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By Ankit Ankit
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Updated on 29 Oct 2026, 11:48 IST
NCERT Solutions for Class 12 Physics Chapter 13, Nuclei, provide step-by-step answers to all six questions in the NCERT exercise. The chapter deals with the composition and size of the nucleus, mass-energy equivalence, mass defect, nuclear binding energy, nuclear force, radioactivity, fission and fusion.
The solutions below follow the questions from the current NCERT Class 12 Physics textbook and show the calculations clearly, including the formulas, substitutions and final answers. They are useful for checking textbook exercises, understanding numerical methods and revising the main ideas from the chapter.
Chapter 13 begins with the basic structure of the nucleus and then moves into the relationship between mass and energy. Students next study mass defect and binding energy, followed by nuclear reactions such as fission and fusion and the basics of radioactivity.
The chapter includes both conceptual questions and numerical problems. Numericals mainly involve mass defect, binding energy, nuclear radius, Q-value, and nuclear reactions. Questions on nuclear composition, stability, fission, fusion, and radioactivity require students to understand the underlying concepts as well.
The chapter also leads into the next part of Class 12 Physics. Chapter 14, Semiconductor Electronics, shifts from the nucleus to semiconductor materials, electronic devices, and their applications, so the two chapters cover very different areas of modern physics and electronics.
Use these step-by-step solutions alongside the NCERT textbook to check your calculations and understand the method used for each exercise.
For the original exercise questions, always refer to the current NCERT textbook. The questions on this page reproduce the Chapter 13 exercise exactly as given in the 2026–27 reprint.
R = R0A1/3

where R0 = 1.2 × 10−15 m.
When atomic masses are used, the mass defect can be calculated as:

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ΔM = ZmH + (A−Z)mn − M
where:
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Fig. 2 — The bound nucleus has slightly less mass than its separated nucleons; the missing mass ΔM is released as binding energy.

