Class 12 Physics | Unit VIII
Chapter 13: Nuclei
Nuclear Properties • Mass Defect • Binding Energy • Radioactivity • Fission & Fusion
1. Composition & Size of Nucleus
Nucleus: Contains protons (Z) and neutrons (N). Together
called nucleons (A = Z + N). A = mass number, Z = atomic number.
Nuclear radius: R = R0A1/3 where R0 = 1.2 fm =
1.2×10−15 m
Nuclear volume: V = (4/3)πR³ ∝ A
Nuclear density: ρ = 3mp/(4πR0³) ≈ 2.3×1017 kg/m³ (constant for all nuclei!)
Nuclear volume: V = (4/3)πR³ ∝ A
Nuclear density: ρ = 3mp/(4πR0³) ≈ 2.3×1017 kg/m³ (constant for all nuclei!)
- Nuclear density is same for all nuclei → nucleons are uniformly distributed and tightly packed.
- 1 fm = 10−15 m (fermi). Nucleus radius: ~1–10 fm depending on A.
1.1 Important Terminology
| Term | Definition | Example |
|---|---|---|
| Isotopes | Same Z, different A (same element) | ¹H, ²H (D), ³H (T) |
| Isobars | Same A, different Z (diff elements) | ³₁H and ³₂He |
| Isotones | Same N, different Z | ¹₄C and ¹₅N (both N=8) |
| Isomers | Same Z and A, different energy states | Nuclear excited states |
2. Mass Defect & Binding Energy
Mass defect (Δm): The mass of a nucleus is always LESS than the sum of masses of its
individual nucleons. This “missing mass” is converted to binding energy via E=mc².
Mass defect:
Δm = [Zmp + (A−Z)mn] − Mnucleus
Binding Energy:
BE = Δm × c² = Δm × 931.5 MeV/u
1 u (atomic mass unit) = 1.66×10−27 kg = 931.5 MeV/c²
Binding Energy per nucleon:
BE/A = measure of nuclear stability. Higher BE/A = more stable nucleus.
Δm = [Zmp + (A−Z)mn] − Mnucleus
Binding Energy:
BE = Δm × c² = Δm × 931.5 MeV/u
1 u (atomic mass unit) = 1.66×10−27 kg = 931.5 MeV/c²
Binding Energy per nucleon:
BE/A = measure of nuclear stability. Higher BE/A = more stable nucleus.
2.1 BE/A Curve — Key Features
- Maximum BE/A ≈ 8.75 MeV/nucleon at A ≈ 56 (56Fe — most stable nucleus).
- Light nuclei (A<20): BE/A increases rapidly. Notable peaks at ⁴He, ¹²C, ¹⁶O (magic numbers).
- Medium nuclei (A = 30–120): BE/A ≈ 8.0–8.75 (relatively flat — most stable region).
- Heavy nuclei (A>120): BE/A decreases slowly to ~7.6 MeV for uranium.
- Implication: Light nuclei can gain stability by fusion (moving right → higher BE/A). Heavy nuclei gain stability by fission (moving left → higher BE/A). Both release energy!
⚠️ NEET: Δm = [Zmp+(A−Z)mn]−M. BE =
Δm×931.5 MeV. 1u = 931.5 MeV/c². Fe-56 = most stable. Higher BE/A = more stable. Density of
ALL nuclei = 2.3×1017 kg/m³.
3. Nuclear Force
Nuclear force: The strong attractive force that holds nucleons together inside the nucleus.
It is the strongest force in nature.
- Short range: Effective only up to ~2–3 fm. Beyond this, it drops to zero rapidly.
- Charge independent: Same between p-p, n-n, and p-n pairs.
- Strongest force: ~100× stronger than electromagnetic force at nuclear distances.
- Attractive but becomes repulsive at very short distances (<0.7 fm) → prevents nucleons from collapsing.
- Saturated: Each nucleon interacts only with its nearest neighbours (not all other nucleons). This explains constant nuclear density and near-constant BE/A.
