Classical Mechanics (Kibble & Berkshire) · Problem 10.18

The angular momentum principle — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · collisions

Problem

Equal masses Show that, when the particles are of equal mass, the elastic scattering formulae take the simple form θ1=12ψθ2=12π−12ψθ=12πE1E0=cos⁡212ψE2E0=sin⁡212ψ\theta_1 = \tfrac{1}{2}\psi \qquad \theta_2 = \tfrac{1}{2}\pi - \tfrac{1}{2}\psi \qquad \theta = \tfrac{1}{2}\pi \qquad \frac{E_1}{E_0} = \cos^2\tfrac{1}{2}\psi \qquad \frac{E_2}{E_0} = \sin^2\tfrac{1}{2}\psi where ψ\psi is the scattering angle in the ZM frame. In the scattering of neutrons of energy EE by neutrons at rest, in what directions should the experimenter look to find neutrons of energy 14E\frac{1}{4}E? What other energies would be observed in these directions?

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