb.models.DH.Stanford() >>> stanford.structure 'RRPRRR'
Notes
Fixed joints, that maintain a constant link relative pose, are not included.
len(self.structure) == self.n
.
- teach(q, block=True, limits=None, vellipse=False, fellipse=False, backend=None)
Graphical teach pendant
robot.teach(q)
creates a matplotlib plot which allows the user to “drive” a graphical robot using a graphical slider panel. The robot’s inital joint configuration isq
. The plot will autoscale with an aspect ratio of 1.robot.teach()
as above except the robot’s stored value ofq
is used.- q
The joint configuration of the robot (Optional, if not supplied will use the stored q values).
- block
Block operation of the code and keep the figure open
- limits
Custom view limits for the plot. If not supplied will autoscale, [x1, x2, y1, y2, z1, z2]
- vellipse
(Plot Option) Plot the velocity ellipse at the end-effector (this option is for ‘pyplot’ only)
- fellipse
(Plot Option) Plot the force ellipse at the end-effector (this option is for ‘pyplot’ only)
- Returns:
A reference to the PyPlot object which controls the matplotlib figure
- Return type:
env
Notes
- Program execution is blocked until the teach window is
dismissed. If
block=False
the method is non-blocking but you need to poll the window manager to ensure that the window remains responsive.
- The slider limits are derived from the joint limit properties.
If not set then: - For revolute joints they are assumed to be [-pi, +pi] - For prismatic joint they are assumed unknown and an error
occurs.
- todegrees(q)
Convert joint angles to degrees
- Parameters:
q – The joint configuration of the robot
- Return type:
- Returns:
q – a vector of joint coordinates in degrees and metres
robot.todegrees(q)
converts joint coordinatesq
to degreestaking into account whether elements of
q
correspond to revoluteor prismatic joints, ie. prismatic joint values are not converted.
If
q
is a matrix, with one column per joint, the conversion isperformed columnwise.
Examples
>>> import roboticstoolbox as rtb >>> from math import pi >>> stanford = rtb.models.DH.Stanford() >>> stanford.todegrees([pi/4, pi/8, 2, -pi/4, pi/6, pi/3]) array([ 45. , 22.5, 2. , -45. , 30. , 60. ])
- property tool: SE3
Get/set robot tool transform
robot.tool
is the robot tool transform as an SE3 objectrobot._tool
is the robot tool transform as a numpy arrayrobot.tool = ...
checks and sets the robot tool transform
- Parameters:
tool – the new robot tool transform (as an SE(3))
- Returns:
robot tool transform
- Return type:
tool
- toradians(q)
Convert joint angles to radians
robot.toradians(q)
converts joint coordinatesq
to radians taking into account whether elements ofq
correspond to revolute or prismatic joints, ie. prismatic joint values are not converted.If
q
is a matrix, with one column per joint, the conversion is performed columnwise.- Parameters:
q – The joint configuration of the robot
- Returns:
a vector of joint coordinates in radians and metres
- Return type:
q
Examples
>>> import roboticstoolbox as rtb >>> stanford = rtb.models.DH.Stanford() >>> stanford.toradians([10, 20, 2, 30, 40, 50]) array([0.1745, 0.3491, 2. , 0.5236, 0.6981, 0.8727])
- vellipse(q, opt='trans', unit='rad', centre=[0, 0, 0], scale=0.1)
Create a velocity ellipsoid object for plotting with PyPlot
robot.vellipse(q)
creates a force ellipsoid for the robot at poseq
. The ellipsoid is centered at the origin.- q
The joint configuration of the robot.
- opt
‘trans’ or ‘rot’ will plot either the translational or rotational force ellipsoid
- unit
‘rad’ or ‘deg’ will plot the ellipsoid in radians or degrees
- centre
The centre of the ellipsoid, either ‘ee’ for the end-effector or a 3-vector [x, y, z] in the world frame
- scale
The scale factor for the ellipsoid
- Returns:
An EllipsePlot object
- Return type:
env
Notes
- By default the ellipsoid related to translational motion is
drawn. Use
opt='rot'
to draw the rotational velocity ellipsoid.
- By default the ellipsoid is drawn at the origin. The option
centre
allows its origin to set to set to the specified 3-vector, or the string “ee” ensures it is drawn at the end-effector position.
- property base: SE2
Get/set robot base transform (Robot superclass)
robot.base
is the robot base transform- Returns:
base – robot tool transform
robot.base = ...
checks and sets the robot base transform
Notes
- The private attribute
_base
will be None in the case of no base transform, but this property will return
SE3()
which is an identity matrix.
- The private attribute
- property reach: float
Reach of the robot
A conservative estimate of the reach of the robot. It is computed as the sum of the translational ETs that define the link transform.
Note
Computed on the first access. If kinematic parameters subsequently change this will not be reflected.
- Returns:
Maximum reach of the robot
- Return type:
reach
Notes
Probably an overestimate of reach
Used by numerical inverse kinematics to scale translational error.
For a prismatic joint, uses
qlim
if it is set
- fkine_all(q)[source]
Compute the pose of every link frame
T = robot.fkine_all(q)
is an SE3 instance withrobot.nlinks + 1
values:T[0]
is the base transformT[i]
is the pose of link whosenumber
isi
- Parameters:
q (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
]]) – The joint configuration- Returns:
Pose of all links
- Return type:
fkine_all
References
J. Haviland, and P. Corke. “Manipulator Differential Kinematics Part I: Kinematics, Velocity, and Applications.” arXiv preprint arXiv:2207.01796 (2022).
Kinematic cache
Link
The ERobot
is defined by a tree of ELink
subclass objects.
