# Manipulator Kinematics

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The kinematics of a robot manipulator describes the relationship between the motion of the joints of the manipulator and the resulting motion of the rigid bodies which form the robot. This chapter gives a description of the kinematics for a general $n$ degree of freedom, open-chain robot manipulator using the tools presented in Chapter 2 - Rigid Body Motion. We also present a brief treatment of redundant and parallel manipulators using this same framework.

## Chapter Summary

The following are the key concepts covered in this chapter:

1. The forward kinematics' of a manipulator is described by a mapping <amsmath>g_{st}:Q \to \mbox{\it{SE}}(3)</amsmath> which describes the end-effector configuration as a function of the robot joint variables. For open-chain manipulators consisting of revolute and prismatic joints, the kinematics can be written using the product of exponentials formula:
<amsmath>
 g_{st}(\theta) = e^{\widehat{\xi}_1 \theta_1} e^{\widehat{\xi}_2 \theta_2} \cdots
e^{\widehat{\xi}_n \theta_n} g_{st}(0),

</amsmath>

where <amsmath>\xi_i</amsmath> is the twist corresponding to the \th{i} joint axis in the reference (<amsmath>\theta = 0</amsmath>) configuration.

2. The (complete) workspace of a manipulator is the set of end-effector configurations which can be reached by some choice of joint angles. The reachable workspace defines end-effector positions which can be reached at some orientation. The dextrous workspace defines end-effector positions which can be reached at any orientation.
3. The inverse kinematics of a manipulator describes the relationship between the end-effector configuration and the joint angles which achieve that configuration. For many manipulators, we can find the inverse kinematics by making use of the following subproblems:
 Subproblem 1: e^{\widehat{\xi}\theta} p = q rotate one point onto another Subproblem 2: e^{\widehat{\xi}_1\theta_1} e^{\widehat{\xi}_2\theta_2} p = q rotate about two intersecting twists Subproblem 3: \|q - e^{\widehat{\xi}\theta} p\| = \delta move one point to a specified distance from another

To find a complete solution, we apply the manipulator kinematics to a set of points which reduce the complete problem into an appropriate set of subproblems.

4. The manipulator Jacobian relates the joint velocities <amsmath>\dot\theta</amsmath> to the end-effector velocity <amsmath>V_{st}</amsmath> and the joint torques <amsmath>\tau</amsmath> to the end-effector wrench <amsmath>F</amsmath>:
<amsmath>
 \alignedat 3
V_{st}^s &= J_{st}^s(\theta) \dot\theta &\qquad
\tau &= (J_{st}^s)^T F_s &\qquad
&\text{(spatial)} \\
V_{st}^b &= J_{st}^b(\theta) \dot\theta &\qquad
\tau &= (J_{st}^b)^T F_t &\qquad
&\text{(body)}.
\endalignedat

</amsmath>

If the manipulator kinematics is written using the product of exponentials formula, then the manipulator Jacobians have the form:

<amsmath>
 \alignedat 2
J_{st}^s(\theta) &=
\bmatrix \xi_1 & \xi_2' & \cdots & \xi_n' \endbmatrix
\displaystyle
e^{\widehat{\xi}_1 \theta_1} \cdots e^{\widehat{\xi}_{i-1} \theta_{i-1}}
\bigr)} \xi_i \\
J_{st}^b(\theta) &=
\bmatrix
\xi_1^\dagger & \cdots & \xi_{n-1}^\dagger & \xi_n^\dagger
\displaystyle
e^{\widehat{\xi}_i \theta_i} \cdots e^{\widehat{\xi}_n \theta_n} g_{st}(0)
\bigr)} \xi_i.
\endaligned

</amsmath>
5. A configuration is singular if the manipulator Jacobian loses rank at that configuration. Examples for a general six degree of freedom arm include:
• Two collinear revolute joints
• Three parallel, coplanar revolute joint axes
• Four intersecting revolute joint axes
The manipulability of a robot provides a measure of the nearness to singularity.
6. A manipulator is kinematically redundant if it has more than the minimally required degrees of freedom. The self-motion manifold describes the set of joint values which can be used to achieve a desired configuration of the end-effector. Internal motions correspond to motions along the self-motion manifold and satisfy
<amsmath>
 J_{st}(\theta) \dot\theta = 0.

</amsmath>
7. A parallel manipulator has multiple kinematic chains connecting the base to the end-effector. For the case of two chains, the kinematics satisfies the structure equation
<amsmath>
 g_{st} =
e^{\widehat{\xi}_{11}\theta_{11}} \cdots e^{\widehat{\xi}_{1n_1}\theta_{1n_1}} g_{st}(0) =
e^{\widehat{\xi}_{21}\theta_{21}} \cdots e^{\widehat{\xi}_{2n_2}\theta_{2n_2}} g_{st}(0),

</amsmath>

where <amsmath>\xi_{ij}</amsmath> is twist for the the \th{j} joint on the \th{i} chain. The Jacobian of the structure equation has the form

<amsmath>
 V_{st}^s = J_1^s(\Theta_1) \dot\Theta_1 = J_2^s(\Theta_2) \dot\Theta_2,

</amsmath>

where <amsmath>\Theta_i = (\theta_{i1}, \dots, \theta_{in_i})</amsmath>. A kinematic singularity occurs when the dimension of the space of admissible forces drops rank. Other singularities can occur when the set of end-effector forces which can be generated by the actuated joints drops rank.