Bohr's Model of the Atom and Hydrogen Spectrum
Atoms and Nuclei • Class 12 Physics • NCERT • CBSE
Bohr radius: a₀ = 0.529 Å. Energy of nth orbit: Eₙ = −13.6/n² eV. Wave number: 1/λ = RH(1/n₁² − 1/n₂²). Rydberg constant RH = 1.097 × 10⁷ m⁻¹.
Key Formulas
Bohr radius: rₙ = n² × 0.529 ÅEnergy: Eₙ = −13.6/n² eVRydberg: 1/λ = RH(1/n₁² − 1/n₂²)RH = 1.097 × 10⁷ m⁻¹Angular momentum: mvr = nħIonisation energy of H = 13.6 eV
Frequently Asked Questions
- What is the energy required to excite a hydrogen atom from n=1 to n=3?
- E₁ = −13.6 eV; E₃ = −13.6/9 = −1.51 eV. Energy required = E₃ − E₁ = −1.51 − (−13.6) = 12.09 eV. A photon of energy 12.09 eV (λ ≈ 103 nm, UV) is absorbed.
- Why are only certain wavelengths seen in hydrogen spectrum?
- Electrons in hydrogen can only exist in certain quantized energy levels (n=1,2,3…). When an electron transitions between two specific levels, it emits a photon of exactly E = hν = E_high − E_low. Since the energy levels are discrete, only specific photon energies (wavelengths) are emitted, producing a line spectrum rather than a continuous spectrum.
- Why is the Balmer series visible while Lyman series is ultraviolet?
- The Lyman series involves transitions to n=1 (ground state), releasing high energy photons (E > 10 eV) corresponding to UV wavelengths (<400 nm). The Balmer series involves transitions to n=2, releasing lower energy photons (1.9–3.4 eV) with wavelengths in the visible range (400–700 nm). Human eyes can detect the Balmer series wavelengths.
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