1. Chapter at a Glance
This chapter explores the structure of the atom and its nucleus. It covers Rutherford's alpha-scattering experiment, Bohr's model of hydrogen and its spectral series, the composition and size of nuclei, mass defect and binding energy, radioactive decay, and nuclear fission and fusion. Together with dual nature, it forms "modern physics" — two or three JEE Main questions every year.
- Bohr model: radius, speed and energy of the nth orbit; hydrogen-like ions.
- Wavelengths of spectral lines and the number of possible lines.
- Binding energy per nucleon and Q-values.
- Radioactive decay law, half-life, mean life, and counting α/β decays.
2. Atomic Models
- Rutherford's experiment: most alpha particles passed straight through gold foil, a few were deflected by large angles. So the atom is mostly empty with a tiny, dense, positive nucleus. Distance of closest approach: r₀ = 2kZe²/K for an alpha of kinetic energy K.
- Rutherford's model could not explain the stability of atoms or line spectra.
- Bohr's postulates: electrons move in certain stationary orbits without radiating; angular momentum is quantised, mvr = nh/2π; radiation is emitted when an electron jumps between orbits, hν = Ei − Ef.
3. Bohr's Model of Hydrogen-like Atoms
| Quantity | Formula | Dependence |
|---|---|---|
| Radius | rn = 0.529 n²/Z Å | ∝ n²/Z |
| Speed | vn = 2.18 × 10⁶ Z/n m s⁻¹ | ∝ Z/n |
| Energy | En = −13.6 Z²/n² eV | ∝ Z²/n² |
| KE, PE | K = −E; U = 2E |
- Series: Lyman (n₁ = 1, UV), Balmer (n₁ = 2, visible), Paschen (3), Brackett (4), Pfund (5) — the last three in the infrared.
- Number of lines when electrons fall from level n to the ground state: n(n − 1)/2.
- Ionisation energy of hydrogen = 13.6 eV; of He⁺ = 54.4 eV; of Li²⁺ = 122.4 eV.
4. The Nucleus
- Nucleus AZX has Z protons and A − Z neutrons. Isotopes: same Z; isobars: same A; isotones: same N.
- Radius R = R₀A1/3 (R₀ ≈ 1.2 fm), so nuclear density (~2.3 × 10¹⁷ kg m⁻³) is the same for all nuclei.
- Nuclear force: strongest force, short range (a few fm), charge-independent, saturating.
- Mass defect Δm = [Zmp + (A − Z)mn] − Mnucleus; binding energy = Δm c² (1 u ↔ 931.5 MeV).
- Binding energy per nucleon peaks near A ≈ 56 (Fe, about 8.8 MeV). Heavy nuclei release energy by fission; light nuclei by fusion.
- Fission of U-235 releases about 200 MeV per nucleus. Fusion powers the Sun (hydrogen → helium).
5. Radioactivity
- After n half-lives, fraction left = (1/2)n.
- α decay: A decreases by 4, Z by 2. β⁻ decay: Z increases by 1 (a neutron becomes a proton, emitting an electron and an antineutrino). β⁺ decay: Z decreases by 1. γ decay: no change in A or Z.
- Penetrating power: γ > β > α; ionising power: α > β > γ.
- Activity unit: becquerel (1 decay per second); 1 curie = 3.7 × 10¹⁰ Bq.
6. Formula Master Table
| Quantity | Formula |
|---|---|
| Bohr radius | rn = 0.529 n²/Z Å |
| Energy | En = −13.6 Z²/n² eV |
| Spectral line | 1/λ = RZ²(1/n₁² − 1/n₂²) |
| Number of lines | n(n − 1)/2 |
| Nuclear radius | R = R₀A1/3 |
| Binding energy | BE = Δm × 931.5 MeV |
| Decay law | N = N₀e−λt; T½ = 0.693/λ |
| Mean life | τ = 1/λ = 1.44T½ |
7. Mind Map
- Rutherford scattering
- Bohr postulates
- r, v, E of orbits
- Series, number of lines
- R ∝ A1/3
- Mass defect, BE
- Fission, fusion
- α, β, γ
- Half-life, mean life
8. Tips and Tricks
- Use λ(nm) = 1240/ΔE(eV) for any transition.
- Count decays in a chain: number of α = ΔA/4; then β⁻ = 2 × (number of α) − ΔZ.
- Ratio of radii of two nuclei = (A₁/A₂)1/3.
- The longest-wavelength line of a series comes from the nearest upper level (e.g. Balmer: 3 → 2).
- Forgetting Z² when using hydrogen formulas for He⁺ or Li²⁺.
- Confusing half-life with mean life.
- Thinking a β⁻ electron comes from the atomic shell — it is created in the nucleus.
9. Important One-liners
- Rutherford's experiment revealed the nucleus.
- The Balmer series lies in the visible region.
- Nuclear density is independent of mass number.
- Iron-56 has nearly the highest binding energy per nucleon.
- Half-life does not depend on temperature, pressure or chemical state.
- γ rays are the most penetrating and least ionising radiation.
10. Solved Numericals: Average to Advanced
Five average-level and five advanced-level problems. Click to reveal each answer and its full working. Take hc = 1240 eV nm and 1 u = 931.5 MeV/c².
Average level
Find the energy and wavelength of the photon emitted when a hydrogen electron falls from n = 3 to n = 2.
Show answer & solution
Concept: ΔE = 13.6(1/n₁² − 1/n₂²) eV; λ = 1240/ΔE.
- ΔE = 13.6(1/4 − 1/9) = 13.6 × 5/36 ≈ 1.89 eV.
- λ = 1240/1.89 ≈ 656 nm (red Balmer line, H-alpha).
Answer: about 1.89 eV; about 656 nm
Find the radius of the second Bohr orbit of hydrogen.
