Two discs of moment of inertia $I_{1}$ and $I_{2}$ about their respective axes and rotating with angular speed $\omega_{1}$ and $\omega_{2}$ are brought into contact face to face with their axes of rotation coincident. Then the loss of in kinetic energy of the system in the process is
(a) $\frac{l_{1} b}{2\left(I_{1}+b_{2}\right)}\left(\omega_{1}-\omega_{2}\right)^{2}$
(b) $-\frac{l_{1} b}{2\left(I_{1}+b_{2}\right)}\left(\omega_{1}-\omega_{2}\right)^{2}$
(c) $\frac{l_{1} l_{2}}{\left(I_{1}+l_{2}\right)}\left(\omega_{1}-\omega_{2}\right)^{2}$
(d) zero