- NOT a central force (unlike gravity and Coulomb). Depends on spin and other quantum properties.
4. Radioactivity
Radioactivity: Spontaneous disintegration of unstable nuclei with emission of radiation
(α, β, γ). Discovered by Henri Becquerel (1896). Further studied by Marie
and Pierre Curie.
4.1 Types of Radioactive Decay
| Property | α-decay | β−-decay | γ-decay |
|---|---|---|---|
| Particle | ⁴₂He (helium nucleus) | e− + antineutrino | Photon (γ-ray) |
| Charge | +2e | −e | 0 |
| Mass | 4u | ~0 | 0 |
| Z change | Z → Z−2 | Z → Z+1 | No change |
| A change | A → A−4 | No change | No change |
| Penetration | Low (paper stops) | Medium (Al sheet stops) | High (lead/concrete) |
| Ionisation | Highest | Medium | Lowest |
| Speed | ~c/10 | ~0.9c | c |
4.2 Nuclear Reactions
α-decay: AZX → A−4Z−2Y +
42He
β−-decay: AZX → AZ+1Y + e− + ν̄ (neutron → proton + electron + antineutrino)
β+-decay: AZX → AZ−1Y + e+ + ν (proton → neutron + positron + neutrino)
γ-decay: AZX* → AZX + γ (excited nucleus → ground state + photon)
β−-decay: AZX → AZ+1Y + e− + ν̄ (neutron → proton + electron + antineutrino)
β+-decay: AZX → AZ−1Y + e+ + ν (proton → neutron + positron + neutrino)
γ-decay: AZX* → AZX + γ (excited nucleus → ground state + photon)
5. Radioactive Decay Law
N(t) = N0 e−λt (exponential decay)
Activity: A = λN = A0e−λt = dN/dt
Units: 1 Becquerel (Bq) = 1 decay/s | 1 Curie (Ci) = 3.7×1010 decays/s
Half-life: T1/2 = ln2/λ = 0.693/λ
After n half-lives: N = N0/2n = N0(1/2)n
Mean life: τ = 1/λ = T1/2/0.693 = 1.44×T1/2
λ = decay constant (probability of decay per unit time)
Activity: A = λN = A0e−λt = dN/dt
Units: 1 Becquerel (Bq) = 1 decay/s | 1 Curie (Ci) = 3.7×1010 decays/s
Half-life: T1/2 = ln2/λ = 0.693/λ
After n half-lives: N = N0/2n = N0(1/2)n
Mean life: τ = 1/λ = T1/2/0.693 = 1.44×T1/2
λ = decay constant (probability of decay per unit time)
- After 1 half-life: 50% remains. After 2: 25%. After 3: 12.5%. After n: (1/2)n.
- Radioactive decay is a statistical (probabilistic) process. We cannot predict when a particular nucleus will decay.
- Half-life is independent of initial amount and external conditions (temperature, pressure, etc.).
⚠️ NEET (Very frequently asked!): N=N0e−λt.
T1/2=0.693/λ. After n half-lives: N0/2n. Mean life =
1.44×T1/2. Activity A=λN. 1 Ci=3.7×1010 Bq.
6. Nuclear Fission
Nuclear fission: A heavy nucleus splits into two lighter nuclei (of comparable mass) with
release of energy and 2–3 neutrons. Discovered by Hahn and Strassmann (1938).
Example: 235U + n → 141Ba + 92Kr + 3n + ~200
MeV
Energy released per fission of U-235 ≈ 200 MeV
The released neutrons can cause further fission → chain reaction.
Energy released per fission of U-235 ≈ 200 MeV
The released neutrons can cause further fission → chain reaction.
- Critical mass: Minimum mass of fissile material needed for a sustained chain reaction.
- Controlled fission: Nuclear reactor (moderator: heavy water/graphite slows neutrons; control rods: cadmium/boron absorb excess neutrons).
- Uncontrolled fission: Atomic bomb.
