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A particle of mass m1 makes a perfectly elastic collision with a stationary particle of mass m2, where m1 > m2. What is the largest possible angle by which the incoming particle can be deflected after the collision?
- arcsin(m2/m1)
- arcsin(m1/m2)
- arccos(m2/m1)
- arctan(m2/m1)
Correct answer: arcsin(m2/m1)
Solution
For m1 > m2 the heavy particle cannot be scattered backward; the maximum lab-frame deflection angle satisfies sin(theta_max) = m2/m1.
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