Atoms and Atomic Structure — NEET Physics Notes
This topic covers the evolution of atomic models, Bohr’s theory of the hydrogen atom, spectral series, and fundamental atomic structure — an important but manageable portion of NEET Physics.
Quick Revision
- Rutherford’s Experiment: Alpha particle scattering → nuclear model of atom
- Bohr’s Postulates: Stationary orbits, angular momentum quantisation, frequency condition
- Hydrogen Spectrum: Lyman, Balmer, Paschen, Brackett, Pfund series
- Rydberg Formula: 1/λ = R(1/n₁² − 1/n₂²), R = 1.097 × 10⁷ m⁻¹
- Energy Levels: En = −13.6/n² eV for hydrogen
- de Broglie Hypothesis: λ = h/p — matter waves
- Atomic Nucleus: protons + neutrons, radius R = R₀A^(1/3)
Standard Study
Rutherford’s Atomic Model
- Gold foil experiment: most alpha particles passed through → atom is mostly empty
- Few particles deflected at large angles → presence of a dense positively charged nucleus
- Limitations: Cannot explain stability of atoms, nor the hydrogen spectrum
Thomson’s Plum Pudding Model
- Positive sphere with electrons embedded like plums in pudding
- Disproved by Rutherford’s experiment
Bohr’s Atomic Model
Postulates:
- Electrons revolve in discrete circular orbits (stationary states) — do not radiate energy
- Angular momentum is quantised: mvr = nh/2π
- Radiation is emitted/absorbed when electrons transition between orbits: E = hν = E₂ − E₁
Successes:
- Explains hydrogen spectrum perfectly
- Explains ionisation energy of hydrogen
- Explains spectral series (Lyman, Balmer, etc.)
Limitations:
- Cannot explain fine spectral lines (Zeeman effect)
- Cannot explain spectral intensity variations
- Fails for multi-electron atoms
Energy Levels and Spectral Series
Hydrogen Spectrum Series:
| Series | Transition (nᵢ → n_f) | Region |
|---|---|---|
| Lyman | nᵢ ≥ 2 → n_f = 1 | UV |
| Balmer | nᵢ ≥ 3 → n_f = 2 | Visible |
| Paschen | nᵢ ≥ 4 → n_f = 3 | IR |
| Brackett | nᵢ ≥ 5 → n_f = 4 | IR |
| Pfund | nᵢ ≥ 6 → n_f = 5 | IR |
Ionisation Energy of Hydrogen: 13.6 eV (ground state) Ionisation Potential: 13.6 V (first ionisation potential)
Hydrogen-like Atoms
- Species with one electron: He⁺, Li²⁺, Be³⁺
- Formula: En = −13.6 Z²/n² eV
- Radius: r = 0.529 n²/Z Å
de Broglie’s Matter Waves
- λ = h/mv = h/√(2mE)
- Applied to electron orbits: for stable orbits, circumference = nλ
- This gives the quantisation condition: mvr = nh/2π
X-rays
- Produced when high-speed electrons strike metal target
- Continuous spectrum (bremsstrahlung) + characteristic spectrum
- Duane-Hunt law: λ_min = hc/eV
- Moseley’s law: ν ∝ (Z − σ)² — frequency increases with atomic number
Deep Study
Velocity and Frequency in Bohr Orbits
- Orbital velocity: vₙ = (ke²Z)/nh = 2.18 × 10⁶ Z/n m/s
- Orbital radius: rₙ = (n²h²)/(4π²mke²Z) = 0.529 n²/Z Å
- Time period: Tₙ = (2πrₙ)/vₙ ∝ n³
- Frequency of revolution: fₙ = 1/Tₙ ∝ 1/n³
Frequency of Emitted Radiation
- ν = (me⁴)/(8ε₀²h³) × (Z²) × (1/n_f² − 1/n_i²)
- Rydberg constant for hydrogen: R = me⁴/(8ε₀²h³c) = 1.097 × 10⁷ m⁻¹
Shortest Wavelength in Hydrogen Spectrum
- Maximum energy transition: n = ∞ to n = 1
- λ_min = 1/R = 912 Å (Lyman series limit)
Atomic Radius and Nucleus Size
- Atomic radius: ~10⁻¹⁰ m (angstrom)
- Nuclear radius: ~10⁻¹⁵ m (femtometer)
- Nuclear radius formula: R = R₀A^(1/3), where R₀ ≈ 1.2 × 10⁻¹⁵ m
Bohr’s Correspondence Principle
- Quantum mechanics gives same results as classical physics for large quantum numbers (n → ∞)
Exam Tips
- Bohr model applies ONLY to hydrogen and hydrogen-like atoms (one electron)
- Ionisation energy: 13.6 eV for H, 54.4 eV for He⁺ (13.6 × 2²)
- Lyman series is in UV region — Balmer series has some lines in visible range
- For H-like atoms: energy depends on Z² and 1/n²
- de Broglie wavelength for electron in nth orbit: λ = (2πrₙ)/n
- Rutherford scattering: most particles go through, few deflect — nucleus is small and dense
- Remember: 1 Å = 10⁻¹⁰ m, 1 fm = 10⁻¹⁵ m
Common Pitfalls
- Applying Bohr model to multi-electron atoms (it doesn’t work)
- Confusing spectral series and their wavelength ranges
- Forgetting to square Z when calculating energy for hydrogen-like ions
- Confusing frequency ν with wave number (1/λ)
- Not knowing that the Balmer series is the one visible in the visible spectrum
Suggested Study Order
- Thomson and Rutherford models — experimental evidence
- Bohr’s postulates and derivation
- Energy levels and spectral series
- Hydrogen-like atoms (extension of Bohr model)
- de Broglie hypothesis and matter waves
- X-rays and Moseley’s law
- Nuclear size and structure