A disc is rotating with angant whose nosition vector 31 axis. A force $\vec{F}$ acts at a point whose position vector with respect to the axis of rotation is $\vec{r}$. The power associated with the torque due to the force is given by
(a) $(\vec{r} \times \vec{F}) \cdot \vec{\omega}$
(b) $(\vec{r} \times \vec{F}) \times \vec{\omega}$
(c) $\bar{r} \cdot(\vec{F} \times \vec{\omega})$
(d) $\bar{r} \times(\vec{F} \cdot \vec{\omega})$