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A system of three masses, m1 , m2 and m3 and a spring (of spring constant k) is set up, as shown, an a straight narrow and smooth track.

The mass, m1 , starts moving with a veloicty u (m/s) and collides elastically with the mass m2 ; A little later, when the spring has been compressed by an amount x0 (metre), the masses m2 and m3 are moving with the same veloicty, say, v. The velocity v, and the spring constant, k, of the spring, are then given respectively by

(1) \(V =\frac{u}{3}ms^{},k=(\frac{1}{30}\frac{u^2_0}{x^2_0})N/M\)

(2) \(V =\frac{u}{3}ms^{-1},k=(\frac{1}{80}\frac{u^2_0}{x^2_0})N/M\)

(3) \(V =\frac{u}{2}ms^{-1},k=(\frac{1}{30}\frac{u^2_0}{x^2_0})N/M\)

(4) \(V =\frac{u}{3}ms^{-1},k=(\frac{1}{30}\frac{u^2_0}{x^2_0})N/M\)

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(4) \(V =\frac{u}{3}ms^{-1},k=(\frac{1}{30}\frac{u^2_0}{x^2_0})N/M\)

The masses m1 and m2 being equal, their velocities, after m1 collides elastically with m2 , are zero and u, respectively. 

A little later, when m2 and m3 have the same veloicty, v, and the spring has been compressed by an amount x0 , we have, by the laws of conservation of momentum and energy.

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