The situation is a particle of mass m striking a rod of the same mass and length $L$ at an angle with an initial velocity $v$ elastically.
Now to describe this situation I wrote the following equations:
$$mv\cos{\theta}=mv_1+mv_2$$
$$mv\cos{\theta}\cdot\frac{L}{4}=mv_1\cdot\frac{L}{4}+\frac{mL^{2}}{12}\cdot\omega$$
$$1=\frac{v_2+\omega\cdot\frac{L}{4}-v_1}{v\cos{\theta}}$$
Here I used linear momentum conservation, angular momentum conservation and coefficient of restitution respectively where $v_1$ is the final velocity of particle in the vertical direction and $v_2$ is the same for the centre of mass of the rod. And $\omega$ is the angular velocity of rod after collison.
Now my query is that since the rod is not hinged anywhere, am I right to conserve angular momentum about the centre of mass? Also I'm not sure whether the equation for coefficient of restitution should be written about the impact point or the centre. Moreover, is it true that the particle's component of velocity parallel to the rod remains unaffected?
Any help would be appreciated.