- Fissile materials: U-235, Pu-239, U-233.
7. Nuclear Fusion
Nuclear fusion: Two light nuclei combine to form a heavier nucleus with release of energy.
Requires extremely high temperature (~107 K) → called thermonuclear
reaction.
Proton-proton cycle (Sun):
4 1H → 4He + 2e+ + 2ν + 26.7 MeV
Energy per fusion ≈ 26.7 MeV (for 4 protons → 1 He)
4 1H → 4He + 2e+ + 2ν + 26.7 MeV
Energy per fusion ≈ 26.7 MeV (for 4 protons → 1 He)
- Energy per nucleon from fusion (~6.7 MeV/nucleon) > fission (~0.85 MeV/nucleon). Fusion releases MORE energy per unit mass!
- Fusion is energy source of all stars including our Sun.
- Hydrogen bomb uses uncontrolled fusion (triggered by fission bomb).
- Controlled fusion not yet achieved on Earth (plasma confinement is the challenge).
7.1 Fission vs Fusion
| Feature | Fission | Fusion |
|---|---|---|
| Nuclei | Heavy → lighter | Light → heavier |
| Energy/reaction | ~200 MeV | ~26.7 MeV |
| Energy/nucleon | ~0.85 MeV | ~6.7 MeV |
| Condition | Neutron bombardment | ~107 K temperature |
| Waste | Radioactive (dangerous) | Helium (safe) |
| Control | Achieved (reactors) | Not yet achieved |
🎓 NEET Previous Year Questions
Q1. [NEET 2022] After 3 half-lives, what fraction of radioactive substance remains?
Answer N/N0 = (1/2)³ =
1/8. So 7/8 has decayed.
Q2. [NEET 2021] The binding energy per nucleon is maximum for:
Answer Fe-56 (iron). BE/A ≈
8.75 MeV/nucleon. Most stable nucleus.
Q3. [NEET 2020] In β− decay, what happens inside the nucleus?
Answer A neutron converts to a
proton: n → p + e− + ν̄. Z increases by 1, A unchanged.
Q4. [NEET 2019] The radius of a nucleus with mass number A is proportional to:
Answer R = R0A1/3. So R ∝
A1/3.
Q5. [NEET 2017] Half-life of a substance is 30 min. How long for 75% to decay?
Answer 75% decayed → 25% left = 1/4 =
(1/2)². So n=2 half-lives = 60 minutes.
💡 Rapid Revision
- R=R0A1/3 | ρ=2.3×1017 kg/m³ (constant!) | 1u=931.5 MeV/c²
- Δm=[Zmp+(A−Z)mn]−M | BE=Δm×931.5 MeV | Fe-56: max BE/A
- α: Z−2, A−4 | β⁻: Z+1, A same | γ: no change in Z or A
- N=N0e−λt | T1/2=0.693/λ | τ=1.44T1/2 | After n T1/2: N0/2n
- Fission: heavy→light (~200 MeV) | Fusion: light→heavy (~26.7 MeV)
- Nuclear force: strongest, short range (~2–3 fm), charge independent
CLASS 12 PHYSICS | NCERT SOLUTIONS
Chapter 13 — Nuclei
22 NCERT Exercise & Exemplar Questions — Step-by-Step Solutions
Key Formulas: R=R0A1/3 |
Δm=[Zmp+(A−Z)mn]−M | BE=Δm×931.5 MeV |
N=N0e−λt | T1/2=0.693/λ | 1u=931.5 MeV/c²
📝 NCERT Exercise Questions (Q1 – Q12)
3 MarksQ1 (Ex 13.1). Find the radius of
197Au and 107Ag nuclei. (R0=1.2 fm)
✓ Solution
R = R0A1/3
Au (A=197): R = 1.2×(197)1/3 = 1.2×5.818 = 6.98 fm
R = R0A1/3
Au (A=197): R = 1.2×(197)1/3 = 1.2×5.818 = 6.98 fm
Ag (A=107): R = 1.2×(107)1/3 = 1.2×4.745
= 5.69 fm
3 MarksQ2 (Ex 13.2). Find the binding energy per
nucleon of 56Fe. Given: m(Fe) = 55.934939 u, mp=1.007825 u, mn=1.008665
u.