Show answer & solution
Concept: rn = 0.529 n² Å for Z = 1.
- r₂ = 0.529 × 4.
- = 2.116 Å.
Answer: 2.116 Å
Hydrogen atoms are excited to n = 5. How many different spectral lines can they emit while returning to the ground state?
Show answer & solution
Concept: number of lines = n(n − 1)/2.
- = 5 × 4/2.
- = 10.
Answer: 10
Find the ratio of the nuclear radii of ²⁷Al and ¹²⁵Te.
Show answer & solution
Concept: R ∝ A1/3.
- R₁/R₂ = (27/125)1/3.
- = 3/5.
Answer: 3 : 5
A radioactive sample has a half-life of 10 days. What fraction remains after 30 days?
Show answer & solution
Concept: fraction = (1/2)n, n = t/T½.
- n = 30/10 = 3.
- Fraction = (1/2)³ = 1/8 = 12.5%.
Answer: 1/8
Advanced level
Find the binding energy and binding energy per nucleon of ⁴He. Atomic masses: ¹H = 1.007825 u, neutron = 1.008665 u, ⁴He = 4.002603 u.
Show answer & solution
Concept: using atomic masses, electron masses cancel: Δm = 2m(¹H) + 2mn − m(⁴He).
- 2 × 1.007825 + 2 × 1.008665 = 4.032980 u.
- Δm = 4.032980 − 4.002603 = 0.030377 u.
- BE = 0.030377 × 931.5 ≈ 28.3 MeV.
- Per nucleon = 28.3/4 ≈ 7.07 MeV.
Answer: about 28.3 MeV; about 7.07 MeV per nucleon
For the sample of N5 (T½ = 10 days), find the decay constant and mean life. If its initial activity is 800 Bq, what is the activity after 20 days?
Show answer & solution
Concept: λ = 0.693/T½; τ = 1/λ; activity also halves every half-life.
- λ = 0.693/10 = 0.0693 day⁻¹.
- τ = 1/0.0693 ≈ 14.4 days.
- 20 days = 2 half-lives ⇒ A = 800/4 = 200 Bq.
Answer: 0.0693 day⁻¹; about 14.4 days; 200 Bq
Each fission of ²³⁵U releases about 200 MeV. Estimate the energy released by the complete fission of 1 g of ²³⁵U.
Show answer & solution
Concept: number of nuclei × energy per fission.
- Number of nuclei = (1/235) × 6.022 × 10²³ ≈ 2.56 × 10²¹.
- Energy = 2.56 × 10²¹ × 200 MeV ≈ 5.13 × 10²³ MeV.
- × 1.6 × 10⁻¹³ J MeV⁻¹ ≈ 8.2 × 10¹⁰ J (about 23 000 kWh).
Answer: about 8.2 × 10¹⁰ J
(a) Find the ionisation energy of He⁺ from its ground state. (b) Find the wavelength of the first Lyman line of hydrogen.
Show answer & solution
Concept: En = −13.6Z²/n² eV.
- (a) He⁺: Z = 2, n = 1 ⇒ E₁ = −54.4 eV, so ionisation energy = 54.4 eV.
- (b) Hydrogen 2 → 1: ΔE = 13.6(1 − 1/4) = 10.2 eV.
- λ = 1240/10.2 ≈ 121.6 nm (ultraviolet).
Answer: 54.4 eV; about 122 nm
²³⁸U (Z = 92) decays through a series of α and β⁻ emissions to stable ²⁰⁶Pb (Z = 82). How many α and β⁻ particles are emitted?
Show answer & solution
Concept: only α changes A (by 4); α lowers Z by 2 and β⁻ raises it by 1.
- Number of α = (238 − 206)/4 = 8.
- After 8 α: Z = 92 − 16 = 76.
- To reach 82, β⁻ = 82 − 76 = 6.
Answer: 8 α and 6 β⁻
11. PYQ-pattern Questions with Solutions
These questions are original and modelled on concepts frequently tested in JEE Main.
Rutherford's alpha-scattering experiment showed that:
- Electrons move in fixed orbits
- The atom has a tiny, dense, positive nucleus
- Energy is quantised
- Neutrons exist
Show solution
Rare large-angle deflections could only come from a small, massive, positive centre.
Answer: (B)
The spectral series of hydrogen lying in the visible region is:
- Lyman
- Balmer
- Paschen
- Pfund
Show solution
Transitions ending at n = 2 give visible lines.
Answer: (B)
What percentage of a radioactive sample remains after four half-lives?
Show solution
(1/2)⁴ = 1/16 = 6.25%.
Answer: 6.25
Nuclear density:
- Increases with A
- Decreases with A
- Is nearly the same for all nuclei
- Depends on Z only
Show solution
Volume ∝ R³ ∝ A and mass ∝ A, so density is constant.
Answer: (C)
Energy is released in nuclear fusion of light nuclei because:
- Mass increases
- Binding energy per nucleon of the product is larger
- Neutrons are absorbed
- Coulomb repulsion increases
Show solution
The product nucleus is more tightly bound; the extra binding energy appears as released energy (mass decreases).
Answer: (B)
In β⁻ decay, by how much does the atomic number change?
Show solution
A neutron turns into a proton: Z increases by 1 (A unchanged).
Answer: 1
12. Quick Revision Summary
- r ∝ n²/Z, v ∝ Z/n, E = −13.6Z²/n² eV.
- Lyman (UV), Balmer (visible), Paschen (IR); lines n(n − 1)/2.
- R = R₀A1/3; BE = Δm × 931.5 MeV; peak near Fe.
- N = N₀e−λt; T½ = 0.693/λ; τ = 1.44T½.
- α: A − 4, Z − 2; β⁻: Z + 1; γ: no change.