Imagine I throw two objects at each other.
- One object is a small rigid body and the other is a very long rod.
- The impact will happen at the closest sections of the two objects, assumed to be normal to their respective longitudinal axis and parallel to each other.
- The line of impact is contained in a plane that also contains the principal axis of inertia of both objects.
- The mass of the rigid body is $\ M_{S}$ (kg) and just before hitting the end section of the rod, it has a known velocity $\ v_{Sb}$ (aligned with the longitudinal axis of the rod).
- After hitting the rigid body has a known velocity $\ v_{Sa}$, in the opposite direction of $\ v_{Sb}$.
- The rod has a mass-length density equal to $\ m_{R}$(kg/m) and just before hitting the end section of the rigid object, it has a known velocity $\ v_{Rb}$ (aligned with the longitudinal axis of the rod).
I'd like to find the final velocity, $\ v_{Ra}$, of the rod after impact.
From the conservation of linear momentum:
$$\ v_{Sb}*M_{S}-v_{Rb}*M_{Rb}=v_{Ra}*M_{Ra}-v_{Sa}*M_{S}$$
But how to define $\ M_{R}$?
Before collapse it can be assumed that the entire rod is traveling with speed $\ v_{Rb}$, so $\ M_{Rb}$is the total mass of the rod.
But immediately after impact? I know that the impact wave will propagate through the rod at the speed of sound through the material of the rod. Therefore, how to define $\ M_{Ra}$? For a given time instant $\ t$ do I need to do the integral of the momentum of the rod along its length with a speed diagram? If yes, which speed diagram?