- class roboticstoolbox.robot.Link.BaseLink(ets=[], name=None, parent=None, joint_name=None, m=None, r=None, I=None, Jm=None, B=None, Tc=None, G=None, qlim=None, geometry=[], collision=[], **kwargs)[source]
Bases:
SceneNode
,ABC
An abstract link superclass for all link types.
- Parameters:
ets (
Union
[ETS
,ETS2
,ET
,ET2
]) – kinematic - The elementary transforms which make up the linkname – name of the link
parent (
Union
[Self
,str
,None
]) – a reference to the parent link in the kinematic chainr (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – dynamic - position of COM with respect to link frameI (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – dynamic - inertia of link with respect to COMTc (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – dynamic - motor Coulomb friction [Tc⁺, Tc⁻]qlim (
Union
[ndarray
,List
[float
],Tuple
[float
],Set
[float
],None
]) – joint variable limits [min, max]geometry (
List
[Shape
]) – the visual geometry which represents the link. This is used to display the link in Swiftcollision (
List
[Shape
]) – the collision geometry which represents the link in collision checkers
Synopsis
It holds metadata related to:
a robot link, such as rigid-body inertial parameters defined in the link frame, and link name
a robot joint, that connects this link to its parent, such as joint limits, direction of motion, motor and transmission parameters.
Notes
- For a more sophisticated actuator model use the
actuator
attribute which is not initialized or used by this Toolbox.
- For a more sophisticated actuator model use the
There is no ability to name a joint as supported by URDF
- property Ts: Optional[ndarray]
Constant part of link ETS
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the constant part. If no constant part is given, this returns an identity matrix.
- Returns:
constant part of link transform
- Return type:
Ts
Examples
>>> from roboticstoolbox import Link, ET >>> link = Link( ET.tz(0.333) * ET.Rx(90, 'deg') * ET.Rz() ) >>> link.Ts array([[ 1. , 0. , 0. , 0. ], [ 0. , 0. , -1. , 0. ], [ 0. , 1. , 0. , 0.333], [ 0. , 0. , 0. , 1. ]]) >>> link = Link( ET.Rz() ) >>> link.Ts
- property ets: ETS
Get/set link ets
link.ets
is the link etslink.ets = ...
checks and sets the link ets
- Parameters:
ets – the new link ets
- Returns:
the current link ets
- Return type:
ets
- __str__()[source]
Pretty prints the ETS Model of the link
Will output angles in degrees
- Returns:
pretty print of the robot link
- Return type:
- copy()[source]
Copy of link object
link.copy()
is a new Link subclass instance with a copy of all the parameters.- Returns:
copy of link object
- Return type:
link
- property v
Variable part of link ETS
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the latter.
- Returns:
joint variable transform
- Return type:
v
Examples
- property name: str
Get/set link name
link.name
is the link namelink.name = ...
checks and sets the link name
- Returns:
link name
- Return type:
name
- property robot: Optional[BaseRobot]
Get forward reference to the robot which owns this link
link.robot
is the robot referencelink.robot = ...
checks and sets the robot reference
- Returns:
The robot object
- Return type:
robot
- property qlim: Optional[ndarray]
Get/set joint limits
link.qlim
is the joint limitslink.qlim = ...
checks and sets the joint limits
- Returns:
joint limits
- Return type:
qlim
Notes
The limits are not widely enforced within the toolbox.
If no joint limits are specified the value is
None
See also
- property hasdynamics: bool
Link has dynamic parameters (Link superclass)
Link has some assigned (non-default) dynamic parameters. These could have been assigned:
at constructor time, eg.
m=1.2
by invoking a setter method, eg.
link.m = 1.2
- Returns:
Link has dynamic parameters
- Return type:
hasdynamics
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot[1].hasdynamics True
- property isflip: bool
Get/set joint flip
link.flip
is the joint flip statuslink.flip = ...
checks and sets the joint flip status
Joint flip defines the direction of motion of the joint.
flip = False
is conventional motion direction:revolute motion is a positive rotation about the z-axis
prismatic motion is a positive translation along the z-axis
flip = True
is the opposite motion direction:revolute motion is a negative rotation about the z-axis
prismatic motion is a negative translation along the z-axis
- Returns:
joint flip
- Return type:
isflip
- property m: float
Get/set link mass
link.m
is the link masslink.m = ...
checks and sets the link mass
- Returns:
link mass
- Return type:
m
- property r: ndarray
Get/set link centre of mass
The link centre of mass is a 3-vector defined with respect to the link frame.
link.r
is the link centre of masslink.r = ...
checks and sets the link centre of mass
- Returns:
link centre of mass
- Return type:
r
- property I: ndarray
Get/set link inertia
Link inertia is a symmetric 3x3 matrix describing the inertia with respect to a frame with its origin at the centre of mass, and with axes parallel to those of the link frame.
link.I
is the link inertialink.I = ...
checks and sets the link inertia
- Returns:
link inertia
- Return type:
I
Synopsis
The inertia matrix is
\(\begin{bmatrix} I_{xx} & I_{xy} & I_{xz} \\ I_{xy} & I_{yy} & I_{yz} \\I_{xz} & I_{yz} & I_{zz} \end{bmatrix}\)
and can be specified as either:
a 3 ⨉ 3 symmetric matrix
a 3-vector \((I_{xx}, I_{yy}, I_{zz})\)
a 6-vector \((I_{xx}, I_{yy}, I_{zz}, I_{xy}, I_{yz}, I_{xz})\)
Notes
Referred to the link side of the gearbox.