✓ Solution
Z=26, A=56, N=30
Δm = 26×1.007825 + 30×1.008665 − 55.934939
= 26.20345 + 30.25995 − 55.934939 = 56.4634 − 55.934939 = 0.528461 u
BE = 0.528461×931.5 = 492.26 MeV
Z=26, A=56, N=30
Δm = 26×1.007825 + 30×1.008665 − 55.934939
= 26.20345 + 30.25995 − 55.934939 = 56.4634 − 55.934939 = 0.528461 u
BE = 0.528461×931.5 = 492.26 MeV
BE/A = 492.26/56 = 8.79 MeV/nucleon (highest — most
stable!)
3 MarksQ3 (Ex 13.3). A radioactive isotope has
half-life of 5 years. How long for its activity to reduce to 3.125% of original?
✓ Solution
3.125% = 3.125/100 = 1/32 = (1/2)5
So n = 5 half-lives
3.125% = 3.125/100 = 1/32 = (1/2)5
So n = 5 half-lives
t = 5×T1/2 = 5×5 = 25 years
3 MarksQ4 (Ex 13.4). α-particle has KE = 5.5
MeV. Find distance of closest approach to gold nucleus (Z=79).
✓ Solution
At closest approach: KE = k×(2e)(Ze)/d ⇒ d = 2kZe²/KE
d = 2×9×109×79×(1.6×10−19)²/(5.5×106×1.6×10−19)
= 2×9×109×79×2.56×10−38/(8.8×10−13)
At closest approach: KE = k×(2e)(Ze)/d ⇒ d = 2kZe²/KE
d = 2×9×109×79×(1.6×10−19)²/(5.5×106×1.6×10−19)
= 2×9×109×79×2.56×10−38/(8.8×10−13)
d = 4.13×10−14 m ≈ 41.3 fm
3 MarksQ5 (Ex 13.5). The half-life of 90Sr
is 28 years. Find disintegration rate of 15 mg sample.
✓ Solution
N = (15×10−3/90)×6.023×1023 = 1.004×1020 atoms
λ = 0.693/T1/2 = 0.693/(28×365.25×24×3600) = 0.693/8.83×108 = 7.847×10−10 s−1
N = (15×10−3/90)×6.023×1023 = 1.004×1020 atoms
λ = 0.693/T1/2 = 0.693/(28×365.25×24×3600) = 0.693/8.83×108 = 7.847×10−10 s−1
A = λN =
7.847×10−10×1.004×1020 =
7.878×1010 decays/s ≈ 7.88×1010 Bq
= 7.88×1010/3.7×1010 = 2.13 Ci3 MarksQ6 (Ex 13.6). Find energy released in
α-decay: 226Ra → 222Rn + 4He. Masses: Ra=226.02540 u,
Rn=222.01750 u, He=4.00260 u.
✓ Solution
Δm = m(Ra) − [m(Rn) + m(He)] = 226.02540 − (222.01750 + 4.00260)
= 226.02540 − 226.02010 = 0.0053 u
Δm = m(Ra) − [m(Rn) + m(He)] = 226.02540 − (222.01750 + 4.00260)
= 226.02540 − 226.02010 = 0.0053 u
Q = 0.0053×931.5 = 4.94 MeV
3 MarksQ7 (Ex 13.7). How many α and β
particles are emitted when 232Th decays to 208Pb?
✓ Solution
Change in A: 232−208 = 24. Each α reduces A by 4 → number of α = 24/4 = 6
Change in Z: Th(90)→Pb(82). 6α would reduce Z by 12 → Z = 90−12 = 78.
