Extra Credit (2pts)
The dynamics equations of motion for rigid body motion is a plane is given by:
SF = m a (translational acceleration)
SMCM = ICM a (rotational acceleration)
where MCM is the moment about the Center of Mass, ICM is moment of inertia about the Center of Mass, and a is the angular acceleration.
Prove that for static or quasi-static analysis, the sum of moments can be taken about any point, as shown below
SF = 0 (translational equilibrium)
SMa = 0 (rotational equilibrium)
where Ma is the moment about any point.