Consider a moving rigid body and the velocity of a point P on the body being a function of the position and velocity of a center-point C and the angular velocity
.
The linear velocity vector
at P is expressed in terms of the velocity vector
at C as:

where
is the angular velocity vector.
The material acceleration at P is:

where
is the angular acceleration vector.
The spatial acceleration
at P is expressed in terms of the spatial acceleration
at C as:
![{\displaystyle {\begin{aligned}{\boldsymbol {\psi }}_{P}&={\frac {\partial \mathbf {v} _{P}}{\partial t}}\\[1ex]&={\boldsymbol {\psi }}_{C}+{\boldsymbol {\alpha }}\times (\mathbf {r} _{P}-\mathbf {r} _{C})\end{aligned}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/19ca076ef089f9344bfa5bc17d5634ba1a289ad3)
which is similar to the velocity transformation above.
In general the spatial acceleration
of a particle point P that is moving with linear velocity
is derived from the material acceleration
at P as:
