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A neutron makes is a head - on elastic c...

A neutron makes is a head - on elastic collision with a stationary deuteron The fraction energy loss of the neutron in the collision is

A

`16//81`

B

`8//9`

C

`8//27`

D

`2//3`

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The correct Answer is:
To solve the problem of the neutron making a head-on elastic collision with a stationary deuteron, we will follow these steps: ### Step 1: Understand the Problem We have a neutron (mass \( m_1 \)) colliding elastically with a stationary deuteron (mass \( m_2 = 2m_1 \)). We need to find the fraction of energy lost by the neutron after the collision. ### Step 2: Conservation of Momentum In an elastic collision, both momentum and kinetic energy are conserved. The conservation of momentum before and after the collision can be expressed as: \[ m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2 \] Here, \( u_1 \) is the initial velocity of the neutron, \( u_2 = 0 \) (the deuteron is stationary), \( v_1 \) is the final velocity of the neutron, and \( v_2 \) is the final velocity of the deuteron. Substituting the values, we get: \[ m_1 u_1 + 0 = m_1 v_1 + 2m_1 v_2 \] This simplifies to: \[ u_1 = v_1 + 2v_2 \quad \text{(Equation 1)} \] ### Step 3: Conservation of Kinetic Energy The conservation of kinetic energy before and after the collision can be expressed as: \[ \frac{1}{2} m_1 u_1^2 + 0 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2 \] Substituting \( m_2 = 2m_1 \): \[ \frac{1}{2} m_1 u_1^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} (2m_1) v_2^2 \] This simplifies to: \[ u_1^2 = v_1^2 + 2v_2^2 \quad \text{(Equation 2)} \] ### Step 4: Solve the Equations Now we have two equations (Equation 1 and Equation 2) to solve for \( v_1 \) and \( v_2 \). From Equation 1: \[ v_1 = u_1 - 2v_2 \] Substituting \( v_1 \) in Equation 2: \[ u_1^2 = (u_1 - 2v_2)^2 + 2v_2^2 \] Expanding and simplifying: \[ u_1^2 = u_1^2 - 4u_1v_2 + 4v_2^2 + 2v_2^2 \] \[ 0 = -4u_1v_2 + 6v_2^2 \] Factoring out \( v_2 \): \[ v_2(6v_2 - 4u_1) = 0 \] Thus, \( v_2 = \frac{2}{3} u_1 \). Substituting \( v_2 \) back into Equation 1: \[ v_1 = u_1 - 2\left(\frac{2}{3} u_1\right) = u_1 - \frac{4}{3} u_1 = -\frac{1}{3} u_1 \] ### Step 5: Calculate Initial and Final Kinetic Energies Initial kinetic energy of the neutron: \[ KE_{initial} = \frac{1}{2} m_1 u_1^2 \] Final kinetic energy of the neutron: \[ KE_{final} = \frac{1}{2} m_1 v_1^2 = \frac{1}{2} m_1 \left(-\frac{1}{3} u_1\right)^2 = \frac{1}{2} m_1 \frac{1}{9} u_1^2 = \frac{1}{18} m_1 u_1^2 \] ### Step 6: Calculate Energy Loss Energy lost by the neutron: \[ \Delta KE = KE_{initial} - KE_{final} = \frac{1}{2} m_1 u_1^2 - \frac{1}{18} m_1 u_1^2 = \left(\frac{9}{18} - \frac{1}{18}\right) m_1 u_1^2 = \frac{8}{18} m_1 u_1^2 = \frac{4}{9} m_1 u_1^2 \] ### Step 7: Fraction of Energy Loss The fraction of energy lost by the neutron is given by: \[ \text{Fraction of energy loss} = \frac{\Delta KE}{KE_{initial}} = \frac{\frac{4}{9} m_1 u_1^2}{\frac{1}{2} m_1 u_1^2} = \frac{4/9}{1/2} = \frac{4}{9} \times \frac{2}{1} = \frac{8}{9} \] ### Final Answer The fraction of energy loss of the neutron in the collision is: \[ \frac{8}{9} \]

To solve the problem of the neutron making a head-on elastic collision with a stationary deuteron, we will follow these steps: ### Step 1: Understand the Problem We have a neutron (mass \( m_1 \)) colliding elastically with a stationary deuteron (mass \( m_2 = 2m_1 \)). We need to find the fraction of energy lost by the neutron after the collision. ### Step 2: Conservation of Momentum In an elastic collision, both momentum and kinetic energy are conserved. The conservation of momentum before and after the collision can be expressed as: \[ ...
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