As an illustration of the principle of relativity in classical mechanics, consider the following generic collision: In inertial frame S, particle A (mass mA, velocity uA) hits particle B (mass mB, velocity uB). In the course of the collision some mass rubs off A and onto B, and we are left with particles C (mass mC , velocity uC) and D (mass mD, velocity uD). Assume that momentum (p ≡mu) is conserved in S.
(a) Prove that momentum is also conserved in inertial frame , which moves with velocity v relative to S. [Use Galileo’s velocity addition rule—this is an entirely classical calculation. What must you assume about mass?]
(b) Suppose the collision is elastic in S; show that it is also elastic in
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