Two particles, 1 and 2, each of mass 𝑚, are connected by a massless spring, and are on a horizontal frictionless plane, as shown in the figure. Initially, the two particles, with their center of mass at
x0, are oscillating with amplitude 𝑎 and angular frequency 𝜔. Thus, their positions at time 𝑡 are given by
x1(t)=(x0+d)+α sinωt and
x2t=(x0−d)−αsin wt, respectively, where
d>2a. Particle 3 of mass 𝑚 moves towards this system with speed 𝑢0 = 𝑎𝜔/2, and undergoes instantaneous elastic collision with particle 2, at time
t0. Finally, particles 1 and 2 acquire a center of mass speed
vcm and oscillate with amplitude 𝑏 and the same angular frequency 𝜔.