But final Z=82 → need 82−78 = 4 increases ⇒ 4 β− particles
Change in A: 232−208 = 24. Each α reduces A by 4 → number of α = 24/4 = 6
Change in Z: Th(90)→Pb(82). 6α would reduce Z by 12 → Z = 90−12 = 78.
But final Z=82 → need 82−78 = 4 increases ⇒ 4 β− particles
6 α-particles and 4 β−-particles
3 MarksQ8 (Ex 13.8). Calculate the energy released in
the fusion reaction: 4 ¹H → ⁴He + 2e+ + 2ν. Masses: H=1.007825 u,
He=4.002603 u.
✓ Solution
Δm = 4×1.007825 − 4.002603 = 4.0313 − 4.002603 = 0.028697 u
(Positron mass included in atomic masses)
Δm = 4×1.007825 − 4.002603 = 4.0313 − 4.002603 = 0.028697 u
(Positron mass included in atomic masses)
Q = 0.028697×931.5 = 26.72 MeV
3 MarksQ9 (Ex 13.9). Calculate the energy released
per fission of 235U if products are 141Ba + 92Kr + 3n. Masses:
U=235.04393, Ba=140.91440, Kr=91.92630, n=1.00867 u.
✓ Solution
Δm = [m(U)+m(n)] − [m(Ba)+m(Kr)+3m(n)]
= (235.04393+1.00867) − (140.91440+91.92630+3×1.00867)
= 236.0526 − (140.91440+91.92630+3.02601) = 236.0526 − 235.86671 = 0.18589 u
Δm = [m(U)+m(n)] − [m(Ba)+m(Kr)+3m(n)]
= (235.04393+1.00867) − (140.91440+91.92630+3×1.00867)
= 236.0526 − (140.91440+91.92630+3.02601) = 236.0526 − 235.86671 = 0.18589 u
Q = 0.18589×931.5 = 173.2 MeV (≈200 MeV including
γ-rays and KE)
3 MarksQ10 (Ex 13.10). A radioactive sample has
activity of 1000 disintegrations/min. After 5 min, activity is 500 disintegrations/min. Find (a) decay
constant, (b) half-life.
✓ Solution
A = A0e−λt ⇒ 500 = 1000×e−5λ
e−5λ = 0.5 ⇒ −5λ = ln(0.5) = −0.693
(a) λ = 0.693/5 = 0.1386 per min
A = A0e−λt ⇒ 500 = 1000×e−5λ
e−5λ = 0.5 ⇒ −5λ = ln(0.5) = −0.693
(a) λ = 0.693/5 = 0.1386 per min
(b) T1/2 = 0.693/λ = 0.693/0.1386 = 5
min
(Activity halved in 5 min → T1/2=5 min, as expected.)3 MarksQ11 (Ex 13.11). Nuclear density is constant
for all nuclei. Calculate its value.
✓ Solution
ρ = mass/volume = Amp/[(4/3)πR³] = Amp/[(4/3)πR0³A]
= mp/[(4/3)πR0³] (A cancels!)
= 1.67×10−27/[(4/3)π(1.2×10−15)³]
= 1.67×10−27/7.238×10−45
ρ = mass/volume = Amp/[(4/3)πR³] = Amp/[(4/3)πR0³A]
= mp/[(4/3)πR0³] (A cancels!)
= 1.67×10−27/[(4/3)π(1.2×10−15)³]
= 1.67×10−27/7.238×10−45
ρ = 2.3×1017 kg/m³ (independent of
A!)