- property Jm: float
Get/set motor inertia
link.Jm
is the motor inertialink.Jm = ...
checks and sets the motor inertia
- Returns:
motor inertia
- Return type:
Jm
Notes
Referred to the motor side of the gearbox.
- property B: float
Get/set motor viscous friction
link.B
is the motor viscous frictionlink.B = ...
checks and sets the motor viscous friction
- Returns:
motor viscous friction
- Return type:
B
Notes
Referred to the motor side of the gearbox.
Viscous friction is the same for positive and negative motion.
- property Tc: ndarray
Get/set motor Coulomb friction
link.Tc
is the motor Coulomb frictionlink.Tc = ...
checks and sets the motor Coulomb friction. If a scalar is given the value is set to [T, -T], if a 2-vector it is assumed to be in the order [Tc⁺, Tc⁻]
Coulomb friction is a non-linear friction effect defined by two parameters such that
\[\begin{split}\tau = \left\{ \begin{array}{ll} \tau_C^+ & \mbox{if $\dot{q} > 0$} \\ \tau_C^- & \mbox{if $\dot{q} < 0$} \end{array} \right.\end{split}\]- Returns:
motor Coulomb friction
- Return type:
Tc
Notes
Referred to the motor side of the gearbox.
- \(\tau_C^+\) must be \(> 0\), and \(\tau_C^-\) must
be \(< 0\).
- property G: float
Get/set gear ratio
link.G
is the transmission gear ratiolink.G = ...
checks and sets the gear ratio
- Returns:
gear ratio
- Return type:
G
Notes
The ratio of motor motion : link motion
The gear ratio can be negative, see also the
flip
attribute.
See also
flip()
- attach(object)
- attach_to(object)
- property collision: SceneGroup
Get/set joint collision geometry
The collision geometries are what is used to check for collisions.
link.collision
is the list of the collision geometries whichrepresent the collidable shape of the link. :return: the collision geometries :rtype: list of Shape
link.collision = ...
checks and sets the collision geometrylink.collision.append(...)
add collision geometry
- property geometry: SceneGroup
Get/set joint visual geometry
link.geometry
is the list of the visual geometries whichrepresent the shape of the link :return: the visual geometries :rtype: list of Shape
link.geometry = ...
checks and sets the geometrylink.geometry.append(...)
add geometry
- property isjoint: bool
Test if link has joint
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the whether the Link contains the variable transform.
- Returns:
test if link has a joint
- Return type:
isjoint
Examples
>>> from roboticstoolbox import models >>> robot = models.URDF.Panda() >>> robot[1].isjoint # link with joint True >>> robot[8].isjoint # static link False
- property jindex: Union[None, int]
Get/set joint index
link.jindex
is the joint indexlink.jindex = ...
checks and sets the joint index
For a serial-link manipulator the joints are numbered starting at zero and increasing sequentially toward the end-effector. For branched mechanisms this is not so straightforward. The link’s
jindex
property specifies the index of its joint variable within a vector of joint coordinates.- Returns:
joint index
- Return type:
jindex
Notes
jindex
values must be a sequence of integers startingat zero.
- property isprismatic: bool
Checks if the joint is of prismatic type
- Returns:
return: True if is prismatic
rtype: bool
- property isrevolute: bool
Checks if the joint is of revolute type
- Returns:
True if is revolute
- Return type:
isrevolute
- property parent: Optional[Self]
Parent link
This is a reference to the links parent in the kinematic chain
- Returns:
Link’s parent
- Return type:
parent
Examples
>>> from roboticstoolbox import models >>> robot = models.URDF.Panda() >>> robot[0].parent # base link has no parent >>> robot[1].parent # second link's parent Link(name = "panda_link0")
- property parent_name: Optional[str]
Parent link name
- Returns:
Link’s parent name
- Return type:
parent_name
- property children: Optional[List[Link]]
List of child links
The list will be empty for a end-effector link
- Returns:
child links
- Return type:
children
- property nchildren: int
Number of child links
Will be zero for an end-effector link
- Returns:
number of child links
- Return type:
nchildren
- closest_point(shape, inf_dist=1.0, skip=False)[source]
Finds the closest point to a shape
closest_point(shape, inf_dist) returns the minimum euclidean distance between this link and shape, provided it is less than inf_dist. It will also return the points on self and shape in the world frame which connect the line of length distance between the shapes. If the distance is negative then the shapes are collided.
:param : :type : param shape: The shape to compare distance to :param : the shape :type : param inf_dist: The minimum distance within which to consider :param : :type : param skip: Skip setting all shape transforms
- iscollided(shape, skip=False)[source]
Checks for collision with a shape
iscollided(shape)
checks if this link and shape have collided- Parameters:
shape (
Shape
) – The shape to compare distance toskip (
bool
) – Skip setting all shape transforms
- Returns:
True if shapes have collided
- Return type:
iscollided
- collided(shape, skip=False)[source]
Checks for collision with a shape
iscollided(shape)
checks if this link and shape have collided- Parameters:
shape (
Shape
) – The shape to compare distance toskip (
bool
) – Skip setting all shape transforms
- Returns:
True if shapes have collided
- Return type:
iscollided
- dyn(indent=0)[source]
Inertial properties of link as a string
link.dyn()
is a string representation the inertial properties of the link object in a multi-line format. The properties shown are mass, centre of mass, inertia, friction, gear ratio and motor properties.- Parameters:
indent – indent each line by this many spaces
:param : :type : type indent: int :param : :type : return: The string representation of the link dynamics :param : :type : rtype: string
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> print(robot.links[2]) # kinematic parameters RevoluteDH: θ=q, d=0.15005, a=0.0203, ⍺=-1.5707963267948966 >>> print(robot.links[2].dyn()) # dynamic parameters m = 4.8 r = -0.02 -0.014 0.07 | 0.066 0 0 | I = | 0 0.086 0 | | 0 0 0.013 | Jm = 0.0002 B = 0.0014 Tc = 0.13(+) -0.1(-) G = -54 qlim = -2.4 to 2.4
See also
dyntable()
- islimit(q)[source]
Checks if joint exceeds limit
link.islimit(q)
is True ifq
exceeds the joint limits defined bylink
.- Parameters:
q (
float
) – joint coordinate- Returns:
True if joint is exceeded
- Return type:
islimit
Notes
If no limits are set always return False.
