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A neutron collides elastically with an initially stationary deuteron. Find the fraction of the kinetic energy lost by the neutron in a head-on collision?

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To solve the problem of finding the fraction of kinetic energy lost by the neutron in a head-on elastic collision with a stationary deuteron, we will follow these steps: ### Step 1: Define the masses and initial velocities Let: - Mass of the neutron, \( m_1 = m \) - Mass of the deuteron, \( m_2 = 2m \) (since a deuteron consists of one proton and one neutron) - Initial velocity of the neutron, \( u_1 = u \) - Initial velocity of the deuteron, \( u_2 = 0 \) (since it is stationary) ### Step 2: Apply conservation of momentum According to the conservation of momentum: \[ m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2 \] Substituting the values: \[ m u + 2m \cdot 0 = m v_1 + 2m v_2 \] This simplifies to: \[ u = v_1 + 2v_2 \quad \text{(1)} \] ### Step 3: Apply conservation of kinetic energy According to the conservation of kinetic energy: \[ \frac{1}{2} m_1 u_1^2 + \frac{1}{2} m_2 u_2^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2 \] Substituting the values: \[ \frac{1}{2} m u^2 + 0 = \frac{1}{2} m v_1^2 + \frac{1}{2} (2m) v_2^2 \] This simplifies to: \[ u^2 = v_1^2 + 2v_2^2 \quad \text{(2)} \] ### Step 4: Solve the equations From equation (1): \[ v_1 = u - 2v_2 \] Substituting \( v_1 \) in equation (2): \[ u^2 = (u - 2v_2)^2 + 2v_2^2 \] Expanding the square: \[ u^2 = u^2 - 4uv_2 + 4v_2^2 + 2v_2^2 \] This simplifies to: \[ 0 = -4uv_2 + 6v_2^2 \] Factoring out \( v_2 \): \[ v_2(6v_2 - 4u) = 0 \] Since \( v_2 \neq 0 \): \[ 6v_2 = 4u \implies v_2 = \frac{2u}{3} \] ### Step 5: Find \( v_1 \) Substituting \( v_2 \) back into equation (1): \[ v_1 = u - 2\left(\frac{2u}{3}\right) = u - \frac{4u}{3} = -\frac{u}{3} \] ### Step 6: Calculate the kinetic energy loss The initial kinetic energy of the neutron: \[ KE_{initial} = \frac{1}{2} m u^2 \] The final kinetic energy of the neutron: \[ KE_{final} = \frac{1}{2} m v_1^2 = \frac{1}{2} m \left(-\frac{u}{3}\right)^2 = \frac{1}{2} m \frac{u^2}{9} = \frac{m u^2}{18} \] The kinetic energy lost by the neutron: \[ \Delta KE = KE_{initial} - KE_{final} = \frac{1}{2} m u^2 - \frac{m u^2}{18} \] Finding a common denominator (which is 18): \[ \Delta KE = \frac{9}{18} m u^2 - \frac{1}{18} m u^2 = \frac{8}{18} m u^2 = \frac{4}{9} m u^2 \] ### Step 7: Calculate the fraction of kinetic energy lost The fraction of kinetic energy lost by the neutron is: \[ \text{Fraction} = \frac{\Delta KE}{KE_{initial}} = \frac{\frac{4}{9} m u^2}{\frac{1}{2} m u^2} = \frac{\frac{4}{9}}{\frac{1}{2}} = \frac{4}{9} \cdot \frac{2}{1} = \frac{8}{9} \] ### Final Answer The fraction of the kinetic energy lost by the neutron in the collision is \( \frac{8}{9} \). ---

To solve the problem of finding the fraction of kinetic energy lost by the neutron in a head-on elastic collision with a stationary deuteron, we will follow these steps: ### Step 1: Define the masses and initial velocities Let: - Mass of the neutron, \( m_1 = m \) - Mass of the deuteron, \( m_2 = 2m \) (since a deuteron consists of one proton and one neutron) - Initial velocity of the neutron, \( u_1 = u \) - Initial velocity of the deuteron, \( u_2 = 0 \) (since it is stationary) ...
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