Paper 4, Section II, A

Dynamics and Relativity | Part IA, 2009

(a) Write down expressions for the relativistic 3 -momentum p\mathbf{p} and energy EE of a particle of rest mass mm and velocity v\mathbf{v}. Show that these expressions are consistent with

E2=ppc2+m2c4E^{2}=\mathbf{p} \cdot \mathbf{p} c^{2}+m^{2} c^{4}

Define the 4-momentum P\mathbf{P} for such a particle and obtain ()(*) by considering the invariance properties of P\mathbf{P}.

(b) Two particles, each with rest mass mm and energy EE, moving in opposite directions, collide head on. Show that it is consistent with the conservation of 4 -momentum for the collision to result in a set of nn particles of rest masses μi\mu_{i} (for 1in)\left.1 \leqslant i \leqslant n\right) only if

E12(i=1nμi)c2.E \geqslant \frac{1}{2}\left(\sum_{i=1}^{n} \mu_{i}\right) c^{2} .

(c) A particle of rest mass m1m_{1} and energy E1E_{1} is fired at a stationary particle of rest mass m2m_{2}. Show that it is consistent with the conservation of 4 -momentum for the collision to result in a set of nn particles of rest masses μi\mu_{i} (for 1in1 \leqslant i \leqslant n ) only if

E1(i=1nμi)2m12m222m2c2E_{1} \geqslant \frac{\left(\sum_{i=1}^{n} \mu_{i}\right)^{2}-m_{1}^{2}-m_{2}^{2}}{2 m_{2}} c^{2}

Deduce the minimum frequency required for a photon fired at a stationary particle of rest mass m2m_{2} to result in the same set of nn particles, assuming that the conservation of 4 -momentum is the only relevant constraint.

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