The fission of uranium nuclei in a nuclear reactor produces high speed neutrons. Before a neutron can trigger additional fissions, it has to be slowed down by collisions with carbon nuclei in the moderator of the reactor. Suppose a neutron with mass of 1.0u travelling at 2.0x107m/s undergoes a head-on elastic collision with a carbon nucleus with mass of 12u initially at rest. Calculate the velocities of the neutron and carbon after the collision.
Let us write the conservation of momentum law:
"m_n v_{n,0} + m_cv_{c,0} = m_n v_{n,1} + m_cv_{c,1}" where "v_{c,0}=0."
"m_n v_{n,0} = m_n v_{n,1} + m_cv_{c,1}"
Due to elastic collision, the energy is conserved, so
"\\dfrac{m_n v_{n,0}^2}{2} + \\dfrac{m_cv_{c,0} ^2}{2}= \\dfrac{m_n v_{n,1}^2}{2} + \\dfrac{m_cv_{c,1}^2}{2}" or "m_n v_{n,0}^2 = m_n v_{n,1}^2 + m_cv_{c,1}^2".
So we have a system of equations
"\\begin{cases}\nm_n v_{n,0} = m_n v_{n,1} + m_cv_{c,1},\\\\\nm_n v_{n,0}^2 = m_n v_{n,1}^2 + m_cv_{c,1}^2\n\\end{cases},"
"\\begin{cases}\n1 v_{n,0} = 1 v_{n,1} + 12v_{c,1},\\\\\n1 v_{n,0}^2 = 1 v_{n,1}^2 + 12v_{c,1}^2\n\\end{cases}"
We solve these equation by substituting "v_{n,1} =v_{n,0} - 12v_{c,1}" into the second equation and get "v_{c,1} = \\dfrac{2}{13}v_0 = \\dfrac{2}{13}\\cdot 2.0\\cdot10^7\\,\\mathrm{m\/s}= 3.1\\cdot10^6\\,\\mathrm{m\/s}" .
"v_{n,1} = v_{n,0} - 12\\cdot v_{c,1} = -1.7\\cdot10^7\\,\\mathrm{m\/s}."
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