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Body A of mass 4m moving with speed u co...

Body A of mass 4m moving with speed u collides with another body B of mass 2m at rest the collision is head on and elastic in nature. After the collision the fraction of energy lost by colliding body A is :

A

`(5)/(9)`

B

`(1)/(9)`

C

`(8)/(9)`

D

`(4)/(9)`

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The correct Answer is:
To solve the problem step by step, we will use the principles of conservation of momentum and conservation of kinetic energy, as the collision is elastic. ### Step 1: Understand the Initial Conditions - Mass of body A, \( m_A = 4m \) - Mass of body B, \( m_B = 2m \) - Initial speed of body A, \( u_A = u \) - Initial speed of body B, \( u_B = 0 \) (at rest) ### Step 2: Write the Conservation of Momentum Equation The total momentum before the collision must equal the total momentum after the collision: \[ m_A \cdot u_A + m_B \cdot u_B = m_A \cdot v_A + m_B \cdot v_B \] Substituting the values, we get: \[ 4m \cdot u + 2m \cdot 0 = 4m \cdot v_1 + 2m \cdot v_2 \] This simplifies to: \[ 4u = 4v_1 + 2v_2 \quad \text{(1)} \] ### Step 3: Write the Conservation of Kinetic Energy Equation The total kinetic energy before the collision must equal the total kinetic energy after the collision: \[ \frac{1}{2} m_A u_A^2 + \frac{1}{2} m_B u_B^2 = \frac{1}{2} m_A v_A^2 + \frac{1}{2} m_B v_B^2 \] Substituting the values, we get: \[ \frac{1}{2} (4m) u^2 + 0 = \frac{1}{2} (4m) v_1^2 + \frac{1}{2} (2m) v_2^2 \] This simplifies to: \[ 2u^2 = 2v_1^2 + v_2^2 \quad \text{(2)} \] ### Step 4: Solve the Equations From equation (1): \[ 4u = 4v_1 + 2v_2 \implies 2u = 2v_1 + v_2 \implies v_2 = 2u - 2v_1 \quad \text{(3)} \] Substituting equation (3) into equation (2): \[ 2u^2 = 2v_1^2 + (2u - 2v_1)^2 \] Expanding the square: \[ 2u^2 = 2v_1^2 + (4u^2 - 8uv_1 + 4v_1^2) \] Combining like terms: \[ 2u^2 = 4u^2 - 6v_1^2 - 8uv_1 \] Rearranging gives: \[ 0 = 2u^2 - 6v_1^2 - 8uv_1 \] Dividing through by 2: \[ 0 = u^2 - 3v_1^2 - 4uv_1 \] This is a quadratic equation in \( v_1 \). Solving using the quadratic formula: \[ v_1 = \frac{-(-4u) \pm \sqrt{(-4u)^2 - 4(-3)(u^2)}}{2(-3)} \] Calculating the discriminant: \[ = \frac{4u \pm \sqrt{16u^2 + 12u^2}}{-6} = \frac{4u \pm \sqrt{28u^2}}{-6} = \frac{4u \pm 2\sqrt{7}u}{-6} = \frac{2u(2 \pm \sqrt{7})}{-6} = -\frac{u(2 \pm \sqrt{7})}{3} \] Taking the positive root for \( v_1 \): \[ v_1 = \frac{u(2 - \sqrt{7})}{3} \] Substituting \( v_1 \) back into equation (3) to find \( v_2 \): \[ v_2 = 2u - 2 \left(\frac{u(2 - \sqrt{7})}{3}\right) = 2u - \frac{2u(2 - \sqrt{7})}{3} \] Calculating gives: \[ v_2 = \frac{6u - 4u + 2u\sqrt{7}}{3} = \frac{2u + 2u\sqrt{7}}{3} = \frac{2u(1 + \sqrt{7})}{3} \] ### Step 5: Calculate the Initial and Final Kinetic Energies - Initial kinetic energy of A: \[ KE_{initial} = \frac{1}{2} (4m) u^2 = 2mu^2 \] - Final kinetic energy of A: \[ KE_{final} = \frac{1}{2} (4m) v_1^2 = 2m \left(\frac{u(2 - \sqrt{7})}{3}\right)^2 = 2m \cdot \frac{u^2(2 - \sqrt{7})^2}{9} \] ### Step 6: Calculate the Energy Lost Energy lost by A: \[ \Delta KE = KE_{initial} - KE_{final} \] Substituting the values: \[ \Delta KE = 2mu^2 - 2m \cdot \frac{u^2(2 - \sqrt{7})^2}{9} \] ### Step 7: Fraction of Energy Lost The fraction of energy lost by A is: \[ \text{Fraction} = \frac{\Delta KE}{KE_{initial}} = \frac{2mu^2 - 2m \cdot \frac{u^2(2 - \sqrt{7})^2}{9}}{2mu^2} \] This simplifies to: \[ = 1 - \frac{(2 - \sqrt{7})^2}{9} \] Calculating gives: \[ = 1 - \frac{4 - 4\sqrt{7} + 7}{9} = 1 - \frac{11 - 4\sqrt{7}}{9} = \frac{9 - (11 - 4\sqrt{7})}{9} = \frac{4\sqrt{7} - 2}{9} \] ### Final Answer The fraction of energy lost by colliding body A is: \[ \frac{8}{9} \]

To solve the problem step by step, we will use the principles of conservation of momentum and conservation of kinetic energy, as the collision is elastic. ### Step 1: Understand the Initial Conditions - Mass of body A, \( m_A = 4m \) - Mass of body B, \( m_B = 2m \) - Initial speed of body A, \( u_A = u \) - Initial speed of body B, \( u_B = 0 \) (at rest) ...
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