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Two particles of same mass m moving with...

Two particles of same mass m moving with velocities `u_(1)` and `u_(2)` collide perfectly inelastically. The loss of energy would be :

A

`1//2m(u_(1)-u_(2))^(2)`

B

`1//4m(u_(1)-u_(2))^(2)`

C

`m(u_(1)-u_(2))^(2)`

D

`2m (u_(1)-u_(2))^(2)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the loss of energy in a perfectly inelastic collision between two particles of the same mass \( m \) moving with velocities \( u_1 \) and \( u_2 \), we can follow these steps: ### Step 1: Understand the Initial and Final States In a perfectly inelastic collision, the two particles stick together after the collision. Therefore, the final mass of the combined system is \( 2m \). ### Step 2: Apply Conservation of Momentum The momentum before the collision must equal the momentum after the collision. The initial momentum \( p_i \) is given by: \[ p_i = m u_1 + m u_2 = m (u_1 + u_2) \] The final momentum \( p_f \) after the collision is: \[ p_f = (2m) v \] Setting the initial and final momentum equal gives: \[ m (u_1 + u_2) = 2m v \] Dividing both sides by \( m \) (assuming \( m \neq 0 \)): \[ u_1 + u_2 = 2v \] Solving for \( v \): \[ v = \frac{u_1 + u_2}{2} \] ### Step 3: Calculate Initial Kinetic Energy The initial kinetic energy \( KE_i \) of the system is the sum of the kinetic energies of both particles: \[ KE_i = \frac{1}{2} m u_1^2 + \frac{1}{2} m u_2^2 \] ### Step 4: Calculate Final Kinetic Energy The final kinetic energy \( KE_f \) of the combined mass after the collision is: \[ KE_f = \frac{1}{2} (2m) v^2 = m v^2 \] Substituting \( v \) from Step 2: \[ KE_f = m \left(\frac{u_1 + u_2}{2}\right)^2 = m \frac{(u_1 + u_2)^2}{4} \] ### Step 5: Expand the Final Kinetic Energy Expanding \( (u_1 + u_2)^2 \): \[ KE_f = m \frac{u_1^2 + 2u_1 u_2 + u_2^2}{4} \] ### Step 6: Calculate the Loss of Energy The loss of kinetic energy \( \Delta KE \) is given by: \[ \Delta KE = KE_i - KE_f \] Substituting the expressions for \( KE_i \) and \( KE_f \): \[ \Delta KE = \left(\frac{1}{2} m u_1^2 + \frac{1}{2} m u_2^2\right) - \left(m \frac{u_1^2 + 2u_1 u_2 + u_2^2}{4}\right) \] Combining the terms: \[ \Delta KE = \frac{1}{2} m u_1^2 + \frac{1}{2} m u_2^2 - \frac{1}{4} m (u_1^2 + 2u_1 u_2 + u_2^2) \] ### Step 7: Simplify the Expression Factoring out \( \frac{m}{4} \): \[ \Delta KE = \frac{m}{4} \left(2u_1^2 + 2u_2^2 - (u_1^2 + 2u_1 u_2 + u_2^2)\right) \] This simplifies to: \[ \Delta KE = \frac{m}{4} \left(u_1^2 + u_2^2 - 2u_1 u_2\right) = \frac{m}{4} (u_1 - u_2)^2 \] ### Final Result Thus, the loss of energy in the collision is: \[ \Delta KE = \frac{m}{4} (u_1 - u_2)^2 \]
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