A system of particles in motion has mass center G as shown in the figure. The particle i has mass mi and its position with respect to a fixed point O is given by the position vector ri. The position of the particle with respect to G is given by the vector $\rho$i. The time rate of change of the angular momentum of the system of particles about G is (The quantity $\ddot{\rho _{i}}$ indicates second derivative of rI with respect to time and likewise for ri).
(a) $\sum ir_{i}$$\times m_{i}\ddot{\rho } _{i}$ (b) $\sum i \rho _{i} \times m_{i} \ddot{r}_{i}$
(c)$\sum ir_{i}\times m_{i} \ddot{r}_{i}$ (d) $\sum i\rho _{i}\times m_{i} \ddot{\rho } _{i}$