See also
- nofriction(coulomb=True, viscous=False)[source]
Clone link without friction
link.nofriction()
is a copy of the link instance with the same parameters except, the Coulomb and/or viscous friction parameters are set to zero.- Parameters:
Notes
- For simulation it can be useful to remove Couloumb friction
which can cause problems for numerical integration.
- friction(qd, coulomb=True)[source]
Compute joint friction
friction(qd)
is the joint friction force/torque for joint velocityqd
. The friction model includes:Viscous friction which is a linear function of velocity.
Coulomb friction which is proportional to sign(qd).
\[\begin{split}\tau = G^2 B \dot{q} + |G| \left\{ \begin{array}{ll} \tau_C^+ & \mbox{if $\dot{q} > 0$} \\ \tau_C^- & \mbox{if $\dot{q} < 0$} \end{array} \right.\end{split}\]- Parameters:
- Returns:
the friction force/torque
- Return type:
tau
Notes
- The friction value should be added to the motor output torque to
determine the nett torque. It has a negative value when qd > 0.
- The returned friction value is referred to the output of the
gearbox.
- The friction parameters in the Link object are referred to the
motor.
Motor viscous friction is scaled up by \(G^2\).
Motor Coulomb friction is scaled up by math:G.
- The appropriate Coulomb friction value to use in the
non-symmetric case depends on the sign of the joint velocity, not the motor velocity.
- Coulomb friction is zero for zero joint velocity, stiction is
not modeled.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 robot has negative gear ratio for joints 1 and 3.
- class roboticstoolbox.robot.Link.Link(ets=[], jindex=None, **kwargs)[source]
Bases:
BaseLink
ETS link class
The Link object holds all information related to a robot link and can form a serial-connected chain or a rigid-body tree. It inherits from the Link class which provides common functionality such as joint and link such as kinematics parameters, The transform to the next link is given as an ETS with the joint variable, if present, as the last term. This is preprocessed and the object stores: -
Ts
the constant part as a NumPy array, or None -v
a pointer to an ETS object representing the joint variable.or None
- Parameters:
ets (
Union
[ETS
,ET
]) – kinematic - The elementary transforms which make up the linkname – name of the link
parent – a reference to the parent link in the kinematic chain
joint_name – the name of the joint variable
m – dynamic - link mass
r – dynamic - position of COM with respect to link frame
I – dynamic - inertia of link with respect to COM
Jm – dynamic - motor inertia
B – dynamic - motor viscous friction
Tc – dynamic - motor Coulomb friction [Tc⁺, Tc⁻]
G – dynamic - gear ratio
qlim – joint variable limits [min, max]
geometry – the visual geometry which represents the link. This is used to display the link in Swift
collision – the collision geometry which represents the link in collision checkers
See also
Link2
,DHLink
- property B: float
Get/set motor viscous friction
link.B
is the motor viscous frictionlink.B = ...
checks and sets the motor viscous friction
- Returns:
motor viscous friction
- Return type:
B
Notes
Referred to the motor side of the gearbox.
Viscous friction is the same for positive and negative motion.
- property G: float
Get/set gear ratio
link.G
is the transmission gear ratiolink.G = ...
checks and sets the gear ratio
- Returns:
gear ratio
- Return type:
G
Notes
The ratio of motor motion : link motion
The gear ratio can be negative, see also the
flip
attribute.
See also
flip()
- property I: ndarray
Get/set link inertia
Link inertia is a symmetric 3x3 matrix describing the inertia with respect to a frame with its origin at the centre of mass, and with axes parallel to those of the link frame.
link.I
is the link inertialink.I = ...
checks and sets the link inertia
- Returns:
link inertia
- Return type:
I
Synopsis
The inertia matrix is
\(\begin{bmatrix} I_{xx} & I_{xy} & I_{xz} \\ I_{xy} & I_{yy} & I_{yz} \\I_{xz} & I_{yz} & I_{zz} \end{bmatrix}\)
and can be specified as either:
a 3 ⨉ 3 symmetric matrix
a 3-vector \((I_{xx}, I_{yy}, I_{zz})\)
a 6-vector \((I_{xx}, I_{yy}, I_{zz}, I_{xy}, I_{yz}, I_{xz})\)
Notes
Referred to the link side of the gearbox.
- property Jm: float
Get/set motor inertia
link.Jm
is the motor inertialink.Jm = ...
checks and sets the motor inertia
- Returns:
motor inertia
- Return type:
Jm
Notes
Referred to the motor side of the gearbox.
- property Tc: ndarray
Get/set motor Coulomb friction
link.Tc
is the motor Coulomb frictionlink.Tc = ...
checks and sets the motor Coulomb friction. If a scalar is given the value is set to [T, -T], if a 2-vector it is assumed to be in the order [Tc⁺, Tc⁻]
Coulomb friction is a non-linear friction effect defined by two parameters such that
\[\begin{split}\tau = \left\{ \begin{array}{ll} \tau_C^+ & \mbox{if $\dot{q} > 0$} \\ \tau_C^- & \mbox{if $\dot{q} < 0$} \end{array} \right.\end{split}\]- Returns:
motor Coulomb friction
- Return type:
Tc
Notes
Referred to the motor side of the gearbox.
