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Question: An alpha particle with kinetic energy K just initiates a nuclear reaction with element X. This being...

An alpha particle with kinetic energy K just initiates a nuclear reaction with element X. This being an endothermic reaction with Q-value of magnitude E0E_0. In another nuclear reaction neutron with same kinetic energy K initiates same nuclear reaction, which is endothermic reaction of Q value of magnitude 1916E0\frac{19}{16}E_0. Atomic mass of X is

Answer

15 u

Explanation

Solution

The threshold kinetic energy (KthK_{th}) of a projectile particle with mass mpm_p incident on a target nucleus with mass mTm_T to initiate an endothermic nuclear reaction with Q-value QQ is given by: Kth=Q(1+mpmT)K_{th} = -Q \left(1 + \frac{m_p}{m_T}\right)

In this problem, the target nucleus is element X, with atomic mass mXm_X. The projectile in the first case is an alpha particle (α\alpha) with mass mαm_\alpha. The reaction is endothermic with Q-value magnitude E0E_0, so Qα=E0Q_\alpha = -E_0. The kinetic energy KK initiates the reaction, meaning KK is the threshold energy for the alpha particle: K=Qα(1+mαmX)=E0(1+mαmX)K = -Q_\alpha \left(1 + \frac{m_\alpha}{m_X}\right) = E_0 \left(1 + \frac{m_\alpha}{m_X}\right) --- (1)

In the second case, the projectile is a neutron (nn) with mass mnm_n. The reaction is endothermic with Q-value magnitude 1916E0\frac{19}{16}E_0, so Qn=1916E0Q_n = -\frac{19}{16}E_0. The kinetic energy KK initiates the same nuclear reaction, implying KK is also the threshold energy for the neutron: K=Qn(1+mnmX)=1916E0(1+mnmX)K = -Q_n \left(1 + \frac{m_n}{m_X}\right) = \frac{19}{16}E_0 \left(1 + \frac{m_n}{m_X}\right) --- (2)

For JEE and NEET exams, the atomic masses of common particles are often approximated as: Mass of alpha particle (mαm_\alpha) 4\approx 4 atomic mass units (u). Mass of neutron (mnm_n) 1\approx 1 atomic mass unit (u).

Equating the expressions for KK from (1) and (2): E0(1+mαmX)=1916E0(1+mnmX)E_0 \left(1 + \frac{m_\alpha}{m_X}\right) = \frac{19}{16}E_0 \left(1 + \frac{m_n}{m_X}\right)

Since E0>0E_0 > 0 (as it's a magnitude of Q-value for an endothermic reaction), we can cancel E0E_0: 1+mαmX=1916(1+mnmX)1 + \frac{m_\alpha}{m_X} = \frac{19}{16} \left(1 + \frac{m_n}{m_X}\right)

Substitute the approximate masses mα=4m_\alpha = 4 u and mn=1m_n = 1 u: 1+4mX=1916(1+1mX)1 + \frac{4}{m_X} = \frac{19}{16} \left(1 + \frac{1}{m_X}\right) 1+4mX=1916+1916mX1 + \frac{4}{m_X} = \frac{19}{16} + \frac{19}{16m_X}

Rearrange the terms to solve for mXm_X: 4mX1916mX=19161\frac{4}{m_X} - \frac{19}{16m_X} = \frac{19}{16} - 1

Combine terms on both sides: 4×161916mX=191616\frac{4 \times 16 - 19}{16m_X} = \frac{19 - 16}{16} 641916mX=316\frac{64 - 19}{16m_X} = \frac{3}{16} 4516mX=316\frac{45}{16m_X} = \frac{3}{16}

Multiply both sides by 16mX16m_X: 45=3mX45 = 3m_X

Solve for mXm_X: mX=453=15m_X = \frac{45}{3} = 15

Therefore, the atomic mass of element X is 15 atomic mass units.