If we are using the equation $\tau=I\cdot \alpha$ (where $\tau$ is the torque, $I$ is the moment of inertia, $\alpha$ is the angular acceleration) in a rotating frame of reference, we have to account for the fictitious forces, so, my question is, do these forces 'act' on the center of mass of the extended object?
As far as I know, the force $-ma_{frame}$ can be thought of as acting at the center of mass effectively, it gives the correct force and torque as we would get if we were to apply the force on each infinitesimal part of the body.
What about the coreolis term, the euler term and the centripetal term of fictitious force?