- \(\tau_C^+\) must be \(> 0\), and \(\tau_C^-\) must
be \(< 0\).
- property Ts: Optional[ndarray]
Constant part of link ETS
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the constant part. If no constant part is given, this returns an identity matrix.
- Returns:
constant part of link transform
- Return type:
Ts
Examples
>>> from roboticstoolbox import Link, ET >>> link = Link( ET.tz(0.333) * ET.Rx(90, 'deg') * ET.Rz() ) >>> link.Ts array([[ 1. , 0. , 0. , 0. ], [ 0. , 0. , -1. , 0. ], [ 0. , 1. , 0. , 0.333], [ 0. , 0. , 0. , 1. ]]) >>> link = Link( ET.Rz() ) >>> link.Ts
- __str__()
Pretty prints the ETS Model of the link
Will output angles in degrees
- Returns:
pretty print of the robot link
- Return type:
- attach(object)
- attach_to(object)
- property children: Optional[List[Link]]
List of child links
The list will be empty for a end-effector link
- Returns:
child links
- Return type:
children
- closest_point(shape, inf_dist=1.0, skip=False)
Finds the closest point to a shape
closest_point(shape, inf_dist) returns the minimum euclidean distance between this link and shape, provided it is less than inf_dist. It will also return the points on self and shape in the world frame which connect the line of length distance between the shapes. If the distance is negative then the shapes are collided.
:param : :type : param shape: The shape to compare distance to :param : the shape :type : param inf_dist: The minimum distance within which to consider :param : :type : param skip: Skip setting all shape transforms
- collided(shape, skip=False)
Checks for collision with a shape
iscollided(shape)
checks if this link and shape have collided- Parameters:
shape (
Shape
) – The shape to compare distance toskip (
bool
) – Skip setting all shape transforms
- Returns:
True if shapes have collided
- Return type:
iscollided
- property collision: SceneGroup
Get/set joint collision geometry
The collision geometries are what is used to check for collisions.
link.collision
is the list of the collision geometries whichrepresent the collidable shape of the link. :return: the collision geometries :rtype: list of Shape
link.collision = ...
checks and sets the collision geometrylink.collision.append(...)
add collision geometry
- copy()
Copy of link object
link.copy()
is a new Link subclass instance with a copy of all the parameters.- Returns:
copy of link object
- Return type:
link
- dyn(indent=0)
Inertial properties of link as a string
link.dyn()
is a string representation the inertial properties of the link object in a multi-line format. The properties shown are mass, centre of mass, inertia, friction, gear ratio and motor properties.- Parameters:
indent – indent each line by this many spaces
:param : :type : type indent: int :param : :type : return: The string representation of the link dynamics :param : :type : rtype: string
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> print(robot.links[2]) # kinematic parameters RevoluteDH: θ=q, d=0.15005, a=0.0203, ⍺=-1.5707963267948966 >>> print(robot.links[2].dyn()) # dynamic parameters m = 4.8 r = -0.02 -0.014 0.07 | 0.066 0 0 | I = | 0 0.086 0 | | 0 0 0.013 | Jm = 0.0002 B = 0.0014 Tc = 0.13(+) -0.1(-) G = -54 qlim = -2.4 to 2.4
See also
dyntable()
- property ets: ETS
Get/set link ets
link.ets
is the link etslink.ets = ...
checks and sets the link ets
- Parameters:
ets – the new link ets
- Returns:
the current link ets
- Return type:
ets
- friction(qd, coulomb=True)
Compute joint friction
friction(qd)
is the joint friction force/torque for joint velocityqd
. The friction model includes:Viscous friction which is a linear function of velocity.
Coulomb friction which is proportional to sign(qd).
\[\begin{split}\tau = G^2 B \dot{q} + |G| \left\{ \begin{array}{ll} \tau_C^+ & \mbox{if $\dot{q} > 0$} \\ \tau_C^- & \mbox{if $\dot{q} < 0$} \end{array} \right.\end{split}\]- Parameters:
- Returns:
the friction force/torque
- Return type:
tau
Notes
- The friction value should be added to the motor output torque to
determine the nett torque. It has a negative value when qd > 0.
- The returned friction value is referred to the output of the
gearbox.
- The friction parameters in the Link object are referred to the
motor.
Motor viscous friction is scaled up by \(G^2\).
Motor Coulomb friction is scaled up by math:G.
- The appropriate Coulomb friction value to use in the
non-symmetric case depends on the sign of the joint velocity, not the motor velocity.
- Coulomb friction is zero for zero joint velocity, stiction is
not modeled.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 robot has negative gear ratio for joints 1 and 3.
- property geometry: SceneGroup
Get/set joint visual geometry
link.geometry
is the list of the visual geometries whichrepresent the shape of the link :return: the visual geometries :rtype: list of Shape
link.geometry = ...
checks and sets the geometrylink.geometry.append(...)
add geometry
- property hasdynamics: bool
Link has dynamic parameters (Link superclass)
Link has some assigned (non-default) dynamic parameters. These could have been assigned:
at constructor time, eg.
m=1.2
by invoking a setter method, eg.
link.m = 1.2
- Returns:
Link has dynamic parameters
- Return type:
hasdynamics
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot[1].hasdynamics True
- iscollided(shape, skip=False)
Checks for collision with a shape
iscollided(shape)
checks if this link and shape have collided- Parameters:
shape (
Shape
) – The shape to compare distance toskip (
bool
) – Skip setting all shape transforms
- Returns:
True if shapes have collided
- Return type:
iscollided
- property isflip: bool
Get/set joint flip
link.flip
is the joint flip statuslink.flip = ...
checks and sets the joint flip status
Joint flip defines the direction of motion of the joint.
flip = False
is conventional motion direction:revolute motion is a positive rotation about the z-axis
prismatic motion is a positive translation along the z-axis
flip = True
is the opposite motion direction:revolute motion is a negative rotation about the z-axis
prismatic motion is a negative translation along the z-axis
- Returns:
joint flip
- Return type:
isflip
- property isjoint: bool
Test if link has joint
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the whether the Link contains the variable transform.
