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Two particles of masses m1m_1 and m2m_2 move with initial velocities u1u_1 and u2u_2 respectively. On collision, one of the particles gets excited to a higher level, after absorbing energy EE. If the final velocities of particles are v1v_1 and v2v_2, then we must have:

A

m12u1+m22u2E=m12v1+m22v2m_1^2 u_1 + m_2^2 u_2 - E = m_1^2 v_1 + m_2^2 v_2

B

12m1u12+12m2u22=12m1v12+12m2v22\frac{1}{2} m_1 u_1^2 + \frac{1}{2} m_2 u_2^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2

C

12m1u12+12m2u22E=12m1v12+12m2v22\frac{1}{2} m_1 u_1^2 + \frac{1}{2} m_2 u_2^2 - E = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2

D

12m12u12+12m22u22+E=12m12v12+12m22v22\frac{1}{2} m_1^2 u_1^2 + \frac{1}{2} m_2^2 u_2^2 + E = \frac{1}{2} m_1^2 v_1^2 + \frac{1}{2} m_2^2 v_2^2

Step-by-Step Solution

This problem is governed by the Law of Conservation of Energy, which states that the total energy of an isolated system remains constant .

  1. Initial Energy: Before the collision, the total energy of the system is the sum of the kinetic energies of the two particles: KEinitial=12m1u12+12m2u22KE_{initial} = \frac{1}{2}m_1 u_1^2 + \frac{1}{2}m_2 u_2^2 .
  2. Final Energy: After the collision, the total energy consists of the final kinetic energies of the particles plus the internal excitation energy EE absorbed by one of the particles: Efinal=12m1v12+12m2v22+EE_{final} = \frac{1}{2}m_1 v_1^2 + \frac{1}{2}m_2 v_2^2 + E .
  3. Energy Balance: Equating the initial and final states: 12m1u12+12m2u22=12m1v12+12m2v22+E\frac{1}{2}m_1 u_1^2 + \frac{1}{2}m_2 u_2^2 = \frac{1}{2}m_1 v_1^2 + \frac{1}{2}m_2 v_2^2 + E
  4. Rearranging: To match the provided options, we subtract EE from both sides: 12m1u12+12m2u22E=12m1v12+12m2v22\frac{1}{2}m_1 u_1^2 + \frac{1}{2}m_2 u_2^2 - E = \frac{1}{2}m_1 v_1^2 + \frac{1}{2}m_2 v_2^2

This describes an inelastic collision where kinetic energy is not conserved because a portion of it is transformed into internal potential/excitation energy .

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