3 MarksQ12 (Ex 13.12). The nucleus 23Na
has mass 22.9898 u. Find mass defect and binding energy per nucleon. (mp=1.00783 u,
mn=1.00867 u)
✓ Solution
Z=11, N=12, A=23
Δm = 11×1.00783 + 12×1.00867 − 22.9898
= 11.08613 + 12.10404 − 22.9898 = 23.19017 − 22.9898 = 0.20037 u
BE = 0.20037×931.5 = 186.64 MeV
Z=11, N=12, A=23
Δm = 11×1.00783 + 12×1.00867 − 22.9898
= 11.08613 + 12.10404 − 22.9898 = 23.19017 − 22.9898 = 0.20037 u
BE = 0.20037×931.5 = 186.64 MeV
BE/A = 186.64/23 = 8.11 MeV/nucleon
🌟 Additional / Exemplar Questions (Q13 – Q22)
3 MarksQ13. A sample initially has
2.0×1016 radioactive atoms. After 24 hours, 0.125×1016 remain. Find
half-life.
✓ Solution
N/N0 = 0.125/2.0 = 1/16 = (1/2)4 ⇒ n=4 half-lives
N/N0 = 0.125/2.0 = 1/16 = (1/2)4 ⇒ n=4 half-lives
T1/2 = 24/4 = 6 hours
3 MarksQ14. Compare the radii of 27Al and
125Te nuclei.
✓ Solution
R ∝ A1/3
RAl/RTe = (27/125)1/3 = (27/125)1/3
R ∝ A1/3
RAl/RTe = (27/125)1/3 = (27/125)1/3
= 3/5 = 0.6
Te nucleus has radius 5/3 times that of Al.3 MarksQ15. The decay constant of a radioactive
sample is 0.0693 per day. Find half-life, mean life, and activity if N = 1010.
✓ Solution
T1/2 = 0.693/λ = 0.693/0.0693 = 10 days
τ = 1/λ = 1/0.0693 = 14.43 days (= 1.44×T1/2 ✓)
T1/2 = 0.693/λ = 0.693/0.0693 = 10 days
τ = 1/λ = 1/0.0693 = 14.43 days (= 1.44×T1/2 ✓)
A = λN = 0.0693/(86400)×1010 =
8.02×10−7×1010 = 8020 decays/s ≈ 8.02
kBq
3 MarksQ16. How many α and β particles are
emitted in: 238U → 206Pb?
✓ Solution
ΔA = 238−206 = 32. Number of α = 32/4 = 8
Z changes: U(92)→Pb(82). 8α reduce Z by 16 → Z=92−16=76. Need 82−76=6 β−
ΔA = 238−206 = 32. Number of α = 32/4 = 8
Z changes: U(92)→Pb(82). 8α reduce Z by 16 → Z=92−16=76. Need 82−76=6 β−
8 α-particles and 6 β−-particles
3 MarksQ17. Calculate the energy equivalent of 1
atomic mass unit in MeV.
✓ Solution
1 u = 1.66054×10−27 kg
E = mc² = 1.66054×10−27×(3×108)²
= 1.66054×10−27×9×1016 = 1.4945×10−10 J
1 u = 1.66054×10−27 kg
E = mc² = 1.66054×10−27×(3×108)²
= 1.66054×10−27×9×1016 = 1.4945×10−10 J
= 1.4945×10−10/1.6×10−19 MeV =
931.5 MeV
3 MarksQ18. Activity of a sample decreases from 1200
Bq to 150 Bq in 9 hours. Find half-life.
✓ Solution
A/A0 = 150/1200 = 1/8 = (1/2)³ ⇒ n=3
A/A0 = 150/1200 = 1/8 = (1/2)³ ⇒ n=3
T1/2 = 9/3 = 3 hours
3 MarksQ19. Find the Q-value of the reaction: ²H
+ ³H → ⁴He + n. Masses: ²H=2.014102 u, ³H=3.016049 u, ⁴He=4.002603 u,
n=1.008665 u.
✓ Solution
Δm = (2.014102+3.016049) − (4.002603+1.008665)
= 5.030151 − 5.011268 = 0.018883 u
Δm = (2.014102+3.016049) − (4.002603+1.008665)
= 5.030151 − 5.011268 = 0.018883 u
Q = 0.018883×931.5 = 17.59 MeV
Positive Q → energy is released (exothermic fusion reaction).3 MarksQ20. Mean life of a radioactive sample is 100
s. Find probability that a nucleus will decay in 200 s.