- Returns:
test if link has a joint
- Return type:
isjoint
Examples
>>> from roboticstoolbox import models >>> robot = models.URDF.Panda() >>> robot[1].isjoint # link with joint True >>> robot[8].isjoint # static link False
- islimit(q)
Checks if joint exceeds limit
link.islimit(q)
is True ifq
exceeds the joint limits defined bylink
.- Parameters:
q (
float
) – joint coordinate- Returns:
True if joint is exceeded
- Return type:
islimit
Notes
If no limits are set always return False.
See also
- property isprismatic: bool
Checks if the joint is of prismatic type
- Returns:
return: True if is prismatic
rtype: bool
- property isrevolute: bool
Checks if the joint is of revolute type
- Returns:
True if is revolute
- Return type:
isrevolute
- property jindex: Union[None, int]
Get/set joint index
link.jindex
is the joint indexlink.jindex = ...
checks and sets the joint index
For a serial-link manipulator the joints are numbered starting at zero and increasing sequentially toward the end-effector. For branched mechanisms this is not so straightforward. The link’s
jindex
property specifies the index of its joint variable within a vector of joint coordinates.- Returns:
joint index
- Return type:
jindex
Notes
jindex
values must be a sequence of integers startingat zero.
- property m: float
Get/set link mass
link.m
is the link masslink.m = ...
checks and sets the link mass
- Returns:
link mass
- Return type:
m
- property name: str
Get/set link name
link.name
is the link namelink.name = ...
checks and sets the link name
- Returns:
link name
- Return type:
name
- property nchildren: int
Number of child links
Will be zero for an end-effector link
- Returns:
number of child links
- Return type:
nchildren
- nofriction(coulomb=True, viscous=False)
Clone link without friction
link.nofriction()
is a copy of the link instance with the same parameters except, the Coulomb and/or viscous friction parameters are set to zero.- Parameters:
Notes
- For simulation it can be useful to remove Couloumb friction
which can cause problems for numerical integration.
- property parent: Optional[Self]
Parent link
This is a reference to the links parent in the kinematic chain
- Returns:
Link’s parent
- Return type:
parent
Examples
>>> from roboticstoolbox import models >>> robot = models.URDF.Panda() >>> robot[0].parent # base link has no parent >>> robot[1].parent # second link's parent Link(name = "panda_link0")
- property parent_name: Optional[str]
Parent link name
- Returns:
Link’s parent name
- Return type:
parent_name
- property qlim: Optional[ndarray]
Get/set joint limits
link.qlim
is the joint limitslink.qlim = ...
checks and sets the joint limits
- Returns:
joint limits
- Return type:
qlim
Notes
The limits are not widely enforced within the toolbox.
If no joint limits are specified the value is
None
See also
- property r: ndarray
Get/set link centre of mass
The link centre of mass is a 3-vector defined with respect to the link frame.
link.r
is the link centre of masslink.r = ...
checks and sets the link centre of mass
- Returns:
link centre of mass
- Return type:
r
- property robot: Optional[BaseRobot]
Get forward reference to the robot which owns this link
link.robot
is the robot referencelink.robot = ...
checks and sets the robot reference
- Returns:
The robot object
- Return type:
robot
- property v
Variable part of link ETS
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the latter.
- Returns:
joint variable transform
- Return type:
v
Examples
- A(q=0.0)[source]
Link transform matrix
link.A(q)
is an SE(3) matrix that describes the rigid-body transformation from the previous to the current link frame to the next, which depends on the joint coordinateq
.- Parameters:
q (
float
) – Joint coordinate (radians or metres). Not required for links with no variable- Returns:
link frame transformation matrix
- Return type:
T
- class roboticstoolbox.robot.Link.Link2(ets=[], jindex=None, **kwargs)[source]
Bases:
BaseLink
- property B: float
Get/set motor viscous friction
link.B
is the motor viscous frictionlink.B = ...
checks and sets the motor viscous friction
- Returns:
motor viscous friction
- Return type:
B
Notes
Referred to the motor side of the gearbox.
Viscous friction is the same for positive and negative motion.
- property G: float
Get/set gear ratio
link.G
is the transmission gear ratiolink.G = ...
checks and sets the gear ratio
- Returns:
gear ratio
- Return type:
G
Notes
The ratio of motor motion : link motion
The gear ratio can be negative, see also the
flip
attribute.
See also
flip()
- property I: ndarray
Get/set link inertia
Link inertia is a symmetric 3x3 matrix describing the inertia with respect to a frame with its origin at the centre of mass, and with axes parallel to those of the link frame.
link.I
is the link inertialink.I = ...
checks and sets the link inertia
- Returns:
link inertia
- Return type:
I
Synopsis
The inertia matrix is
\(\begin{bmatrix} I_{xx} & I_{xy} & I_{xz} \\ I_{xy} & I_{yy} & I_{yz} \\I_{xz} & I_{yz} & I_{zz} \end{bmatrix}\)
and can be specified as either:
a 3 ⨉ 3 symmetric matrix
a 3-vector \((I_{xx}, I_{yy}, I_{zz})\)
a 6-vector \((I_{xx}, I_{yy}, I_{zz}, I_{xy}, I_{yz}, I_{xz})\)
Notes
Referred to the link side of the gearbox.
