JEE Challenger
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Kinematics and Energetics of Binary Nuclear Fission

A heavy parent nucleus NN, initially at rest, undergoes fission into two lighter daughter nuclei via N→P+QN \rightarrow P + Q. Let mass defect be δ=MN−MP−MQ\delta = M_N - M_P - M_Q, where MPM_P, MQM_Q, and MNM_N represent the rest masses of PP, QQ, and NN, respectively. Let EPE_P and EQE_Q denote the kinetic energies of PP and QQ, while vPv_P and vQv_Q are their corresponding speeds. If cc is the speed of light, which of the following statement(s) is/are correct?

Options

A

EP+EQ=c2δE_P + E_Q = c^2 \delta

Correct
B

EP=(MPMP+MQ)c2δE_P = \left( \frac{M_P}{M_P + M_Q} \right) c^2 \delta

C

vPvQ=MQMP\frac{v_P}{v_Q} = \frac{M_Q}{M_P}

Correct
D

The magnitude of momentum for PP as well as QQ is c2μδc \sqrt{2\mu \delta}, where reduced mass μ=MPMQ(MP+MQ)\mu = \frac{M_P M_Q}{(M_P + M_Q)}

Correct

Topics & Concepts

Step-by-Step Solution

To determine the correct statements, we analyze the energetics and kinematics of the binary nuclear fission reaction N→P+QN \rightarrow P + Q, where the heavy parent nucleus NN is initially at rest.

1. Conservation of Energy

The total energy before the fission process is equal to the total energy after the process. Total initial energy=MNc2\text{Total initial energy} = M_N c^2 Total final energy=MPc2+MQc2+EP+EQ\text{Total final energy} = M_P c^2 + M_Q c^2 + E_P + E_Q

Applying the law of conservation of energy: MNc2=MPc2+MQc2+EP+EQM_N c^2 = M_P c^2 + M_Q c^2 + E_P + E_Q

Rearranging the terms in terms of the mass defect δ=MN−MP−MQ\delta = M_N - M_P - M_Q: EP+EQ=(MN−MP−MQ)c2=δc2E_P + E_Q = (M_N - M_P - M_Q) c^2 = \delta c^2

This confirms that Statement (A) is correct.


2. Conservation of Linear Momentum

Since the parent nucleus NN is initially at rest, the total initial momentum of the system is zero. By conservation of linear momentum: p⃗P+p⃗Q=0  ⟹  p⃗P=−p⃗Q\vec{p}_P + \vec{p}_Q = 0 \implies \vec{p}_P = -\vec{p}_Q

Taking the magnitude of momentum for both daughter nuclei: ∣p⃗P∣=∣p⃗Q∣=p|\vec{p}_P| = |\vec{p}_Q| = p

Using the non-relativistic expression for momentum (p=Mvp = M v): MPvP=MQvQ  ⟹  vPvQ=MQMPM_P v_P = M_Q v_Q \implies \frac{v_P}{v_Q} = \frac{M_Q}{M_P}

This confirms that Statement (C) is correct.


3. Kinetic Energies and Reduced Mass

The kinetic energy of each daughter nucleus in terms of momentum pp is given by: EP=p22MPandEQ=p22MQE_P = \frac{p^2}{2 M_P} \quad \text{and} \quad E_Q = \frac{p^2}{2 M_Q}

The total kinetic energy is: EP+EQ=p22MP+p22MQ=p22(1MP+1MQ)=p22(MP+MQMPMQ)E_P + E_Q = \frac{p^2}{2 M_P} + \frac{p^2}{2 M_Q} = \frac{p^2}{2} \left( \frac{1}{M_P} + \frac{1}{M_Q} \right) = \frac{p^2}{2} \left( \frac{M_P + M_Q}{M_P M_Q} \right)

Defining the reduced mass μ=MPMQMP+MQ\mu = \frac{M_P M_Q}{M_P + M_Q}, we have: EP+EQ=p22μE_P + E_Q = \frac{p^2}{2\mu}

Equating this to the total energy released δc2\delta c^2: p22μ=δc2  ⟹  p2=2μδc2  ⟹  p=c2μδ\frac{p^2}{2\mu} = \delta c^2 \implies p^2 = 2 \mu \delta c^2 \implies p = c \sqrt{2 \mu \delta}

This confirms that Statement (D) is correct.


4. Kinetic Energy of PP

Using the magnitude of momentum derived above, the kinetic energy of fragment PP is: EP=p22MP=2μδc22MP=μMPδc2=(MQMP+MQ)δc2E_P = \frac{p^2}{2 M_P} = \frac{2 \mu \delta c^2}{2 M_P} = \frac{\mu}{M_P} \delta c^2 = \left( \frac{M_Q}{M_P + M_Q} \right) \delta c^2

Therefore, Statement (B) is incorrect because it has MPM_P instead of MQM_Q in the numerator.


Conclusion

The correct options are A, C, and D.