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A neutron collides, head-on with a deute...

A neutron collides, head-on with a deuterium at rest. What fraction of the neutron's energy would be transferred to the deuterium?

A

`89%`

B

`11%`

C

`79%`

D

`21%`

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The correct Answer is:
To solve the problem of determining the fraction of the neutron's energy that is transferred to the deuterium during a head-on elastic collision, we can follow these steps: ### Step 1: Define the masses and initial conditions Let: - Mass of the neutron = \( m \) - Mass of the deuterium (which consists of one proton and one neutron) = \( 2m \) - Initial velocity of the neutron = \( u \) - Initial velocity of the deuterium = \( 0 \) (at rest) ### Step 2: Apply conservation of momentum According to the law of conservation of momentum: \[ \text{Initial momentum} = \text{Final momentum} \] This gives us: \[ mu = mv_1 + 2mv_2 \] where \( v_1 \) is the final velocity of the neutron and \( v_2 \) is the final velocity of the deuterium. We can simplify this equation by dividing through by \( m \): \[ u = v_1 + 2v_2 \tag{1} \] ### Step 3: Apply the coefficient of restitution For an elastic collision, the coefficient of restitution \( e \) is equal to 1. This means: \[ \frac{v_2 - v_1}{u - 0} = 1 \] From this, we can derive: \[ v_2 - v_1 = u \tag{2} \] ### Step 4: Solve equations (1) and (2) Now we have two equations: 1. \( u = v_1 + 2v_2 \) 2. \( v_2 - v_1 = u \) From equation (2), we can express \( v_2 \) in terms of \( v_1 \): \[ v_2 = u + v_1 \tag{3} \] Substituting equation (3) into equation (1): \[ u = v_1 + 2(u + v_1) \] Expanding this gives: \[ u = v_1 + 2u + 2v_1 \] Combining like terms: \[ u = 3v_1 + 2u \] Rearranging gives: \[ 3v_1 = u - 2u = -u \] Thus: \[ v_1 = -\frac{u}{3} \tag{4} \] Now substituting \( v_1 \) back into equation (3) to find \( v_2 \): \[ v_2 = u + \left(-\frac{u}{3}\right) = \frac{3u}{3} - \frac{u}{3} = \frac{2u}{3} \tag{5} \] ### Step 5: Calculate the kinetic energy transferred to deuterium The kinetic energy of the deuterium after the collision is given by: \[ KE_{D} = \frac{1}{2} \times 2m \times v_2^2 = m \left(\frac{2u}{3}\right)^2 = m \times \frac{4u^2}{9} = \frac{4}{9} mu^2 \] The initial kinetic energy of the neutron is: \[ KE_{n} = \frac{1}{2} mu^2 \] ### Step 6: Determine the fraction of energy transferred The fraction of the neutron's energy transferred to the deuterium is: \[ \text{Fraction} = \frac{KE_{D}}{KE_{n}} = \frac{\frac{4}{9} mu^2}{\frac{1}{2} mu^2} = \frac{\frac{4}{9}}{\frac{1}{2}} = \frac{4}{9} \times \frac{2}{1} = \frac{8}{9} \] ### Step 7: Convert to percentage (if needed) To convert this fraction to a percentage: \[ \frac{8}{9} \times 100 \approx 88.89\% \] ### Final Answer The fraction of the neutron's energy that is transferred to the deuterium is approximately \( \frac{8}{9} \) or about 89%. ---

To solve the problem of determining the fraction of the neutron's energy that is transferred to the deuterium during a head-on elastic collision, we can follow these steps: ### Step 1: Define the masses and initial conditions Let: - Mass of the neutron = \( m \) - Mass of the deuterium (which consists of one proton and one neutron) = \( 2m \) - Initial velocity of the neutron = \( u \) - Initial velocity of the deuterium = \( 0 \) (at rest) ...
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