- property Jm: float
Get/set motor inertia
link.Jm
is the motor inertialink.Jm = ...
checks and sets the motor inertia
- Returns:
motor inertia
- Return type:
Jm
Notes
Referred to the motor side of the gearbox.
- property Tc: ndarray
Get/set motor Coulomb friction
link.Tc
is the motor Coulomb frictionlink.Tc = ...
checks and sets the motor Coulomb friction. If a scalar is given the value is set to [T, -T], if a 2-vector it is assumed to be in the order [Tc⁺, Tc⁻]
Coulomb friction is a non-linear friction effect defined by two parameters such that
\[\begin{split}\tau = \left\{ \begin{array}{ll} \tau_C^+ & \mbox{if $\dot{q} > 0$} \\ \tau_C^- & \mbox{if $\dot{q} < 0$} \end{array} \right.\end{split}\]- Returns:
motor Coulomb friction
- Return type:
Tc
Notes
Referred to the motor side of the gearbox.
- \(\tau_C^+\) must be \(> 0\), and \(\tau_C^-\) must
be \(< 0\).
- property Ts: Optional[ndarray]
Constant part of link ETS
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the constant part. If no constant part is given, this returns an identity matrix.
- Returns:
constant part of link transform
- Return type:
Ts
Examples
>>> from roboticstoolbox import Link, ET >>> link = Link( ET.tz(0.333) * ET.Rx(90, 'deg') * ET.Rz() ) >>> link.Ts array([[ 1. , 0. , 0. , 0. ], [ 0. , 0. , -1. , 0. ], [ 0. , 1. , 0. , 0.333], [ 0. , 0. , 0. , 1. ]]) >>> link = Link( ET.Rz() ) >>> link.Ts
- __str__()
Pretty prints the ETS Model of the link
Will output angles in degrees
- Returns:
pretty print of the robot link
- Return type:
- attach(object)
- attach_to(object)
- property children: Optional[List[Link]]
List of child links
The list will be empty for a end-effector link
- Returns:
child links
- Return type:
children
- closest_point(shape, inf_dist=1.0, skip=False)
Finds the closest point to a shape
closest_point(shape, inf_dist) returns the minimum euclidean distance between this link and shape, provided it is less than inf_dist. It will also return the points on self and shape in the world frame which connect the line of length distance between the shapes. If the distance is negative then the shapes are collided.
:param : :type : param shape: The shape to compare distance to :param : the shape :type : param inf_dist: The minimum distance within which to consider :param : :type : param skip: Skip setting all shape transforms
- collided(shape, skip=False)
Checks for collision with a shape
iscollided(shape)
checks if this link and shape have collided- Parameters:
shape (
Shape
) – The shape to compare distance toskip (
bool
) – Skip setting all shape transforms
- Returns:
True if shapes have collided
- Return type:
iscollided
- property collision: SceneGroup
Get/set joint collision geometry
The collision geometries are what is used to check for collisions.
link.collision
is the list of the collision geometries whichrepresent the collidable shape of the link. :return: the collision geometries :rtype: list of Shape
link.collision = ...
checks and sets the collision geometrylink.collision.append(...)
add collision geometry
- copy()
Copy of link object
link.copy()
is a new Link subclass instance with a copy of all the parameters.- Returns:
copy of link object
- Return type:
link
- dyn(indent=0)
Inertial properties of link as a string
link.dyn()
is a string representation the inertial properties of the link object in a multi-line format. The properties shown are mass, centre of mass, inertia, friction, gear ratio and motor properties.- Parameters:
indent – indent each line by this many spaces
:param : :type : type indent: int :param : :type : return: The string representation of the link dynamics :param : :type : rtype: string
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> print(robot.links[2]) # kinematic parameters RevoluteDH: θ=q, d=0.15005, a=0.0203, ⍺=-1.5707963267948966 >>> print(robot.links[2].dyn()) # dynamic parameters m = 4.8 r = -0.02 -0.014 0.07 | 0.066 0 0 | I = | 0 0.086 0 | | 0 0 0.013 | Jm = 0.0002 B = 0.0014 Tc = 0.13(+) -0.1(-) G = -54 qlim = -2.4 to 2.4
See also
dyntable()
- property ets: ETS
Get/set link ets
link.ets
is the link etslink.ets = ...
checks and sets the link ets
- Parameters:
ets – the new link ets
- Returns:
the current link ets
- Return type:
ets
- friction(qd, coulomb=True)
Compute joint friction
friction(qd)
is the joint friction force/torque for joint velocityqd
. The friction model includes:Viscous friction which is a linear function of velocity.
Coulomb friction which is proportional to sign(qd).
\[\begin{split}\tau = G^2 B \dot{q} + |G| \left\{ \begin{array}{ll} \tau_C^+ & \mbox{if $\dot{q} > 0$} \\ \tau_C^- & \mbox{if $\dot{q} < 0$} \end{array} \right.\end{split}\]- Parameters:
- Returns:
the friction force/torque
- Return type:
tau
Notes
- The friction value should be added to the motor output torque to
determine the nett torque. It has a negative value when qd > 0.
- The returned friction value is referred to the output of the
gearbox.
- The friction parameters in the Link object are referred to the
motor.
Motor viscous friction is scaled up by \(G^2\).
Motor Coulomb friction is scaled up by math:G.
