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Question: In a particle accelerator, a neutron moving with velocity v ≈ 2 × 103 m/s collides elastically with ...

In a particle accelerator, a neutron moving with velocity v ≈ 2 × 103 m/s collides elastically with a C-12 nucleus at rest. Assuming head-on collision, the fraction a of neutron's kinetic energy transferred to the carbon nucleus is (Ignore relativistic effects)

Answer

48/169

Explanation

Solution

In a head-on elastic collision between a neutron (mass mnm_n) moving with velocity vnv_n and a C-12 nucleus (mass mCm_C) at rest (vC=0v_C = 0), both linear momentum and kinetic energy are conserved.

Conservation of linear momentum:

mnvn+mCvC=mnvn+mCvCm_n v_n + m_C v_C = m_n v_n' + m_C v_C'

mnvn=mnvn+mCvCm_n v_n = m_n v_n' + m_C v_C' (since vC=0v_C = 0)

Conservation of kinetic energy:

12mnvn2+12mCvC2=12mnvn2+12mCvC2\frac{1}{2} m_n v_n^2 + \frac{1}{2} m_C v_C^2 = \frac{1}{2} m_n v_n'^2 + \frac{1}{2} m_C v_C'^2

12mnvn2=12mnvn2+12mCvC2\frac{1}{2} m_n v_n^2 = \frac{1}{2} m_n v_n'^2 + \frac{1}{2} m_C v_C'^2 (since vC=0v_C = 0)

Solving these two equations for the final velocities vnv_n' and vCv_C' gives:

vC=2mnmn+mCvnv_C' = \frac{2 m_n}{m_n + m_C} v_n

The initial kinetic energy of the neutron is Kn=12mnvn2K_n = \frac{1}{2} m_n v_n^2.

The kinetic energy transferred to the carbon nucleus is its final kinetic energy, KC=12mCvC2K_C' = \frac{1}{2} m_C v_C'^2.

The fraction α\alpha of the neutron's kinetic energy transferred to the carbon nucleus is:

α=KCKn=12mCvC212mnvn2=mCmn(vCvn)2\alpha = \frac{K_C'}{K_n} = \frac{\frac{1}{2} m_C v_C'^2}{\frac{1}{2} m_n v_n^2} = \frac{m_C}{m_n} \left(\frac{v_C'}{v_n}\right)^2

Substitute the expression for vC/vnv_C'/v_n:

α=mCmn(2mnmn+mCvnvn)2=mCmn(2mnmn+mC)2=4mn2mCmn(mn+mC)2=4mnmC(mn+mC)2\alpha = \frac{m_C}{m_n} \left(\frac{\frac{2 m_n}{m_n + m_C} v_n}{v_n}\right)^2 = \frac{m_C}{m_n} \left(\frac{2 m_n}{m_n + m_C}\right)^2 = \frac{4 m_n^2 m_C}{m_n (m_n + m_C)^2} = \frac{4 m_n m_C}{(m_n + m_C)^2}

The mass of a C-12 nucleus is approximately 12 times the mass of a neutron (mC12mnm_C \approx 12 m_n). Let mn=mm_n = m and mC=12mm_C = 12m.

α=4m(12m)(m+12m)2=48m2(13m)2=48m2169m2=48169\alpha = \frac{4 m (12m)}{(m + 12m)^2} = \frac{48 m^2}{(13m)^2} = \frac{48 m^2}{169 m^2} = \frac{48}{169}

Therefore, the fraction of neutron's kinetic energy transferred to the carbon nucleus is 48169\frac{48}{169}. The initial velocity value is not needed for this calculation.