Eb = ΔM c2
Using 1 u = 931.5 MeV/c², we get:
Eb = ΔM × 931.5 MeV
Q = (sum of initial masses − sum of final masses) c2
A positive Q-value indicates an exothermic reaction, while a negative Q-value indicates an endothermic reaction.
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Fig. 3 — Binding energy per nucleon rises sharply for light nuclei, peaks near A ≈ 56–62, then declines slowly — this shape is why fusion of light nuclei and fission of heavy nuclei can both release energy.
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Fig. 4 — Fission splits a heavy nucleus into lighter fragments; fusion combines light nuclei into a heavier, more tightly bound nucleus.
Question 1: Obtain the binding energy (in MeV) of a nitrogen nucleus ¹⁴₇N, given m(¹⁴₇N) = 14.00307 u.
Given
A = 14, Z = 7 ⇒ N = A − Z = 7
mH = 1.007825 u, mn = 1.008665 u
Mass of the separated nucleons
M = ZmH + (A−Z)mn = 7(1.007825) + 7(1.008665)
M = 7.054775 + 7.060655 = 14.115430 u
Mass defect
ΔM = M − m(¹⁴₇N) = 14.115430 − 14.00307 = 0.112360 u
Binding energy
Eb = ΔM × 931.5 = 0.112360 × 931.5 ≈ 104.66 MeV
Answer
Eb ≈ 104.66 MeV
Question 2: Obtain the binding energy of the nuclei ⁵⁶₂₆Fe and ²⁰⁹₈₃Bi in units of MeV from the following data: m(⁵⁶₂₆Fe) = 55.934939 u and m(²⁰⁹₈₃Bi) = 208.980388 u.
For ⁵⁶₂₆Fe
Given
A = 56, Z = 26 ⇒ N = 30
M = 26(1.007825) + 30(1.008665) = 26.20345 + 30.25995 = 56.46340 u
ΔM = 56.46340 − 55.934939 = 0.528461 u
Eb = 0.528461 × 931.5 ≈ 492.26 MeV
For ²⁰⁹₈₃Bi
Given
A = 209, Z = 83 ⇒ N = 126
M = 83(1.007825) + 126(1.008665) = 83.649475 + 127.091790 = 210.741265 u
ΔM = 210.741265 − 208.980388 = 1.760877 u
Eb = 1.760877 × 931.5 ≈ 1640.26 MeV
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Fig. 5 — Fe-56 sits almost exactly at the peak of the binding-energy curve; Bi-209 lies further along the slowly falling right-hand side.
Answer
Eb(⁵⁶Fe) ≈ 492.26 MeV
Eb(²⁰⁹Bi) ≈ 1640.26 MeV
Question 3: A given coin has a mass of 3.0 g. Calculate the nuclear energy that would be required to separate all the neutrons and protons from each other. For simplicity assume that the coin is entirely made of ⁶³₂₉Cu atoms (of mass 62.92960 u).
Given
A = 63, Z = 29 ⇒ N = 34, M = 62.92960 u
Step 1: Mass defect of one copper nucleus
ΔM = ZmH + (A−Z)mn − M = 29(1.007825) + 34(1.008665) − 62.92960
29(1.007825) = 29.227925, 34(1.008665) = 34.294610
ΔM = 29.227925 + 34.294610 − 62.92960 = 0.592935 u
Step 2: Binding energy of one copper nucleus
Eb = 0.592935 × 931.5 ≈ 552.36 MeV
Step 3: Number of copper atoms in the coin
number of moles = 3.0/62.92960 ≈ 0.04767 mol
N = 0.04767 × 6.023 × 1023 ≈ 2.87 × 1022 atoms
Step 4: Total nuclear energy
E(total) = (2.87 × 1022)(552.36 MeV) ≈ 1.58 × 1025 MeV
Using 1 MeV = 1.6 × 10⁻¹³ J:
E(total) = 1.58 × 1025 × 1.6 × 10−13 ≈ 2.53 × 1012 J
Answer
E(total) ≈ 2.53 × 1012 J
Question 4: Obtain approximately the ratio of the nuclear radii of the gold isotope ¹⁹⁷₇₉Au and the silver isotope ¹⁰⁷₄₇Ag.
Given
A(Au) = 197, A(Ag) = 107
Formula
R = R0A1/3 ⇒ R(Au)/R(Ag) = [A(Au)/A(Ag)]1/3
The R₀ terms cancel since both nuclei use the same R₀.
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Fig. 6 — The gold nucleus is larger than the silver nucleus, in proportion to A¹ᵟ³.
Calculation
197/107 ≈ 1.841
R(Au)/R(Ag) ≈ (1.841)1/3 ≈ 1.23
Answer
R(Au)/R(Ag) ≈ 1.23
Question 5: The Q value of a nuclear reaction A + b → C + d is defined by Q = [m(A) + m(b) − m(C) − m(d)]c², where the masses refer to the respective nuclei. Determine from the given data the Q-value of the following reactions and state whether the reactions are exothermic or endothermic. (i) ¹₁H + ³₁H → ²₁H + ²₁H (ii) ¹²₆C + ¹²₆C → ²⁰₁₀Ne + ⁴₂He
Given
m(²H) = 2.014102 u, m(³H) = 3.016049 u
m(¹²C) = 12.000000 u, m(²⁰Ne) = 19.992439 u, m(⁴He) = 4.002603 u
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Fig. 7 — Comparing total mass before and after each reaction shows directly whether Q is positive or negative.
(i) ¹H + ³H → ²H + ²H
Q = [m(¹H) + m(³H) − 2m(²H)]c2 = [1.007825 + 3.016049 − 2(2.014102)]c2
Q = [4.023874 − 4.028204]c2 = −0.004330 u·c2
Q = −0.004330 × 931.5 ≈ −4.03 MeV
The Q-value is negative, so the reaction is endothermic.
(ii) ¹²C + ¹²C → ²⁰Ne + ⁴He
Q = [2m(¹²C) − m(²⁰Ne) − m(⁴He)]c2 = [24.000000 − 19.992439 − 4.002603]c2
Q = [24.000000 − 23.995042]c2 = 0.004958 u·c2
Q = 0.004958 × 931.5 ≈ 4.62 MeV
The Q-value is positive, so the reaction is exothermic.
Answer
(i) Q ≈ −4.03 MeV — endothermic
(ii) Q ≈ +4.62 MeV — exothermic
Question 6: Suppose, we think of fission of a ⁵⁶₂₆Fe nucleus into two equal fragments, ²⁸₁₃Al. Is the fission energetically possible? Argue by working out Q of the process. Given m(⁵⁶₂₆Fe) = 55.93494 u and m(²⁸₁₃Al) = 27.98191 u.
The proposed fission reaction is ⁵⁶Fe → 2 ²⁸Al.
Q-value
Q = [m(⁵⁶Fe) − 2m(²⁸Al)]c2 = [55.93494 − 2(27.98191)]c2
Q = [55.93494 − 55.96382]c2 = −0.02888 u·c2
Q = −0.02888 × 931.5 ≈ −26.90 MeV
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Fig. 8 — The two aluminium fragments together weigh more than the original iron nucleus, so the process would absorb energy rather than release it.
The Q-value is negative. Therefore, the proposed fission does not release energy — instead, approximately 26.90 MeV would have to be supplied for the process to occur.
Answer
Q ≈ −26.90 MeV
Since Q < 0, the fission is not energetically possible as an energy-releasing process.
Most numerical questions in this chapter can be approached systematically.
Step 1: Identify A and Z
For a nuclide ᴬₓX: A gives the total number of nucleons, Z gives the number of protons, and A − Z gives the number of neutrons.
Step 2: Select the appropriate formula
For binding energy:
Eb = ΔM × 931.5 MeV
For nuclear radius:
R = R0A1/3
For a nuclear reaction:
Q = (initial mass − final mass) × 931.5 MeV
Step 3: Keep the units consistent
Masses given in atomic mass units should be used with 1 u = 931.5 MeV/c². If the final answer is required in joules, use 1 MeV = 1.6 × 10⁻¹³ J.
Step 4: Check the sign
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The current NCERT exercise for Chapter 13, Nuclei, contains six questions, numbered 13.1 to 13.6.
The exercise covers binding energy, mass defect, nuclear energy, nuclear radii, Q-value and the energetics of a proposed nuclear fission process.
The binding energy is calculated using: Eb = ΔMc2
When the mass defect is expressed in atomic mass units: Eb = ΔM × 931.5 MeV.
A positive Q-value means that the final state has lower total mass-energy than the initial state, so energy is released in the reaction. The reaction is exothermic.
A negative Q-value means that energy must be supplied for the reaction to occur. The reaction is endothermic.
It gives the energy equivalent of one atomic mass unit using Einstein's mass-energy relation. It allows a mass defect measured in u to be converted directly into energy in MeV.