- The appropriate Coulomb friction value to use in the
non-symmetric case depends on the sign of the joint velocity, not the motor velocity.
- Coulomb friction is zero for zero joint velocity, stiction is
not modeled.
- The absolute value of the gear ratio is used. Negative gear
ratios are tricky: the Puma560 robot has negative gear ratio for joints 1 and 3.
- property geometry: SceneGroup
Get/set joint visual geometry
link.geometry
is the list of the visual geometries whichrepresent the shape of the link :return: the visual geometries :rtype: list of Shape
link.geometry = ...
checks and sets the geometrylink.geometry.append(...)
add geometry
- property hasdynamics: bool
Link has dynamic parameters (Link superclass)
Link has some assigned (non-default) dynamic parameters. These could have been assigned:
at constructor time, eg.
m=1.2
by invoking a setter method, eg.
link.m = 1.2
- Returns:
Link has dynamic parameters
- Return type:
hasdynamics
Examples
>>> import roboticstoolbox as rtb >>> robot = rtb.models.DH.Puma560() >>> robot[1].hasdynamics True
- iscollided(shape, skip=False)
Checks for collision with a shape
iscollided(shape)
checks if this link and shape have collided- Parameters:
shape (
Shape
) – The shape to compare distance toskip (
bool
) – Skip setting all shape transforms
- Returns:
True if shapes have collided
- Return type:
iscollided
- property isflip: bool
Get/set joint flip
link.flip
is the joint flip statuslink.flip = ...
checks and sets the joint flip status
Joint flip defines the direction of motion of the joint.
flip = False
is conventional motion direction:revolute motion is a positive rotation about the z-axis
prismatic motion is a positive translation along the z-axis
flip = True
is the opposite motion direction:revolute motion is a negative rotation about the z-axis
prismatic motion is a negative translation along the z-axis
- Returns:
joint flip
- Return type:
isflip
- property isjoint: bool
Test if link has joint
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the whether the Link contains the variable transform.
- Returns:
test if link has a joint
- Return type:
isjoint
Examples
>>> from roboticstoolbox import models >>> robot = models.URDF.Panda() >>> robot[1].isjoint # link with joint True >>> robot[8].isjoint # static link False
- islimit(q)
Checks if joint exceeds limit
link.islimit(q)
is True ifq
exceeds the joint limits defined bylink
.- Parameters:
q (
float
) – joint coordinate- Returns:
True if joint is exceeded
- Return type:
islimit
Notes
If no limits are set always return False.
See also
- property isprismatic: bool
Checks if the joint is of prismatic type
- Returns:
return: True if is prismatic
rtype: bool
- property isrevolute: bool
Checks if the joint is of revolute type
- Returns:
True if is revolute
- Return type:
isrevolute
- property jindex: Union[None, int]
Get/set joint index
link.jindex
is the joint indexlink.jindex = ...
checks and sets the joint index
For a serial-link manipulator the joints are numbered starting at zero and increasing sequentially toward the end-effector. For branched mechanisms this is not so straightforward. The link’s
jindex
property specifies the index of its joint variable within a vector of joint coordinates.- Returns:
joint index
- Return type:
jindex
Notes
jindex
values must be a sequence of integers startingat zero.
- property m: float
Get/set link mass
link.m
is the link masslink.m = ...
checks and sets the link mass
- Returns:
link mass
- Return type:
m
- property name: str
Get/set link name
link.name
is the link namelink.name = ...
checks and sets the link name
- Returns:
link name
- Return type:
name
- property nchildren: int
Number of child links
Will be zero for an end-effector link
- Returns:
number of child links
- Return type:
nchildren
- nofriction(coulomb=True, viscous=False)
Clone link without friction
link.nofriction()
is a copy of the link instance with the same parameters except, the Coulomb and/or viscous friction parameters are set to zero.- Parameters:
Notes
- For simulation it can be useful to remove Couloumb friction
which can cause problems for numerical integration.
- property parent: Optional[Self]
Parent link
This is a reference to the links parent in the kinematic chain
- Returns:
Link’s parent
- Return type:
parent
Examples
>>> from roboticstoolbox import models >>> robot = models.URDF.Panda() >>> robot[0].parent # base link has no parent >>> robot[1].parent # second link's parent Link(name = "panda_link0")
- property parent_name: Optional[str]
Parent link name
- Returns:
Link’s parent name
- Return type:
parent_name
- property qlim: Optional[ndarray]
Get/set joint limits
link.qlim
is the joint limitslink.qlim = ...
checks and sets the joint limits
- Returns:
joint limits
- Return type:
qlim
Notes
The limits are not widely enforced within the toolbox.
If no joint limits are specified the value is
None
See also
- property r: ndarray
Get/set link centre of mass
The link centre of mass is a 3-vector defined with respect to the link frame.
link.r
is the link centre of masslink.r = ...
checks and sets the link centre of mass
- Returns:
link centre of mass
- Return type:
r
- property robot: Optional[BaseRobot]
Get forward reference to the robot which owns this link
link.robot
is the robot referencelink.robot = ...
checks and sets the robot reference
- Returns:
The robot object
- Return type:
robot
- property v
Variable part of link ETS
The ETS for each Link comprises a constant part (possible the identity) followed by an optional joint variable transform. This property returns the latter.
- Returns:
joint variable transform
- Return type:
v
Examples
- A(q=0.0)[source]
Link transform matrix
link.A(q)
is an SE(2) matrix that describes the rigid-body transformation from the previous to the current link frame to the next, which depends on the joint coordinateq
.- Parameters:
q (
float
) – Joint coordinate (radians or metres). Not required for links with no variable- Returns:
link frame transformation matrix
- Return type:
T