1. Define variables:
2. Apply the principle of conservation of momentum:
The total momentum before the collision equals the total momentum after the collision:
$m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2$
$(1)(12) + (2)(-24) = (1)v_1 + (2)v_2$
$12 - 48 = v_1 + 2v_2$
$v_1 + 2v_2 = -36$ (Equation 1)
3. Apply the definition of the coefficient of restitution:
$e = \frac{\text{relative velocity of separation}}{\text{relative velocity of approach}} = \frac{v_2 - v_1}{u_1 - u_2}$
$\frac{2}{3} = \frac{v_2 - v_1}{12 - (-24)}$
$\frac{2}{3} = \frac{v_2 - v_1}{36}$
$24 = v_2 - v_1$
$v_2 - v_1=24$ (Equation 2)
4. Solve the simultaneous equations:
Adding Equation 1 and Equation 2:
$3v_2 = -12$
$v_2 = -4$ m/s
Substituting $v_2$ back into Equation 2:
$-4 - v_1 = 24$
$v_1 = -28$ m/s
The correct answer is (B) $-28$ ms-1, $-4$ ms-1.
As shown below, bob A of a pendulum having a massless string of length \( R \) is released from 60° to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):