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A spherical ball of mass m(1) collides h...

A spherical ball of mass `m_(1)` collides head on with another ball of mass `m_(2)` at rest . The collision is elastic . The fraction of kinetic energy lost by `m_(1)` is `:`

A

`(4m_1m_2)/((m_1+m_2)^2)`

B

`m_1/(m_1+m_2)`

C

`m_2/(m_1+m_2)`

D

`(m_1m_2)/((m_1+m_2)^2)`

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To find the fraction of kinetic energy lost by the mass \( m_1 \) during an elastic collision with another mass \( m_2 \) that is initially at rest, we can follow these steps: ### Step 1: Understand the Problem We have two masses, \( m_1 \) (moving) and \( m_2 \) (at rest). The collision is elastic, meaning both momentum and kinetic energy are conserved. ### Step 2: Apply Conservation of Momentum The conservation of momentum before and after the collision can be expressed as: \[ m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2 \] Since \( m_2 \) is at rest initially, \( u_2 = 0 \). Thus, the equation simplifies to: \[ m_1 u_1 = m_1 v_1 + m_2 v_2 \] This can be rearranged to: \[ u_1 = v_1 + \frac{m_2}{m_1} v_2 \quad \text{(Equation 1)} \] ### Step 3: Apply Conservation of Kinetic Energy For elastic collisions, kinetic energy is also conserved: \[ \frac{1}{2} m_1 u_1^2 + \frac{1}{2} m_2 u_2^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2 \] Again, since \( u_2 = 0 \), we have: \[ \frac{1}{2} m_1 u_1^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2 \] This can be rearranged to: \[ m_1 u_1^2 = m_1 v_1^2 + m_2 v_2^2 \quad \text{(Equation 2)} \] ### Step 4: Use Coefficient of Restitution For elastic collisions, the coefficient of restitution \( e = 1 \): \[ e = \frac{v_2 - v_1}{u_1 - u_2} = 1 \] Since \( u_2 = 0 \), we have: \[ v_2 - v_1 = u_1 \quad \Rightarrow \quad v_2 = u_1 + v_1 \quad \text{(Equation 3)} \] ### Step 5: Substitute Equation 3 into Equation 1 Substituting \( v_2 \) from Equation 3 into Equation 1 gives: \[ u_1 = v_1 + \frac{m_2}{m_1}(u_1 + v_1) \] Rearranging this leads to: \[ u_1(1 - \frac{m_2}{m_1}) = v_1(1 + \frac{m_2}{m_1}) \] This can be simplified to: \[ v_1 = u_1 \frac{1 - \frac{m_2}{m_1}}{1 + \frac{m_2}{m_1}} \quad \text{(Equation 4)} \] ### Step 6: Calculate the Kinetic Energy Loss The initial kinetic energy of \( m_1 \) is: \[ KE_{initial} = \frac{1}{2} m_1 u_1^2 \] The final kinetic energy of \( m_1 \) is: \[ KE_{final} = \frac{1}{2} m_1 v_1^2 \] The kinetic energy lost is: \[ KE_{lost} = KE_{initial} - KE_{final} = \frac{1}{2} m_1 u_1^2 - \frac{1}{2} m_1 v_1^2 \] The fraction of kinetic energy lost is: \[ \text{Fraction lost} = \frac{KE_{lost}}{KE_{initial}} = \frac{\frac{1}{2} m_1 u_1^2 - \frac{1}{2} m_1 v_1^2}{\frac{1}{2} m_1 u_1^2} = 1 - \frac{v_1^2}{u_1^2} \] ### Step 7: Substitute \( v_1 \) from Equation 4 Substituting \( v_1 \) from Equation 4 into the fraction gives: \[ \text{Fraction lost} = 1 - \left( \frac{m_1 - m_2}{m_1 + m_2} \right)^2 \] ### Final Result After simplifying, we find the fraction of kinetic energy lost by \( m_1 \): \[ \text{Fraction lost} = \frac{4 m_1 m_2}{(m_1 + m_2)^2} \]

To find the fraction of kinetic energy lost by the mass \( m_1 \) during an elastic collision with another mass \( m_2 \) that is initially at rest, we can follow these steps: ### Step 1: Understand the Problem We have two masses, \( m_1 \) (moving) and \( m_2 \) (at rest). The collision is elastic, meaning both momentum and kinetic energy are conserved. ### Step 2: Apply Conservation of Momentum The conservation of momentum before and after the collision can be expressed as: \[ ...
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