✓ Solution
λ = 1/τ = 1/100 = 0.01 s−1
Probability of survival in time t: P(survive) = e−λt = e−0.01×200 = e−2 = 0.1353
λ = 1/τ = 1/100 = 0.01 s−1
Probability of survival in time t: P(survive) = e−λt = e−0.01×200 = e−2 = 0.1353
Probability of decay = 1 − e−2 = 1 − 0.1353 =
0.8647 ≈ 86.5%
3 MarksQ21. If the mass of a proton is 1.0073 u and
neutron is 1.0087 u, find the BE/A of 4He (mass = 4.0015 u).
✓ Solution
Z=2, N=2
Δm = 2×1.0073 + 2×1.0087 − 4.0015 = 2.0146 + 2.0174 − 4.0015 = 0.0305 u
BE = 0.0305×931.5 = 28.41 MeV
Z=2, N=2
Δm = 2×1.0073 + 2×1.0087 − 4.0015 = 2.0146 + 2.0174 − 4.0015 = 0.0305 u
BE = 0.0305×931.5 = 28.41 MeV
BE/A = 28.41/4 = 7.1 MeV/nucleon
3 MarksQ22. How much energy is released if all atoms
in 1 kg of U-235 undergo fission? (200 MeV per fission)
✓ Solution
Number of atoms = (1000/235)×6.023×1023 = 2.563×1024
Total energy = 2.563×1024×200 MeV = 5.126×1026 MeV
= 5.126×1026×1.6×10−13 J = 8.2×1013 J
Number of atoms = (1000/235)×6.023×1023 = 2.563×1024
Total energy = 2.563×1024×200 MeV = 5.126×1026 MeV
= 5.126×1026×1.6×10−13 J = 8.2×1013 J
E = 8.2×1013 J ≈ 82 TJ (≈ same as
20,000 tonnes of TNT!)
✍ Score Guide — 22 Questions
NCERT Ex 13.1–13.12: 3 marks × 12 = 36 | Additional Q13–Q22: 3 marks × 10 = 30 | Total: 66 marks
NCERT Ex 13.1–13.12: 3 marks × 12 = 36 | Additional Q13–Q22: 3 marks × 10 = 30 | Total: 66 marks
CLASS 12 PHYSICS | FORMULA CAPSULE
Nuclei
Chapter 13 — Complete Formula Sheet for NEET/JEE
📅 Section A — Nuclear Properties
| Quantity | Formula | Key Note |
|---|---|---|
| Radius | R = R0A1/3 | R0=1.2 fm; R ∝ A1/3 |
| Volume | V = (4/3)πR³ ∝ A | V ∝ A (linear) |
| Density | ρ ≈ 2.3×1017 kg/m³ | Constant for ALL nuclei! |
| Isotopes | Same Z, different A | Same element, diff mass |
| Isobars | Same A, different Z | Different elements |
| Isotones | Same N, different Z | Same neutron number |
📅 Section B — Mass Defect & Binding Energy
| Quantity | Formula | Key Note |
|---|---|---|
| Mass defect | Δm = Zmp+(A−Z)mn−M | Always positive |
| Binding energy | BE = Δm×931.5 MeV | 1u = 931.5 MeV/c² |
| BE per nucleon | BE/A | Higher = more stable |
| Most stable | Fe-56: BE/A ≈ 8.75 MeV | Peak of BE/A curve |
| Q-value | Q = (Δmreactants−Δmproducts)c² | +Q = exothermic |
📅 Section C — Radioactive Decay
| Quantity | Formula | Key Note |
|---|---|---|
| Decay law | N = N0e−λt | Exponential decay |
| Activity | A = λN = A0e−λt | Bq or Ci |
| Half-life | T1/2 = 0.693/λ | 50% remains after T1/2 |
| After n half-lives | N = N0/2n | n = t/T1/2 |
| Mean life | τ = 1/λ = 1.44 T1/2 | τ > T1/2 always |
📅 Section D — Decay Rules & α/β Count
| Decay | ΔZ | ΔA | Particle |
|---|---|---|---|
| α-decay | −2 | −4 | 4He |
