JEE Challenger
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Radioactive Decay Chain of Thorium to Lead Nucleus

Consider a radioactive decay sequence where a 90232Th^{232}_{90}\text{Th} nucleus transforms into a 82212Pb^{212}_{82}\text{Pb} nucleus. If NαN_\alpha and NβN_\beta represent the total count of α\alpha and β−\beta^- particles emitted throughout this decay chain, select the correct statement(s):

Options

A

Nα=5N_\alpha = 5

Correct
B

Nα=6N_\alpha = 6

C

Nβ=2N_\beta = 2

Correct
D

Nβ=4N_\beta = 4

Step-by-Step Solution

To determine the total number of α\alpha particles (NαN_\alpha) and β−\beta^- particles (NβN_\beta) emitted during the radioactive decay chain, we can write the general nuclear equation for the transformation of a Thorium nucleus (90232Th^{232}_{90}\text{Th}) into a Lead nucleus (82212Pb^{212}_{82}\text{Pb}):

90232Th⟶82212Pb+Nα(24He)+Nβ(−10e)+neutrinos^{232}_{90}\text{Th} \longrightarrow {^{212}_{82}\text{Pb}} + N_\alpha \left(^{4}_{2}\text{He}\right) + N_\beta \left(^{0}_{-1}\text{e}\right) + \text{neutrinos}

By applying the principles of conservation of mass number (AA) and atomic number (ZZ):

1. Conservation of Mass Number (AA):

The total mass number must be conserved before and after the decay process: 232=212+4Nα+0⋅Nβ232 = 212 + 4 N_\alpha + 0 \cdot N_\beta

Solving for NαN_\alpha: 232−212=4Nα232 - 212 = 4 N_\alpha 20=4Nα  ⟹  Nα=520 = 4 N_\alpha \implies N_\alpha = 5

2. Conservation of Atomic Number (ZZ):

The total atomic number (charge) must also be conserved: 90=82+2Nα−1⋅Nβ90 = 82 + 2 N_\alpha - 1 \cdot N_\beta

Substituting Nα=5N_\alpha = 5 into the equation: 90=82+2(5)−Nβ90 = 82 + 2(5) - N_\beta 90=82+10−Nβ90 = 82 + 10 - N_\beta 90=92−Nβ  ⟹  Nβ=290 = 92 - N_\beta \implies N_\beta = 2

Thus, the total number of α\alpha particles emitted is Nα=5N_\alpha = 5 and the total number of β−\beta^- particles emitted is Nβ=2N_\beta = 2.

Correct Options:

  • (A) Nα=5N_\alpha = 5
  • (C) Nβ=2N_\beta = 2