1. Physics 321 Hour 37 Collisions in Three Dimensions

2. Collision in the CM Frame Assume we know the masses, the initial momentum of each body (they’re the same), and the scattering angle. Θ Θ

3. Collision in the CM Frame Assume we know any energy loss as well. We can find the kinetic energies is we know the momenta and the masses.

4. Collision in the CM Frame First, we find P. Then we find T 1 and T 2. Now we know everything!

5. Elastic Scattering If E ex =0, All the scattering can do is change the directions of the particles.

6. The CM Frame The cm frame is really easy… Theorists (almost) always work in the cm frame. Experimentalists usually convert cross sections to the cm as well. But, experiments are not usually conducted in the cm frame!

7. CM to Lab Now let’s assume we have the CM solution and we want to get back to the lab frame. First, we write everything in terms of velocity

8. CM to Lab So we can find the lab quantities

9. CM to Lab

10. But usually we don’t know Θ a priori. This is a quadratic equation we can solve for p 1. Then we can find Θ and everything else.

11. Example CollisionKinematics.nb