| β−-decay | +1 | 0 | e− + ν̄ |
| β+-decay | −1 | 0 | e+ + ν |
| γ-decay | 0 | 0 | γ-photon |
| To find α & β count | Formula |
|---|---|
| Number of α | nα = ΔA/4 |
| Number of β− | nβ = Zfinal − (Zinitial − 2nα) |
📅 Section E — Fission & Fusion
| Property | Fission | Fusion |
|---|---|---|
| Process | Heavy → lighter | Light → heavier |
| Energy/reaction | ~200 MeV (U-235) | ~26.7 MeV (4H→He) |
| Energy/nucleon | ~0.85 MeV | ~6.7 MeV (higher!) |
| Condition | Neutron bombardment | ~107 K |
| Example | Nuclear reactor, A-bomb | Sun, H-bomb |
🧠 Memory Tricks
“α = −2, −4 | β = +1, 0”
Alpha: Z drops by 2, A drops by 4. Beta⁻: Z rises by 1, A unchanged. Gamma: nothing changes (just
energy loss). For α/β counting: α from ΔA, then β adjusts Z.
“Half = Halve: 1/2, 1/4, 1/8, 1/16...”
After 1 half-life: 1/2. After 2: 1/4. After 3: 1/8. After n: 1/2n. Quick trick: 3.125% = 1/32
= (1/2)5 = 5 half-lives. 6.25% = (1/2)4 = 4.
“τ = 1.44 × T1/2”
Mean life is always 1.44 times the half-life. Or: T1/2 = 0.693τ. λ =
0.693/T1/2 = 1/τ. These three are interconnected by ln2 = 0.693.
“1u = 931.5 MeV”
Golden conversion! Mass in u × 931.5 = energy in MeV. mp ≈ mn ≈
1u ≈ 931.5 MeV. BE = Δm × 931.5 MeV. Always use this for quick calculations.
“Fe-56 = King of Stability”
Iron-56 has highest BE/A (~8.75 MeV). Left of Fe: fusion releases energy. Right of Fe: fission releases
energy. Both move toward Fe on the BE/A curve!
“Nuclear density = constant!”
ρ = 2.3×1017 kg/m³ for ALL nuclei (A cancels in the formula). A teaspoon of
nuclear matter would weigh ~1012 kg! Nuclear force saturates.
🔢 Critical Values
1u = 931.5 MeV/c²
1u = 1.66×10⁻²⁷ kg
R0 = 1.2 fm
ρ = 2.3×1017 kg/m³
mp = 1.00783 u
mn = 1.00867 u
1 Ci = 3.7×1010 Bq
U-235 fission ≈ 200 MeV
4H→He fusion ≈ 26.7 MeV
❌ Common Mistakes to Avoid
- β⁻ is NOT an orbital electron: In β⁻ decay, the electron comes from INSIDE the nucleus (n→p+e⁻+ν̄), not from the electron cloud.
- γ changes neither Z nor A: γ-decay is just energy release from excited nucleus. No transmutation occurs.
- Half-life ≠ mean life: τ = 1.44×T1/2. Mean life is LONGER than half-life. Don't use them interchangeably.
- Fission energy per reaction > fusion: But fusion energy per nucleon is HIGHER. Per kg of fuel, fusion gives much more energy.
- Nuclear density is constant: Don't say “heavier nuclei are denser”. ALL nuclei have the same density (~2.3×1017 kg/m³).
- BE/A ≠ BE: Fe-56 has highest BE/A but NOT highest total BE. Heavy nuclei have higher total BE but lower BE/A.
📱 Practice MCQs for this topic inside our App
📱 Practice MCQs for this topic inside our App
📱 Practice MCQs for this topic inside our App
📱 Practice MCQs for this topic inside our App
