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A body of mass m1 collides head on perfe...

A body of mass m1 collides head on perfectly elastically with a stationary body of mass `m_(2)`. If velocities of `m_(1)` before and after the collision are v and –v/3 respectively then the value of `m_(1)//m_(2)` is-

A

1

B

2

C

0.5

D

4

Text Solution

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The correct Answer is:
To solve the problem, we will use the principles of conservation of momentum and conservation of kinetic energy, as the collision is perfectly elastic. ### Step-by-Step Solution: 1. **Identify the Given Information:** - Mass of the first body: \( m_1 \) - Mass of the second body: \( m_2 \) - Initial velocity of \( m_1 \): \( v \) - Initial velocity of \( m_2 \): \( 0 \) (stationary) - Final velocity of \( m_1 \): \( -\frac{v}{3} \) - Final velocity of \( m_2 \): \( v_1 \) (unknown) 2. **Apply Conservation of Momentum:** The total momentum before the collision equals the total momentum after the collision. \[ m_1 v + m_2 \cdot 0 = m_1 \left(-\frac{v}{3}\right) + m_2 v_1 \] Simplifying this, we have: \[ m_1 v = -\frac{m_1 v}{3} + m_2 v_1 \] Rearranging gives: \[ m_1 v + \frac{m_1 v}{3} = m_2 v_1 \] \[ \frac{4m_1 v}{3} = m_2 v_1 \quad \text{(Equation 1)} \] 3. **Apply Conservation of Kinetic Energy:** The total kinetic energy before the collision equals the total kinetic energy after the collision. \[ \frac{1}{2} m_1 v^2 = \frac{1}{2} m_1 \left(-\frac{v}{3}\right)^2 + \frac{1}{2} m_2 v_1^2 \] Simplifying this, we have: \[ \frac{1}{2} m_1 v^2 = \frac{1}{2} m_1 \frac{v^2}{9} + \frac{1}{2} m_2 v_1^2 \] Multiplying through by 2 to eliminate the fractions: \[ m_1 v^2 = \frac{m_1 v^2}{9} + m_2 v_1^2 \] Rearranging gives: \[ m_1 v^2 - \frac{m_1 v^2}{9} = m_2 v_1^2 \] \[ \frac{8m_1 v^2}{9} = m_2 v_1^2 \quad \text{(Equation 2)} \] 4. **Substituting \( m_2 \) from Equation 1 into Equation 2:** From Equation 1, we can express \( m_2 \): \[ m_2 = \frac{4m_1 v}{3v_1} \] Substituting this into Equation 2: \[ \frac{8m_1 v^2}{9} = \left(\frac{4m_1 v}{3v_1}\right) v_1^2 \] Simplifying gives: \[ \frac{8m_1 v^2}{9} = \frac{4m_1 v v_1}{3} \] Canceling \( m_1 \) (assuming \( m_1 \neq 0 \)): \[ \frac{8v^2}{9} = \frac{4v v_1}{3} \] Cross-multiplying gives: \[ 8v^2 \cdot 3 = 4v v_1 \cdot 9 \] \[ 24v^2 = 36v v_1 \] Dividing both sides by \( 12v \) (assuming \( v \neq 0 \)): \[ 2 = 3v_1 \] Thus: \[ v_1 = \frac{2}{3} v \] 5. **Finding the Ratio \( \frac{m_1}{m_2} \):** Substitute \( v_1 \) back into the expression for \( m_2 \): \[ m_2 = \frac{4m_1 v}{3 \cdot \frac{2}{3}v} = \frac{4m_1 v}{2v} = 2m_1 \] Therefore: \[ \frac{m_1}{m_2} = \frac{m_1}{2m_1} = \frac{1}{2} \] ### Final Answer: \[ \frac{m_1}{m_2} = \frac{1}{2} \quad \text{or} \quad 0.5 \]
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MOTION-CENTRE OF MASS-Exercise - 1
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