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- Trying to understand physics of maximum deflection
When a heavier mass (or nucleus say) collides with a lighter one, it deflects through a certain angle which has a theoretical maximum. There are numerous derivations for this maximum angle of deflection ##(\sin\theta_{d_{max}}=m/M)## where m is the small mass and M the larger but none seem to provide a clear physical explanation of what is going on. I tried to understand it in terms of energy transfer but got nowhere with that. So my question is what is physically going on when we reach maximum angle of deflection ? Is there something that physically defines when we move from a 'grazing' collision to a 'non grazing' collision ? Here for example is a plot of ##\tan\theta_d## vs ##\theta_i## where the latter angle of incidence is measured from the plane of contact. The mass ratio m/M in this case is 0.6 and so ##\theta_{d_{max}}=36.87^{\circ}## when ##\theta_i=63.42^{\circ}.##
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