Jacobians: velocities and static forces
Relative Velocity
${}^A ({}^B V_{Q})$ is the velocity of Q relative to {B}, described in {A}
${}^A ({}^A V_{Q})$ can be written as ${}^A V_{Q}$
${}^U V_{CORG}$ can be written as $v_c$ (U is the world frame)
Observation of motion in {B} from {A}
$$
{}^AV_Q={}^AV_{BORG}+{}^A_B R {}^B V_Q + {}^A \Omega_B \times {}^A_B R {}^B Q \tag{5-13}
$$
three parts:
- velocity of {B} origin relative to {A}
- velocity of Q relative to {B}, described in {A}
- effect caused by rotation of {B}, relative to {A}
Velocity “propagation”
a special case of (5-13)
$$
{}^{i+1}\omega_{i+1} = {}^{i+1}_ iR {}^i\omega_i + \dot{\theta} _{i+1} {}^{i+1}\hat{Z} _{i+1} \tag{5-45}
$$
$$
{}^{i+1}v_{i+1} = {}^{i+1}_ iR({}^iv_i+{}^i\omega_i \times {}^iP_{i+1}) \tag{5-46}
$$
Jacobian (6*N)
$$
\begin{bmatrix} v \\ \omega \end{bmatrix} = J(\theta)\dot{\theta} \tag{5-64}
$$
$$
J(\theta) = \begin{bmatrix}
\hat{Z}_0 \times (O_N - O_0) & \hat{Z}_1 \times (O_N - O_1) & \cdots \\
\hat{Z}_0 & \hat{Z}_1 & \cdots
\end{bmatrix}
$$
transform 6*6 jacobian from {B} to {A}:
$$
{}^A J(\theta) = \begin{bmatrix} {}^A_B R & 0 \\ 0 & {}^A_B R \end{bmatrix} {}^B J(\theta) \tag{5-71}
$$
Singularity
$$
det(J(\theta)) = 0
$$
- Workspace-boundary singularities: when it is fully stretched out or folded back
- Workspace-interior singularities: when multiple joints line up
Static force
According to the principle of virtual work:
$$
\tau = J^T \mathcal{F}
$$
$\mathcal{F}$ consists of force and moment at the end, which can be mapped to joint torque by jacobian transpose