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Atomic Structure and Bohr Model

Part of the JAMB UTME study roadmap. Physics topic phy-16 of Physics.

Atomic Structure and Bohr Model

🟢 Lite — Quick Review (1h–1d)

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Atomic Structure and Bohr Model — Key Facts Bohr’s postulates: (1) electrons orbit in discrete shells without radiating energy, (2) angular momentum is quantised $L = n\hbar = n\frac{h}{2\pi}$, (3) energy emitted/absorbed when electrons transition Energy levels: $E_n = -\frac{13.6}{n^2}$ eV for hydrogen; for other atoms $E_n = -\frac{13.6Z^2}{n^2}$ eV Rydberg formula: $\frac{1}{\lambda} = R\left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)$ where $R = 1.097 \times 10^7 m^{-1}$ ⚡ Exam tip: Lyman series (UV) → n₁=1; Balmer series (visible) → n₁=2; Paschen series (IR) → n₁=3


🟡 Standard — Regular Study (2d–2mo)

Standard content for students with a few days to months.

Atomic Structure and Bohr Model — JAMB Physics Study Guide Hydrogen spectral series:

  • Lyman series: all transitions ending at n=1; wavelength range 91-121 nm (ultraviolet)
  • Balmer series: ending at n=2; wavelength range 364-656 nm (visible — red Hα, blue-green Hβ, violet Hγ)
  • Paschen series: ending at n=3; wavelength > 820 nm (infrared)
  • Brackett series: ending at n=4; wavelength > 1.45 μm (infrared)

Bohr model limitations: explains only hydrogen-like atoms (He⁺, Li²⁺); cannot explain fine structure, Zeeman effect, Stark effect.

Wave-particle duality: de Broglie wavelength $\lambda = \frac{h}{mv} = \frac{h}{\sqrt{2mE_k}}$; electron diffraction confirmed wave nature.

Ionisation energy: energy to remove electron from ground state: $E = 13.6$ eV for H, $Z^2 \times 13.6$ eV for hydrogen-like atoms.

Common student mistakes: confusing energy levels with energy released; forgetting the negative sign in energy calculations; using wrong principal quantum numbers.


🔴 Extended — Deep Study (3mo+)

Comprehensive coverage for students on a longer study timeline.

Atomic Structure and Bohr Model — Comprehensive Physics Notes

Derivation of Bohr’s quantisation condition: For electron in circular orbit around nucleus with atomic number Z: Centripetal force = electrostatic force: $$\frac{mv^2}{r} = \frac{(Ze)(e)}{4\pi\varepsilon_0 r^2}$$

Also quantisation of angular momentum: $$mvr = n\frac{h}{2\pi}$$

Solving these simultaneously: $$r_n = \frac{\varepsilon_0 h^2 n^2}{\pi me^2 Z} = 0.529 \times 10^{-10} \frac{n^2}{Z} m = a_0 \frac{n^2}{Z}$$

where $a_0 = 0.53$ Å is the Bohr radius.

Energy: $$E_n = \frac{1}{2}mv^2 - \frac{Ze^2}{4\pi\varepsilon_0 r} = -\frac{Ze^2 me^2}{8\varepsilon_0^2 h^2 n^2} = -\frac{13.6 Z^2}{n^2} eV$$

Frequency and wavelength of emitted radiation: When electron transitions from $n_2$ to $n_1$ (where $n_2 > n_1$): $$\Delta E = E_{n_2} - E_{n_1} = h\nu = \frac{hc}{\lambda}$$ $$\frac{1}{\lambda} = \frac{\Delta E}{hc} = R\left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)$$

where Rydberg constant $R = \frac{me^4}{8\varepsilon_0^2 h^3 c} = 1.097 \times 10^7 m^{-1}$.

de Broglie’s contribution: From Bohr quantisation: $mvr = n\frac{h}{2\pi}$, so circumference $= 2\pi r = n\lambda$, which equals $n$ wavelengths — a standing wave condition. This gave de Broglie the idea that matter has wave properties.

X-ray production: Continuous (bremsstrahlung) spectrum: minimum wavelength $\lambda_{min} = \frac{hc}{eV}$ where V is accelerating voltage. Characteristic X-rays: $K_\alpha$ line corresponds to transition from L to K shell.

Radioactivity connection: In nuclear physics, the nucleus contains protons and neutrons. The arrangement of electrons in shells (Bohr model) determines chemical properties, while the nucleus determines radioactive behaviour.

JAMB exam patterns:

  • 2022 JAMB: Calculate wavelength of Hα line in Balmer series
  • 2021 JAMB: Energy released when electron falls from n=3 to n=1 in hydrogen
  • 2020 JAMB: Which spectral series lies in visible region?


📊 JAMB Exam Essentials

DetailValue
Questions180 MCQs (UTME)
Subjects4 subjects (language + 3 for course)
Time2 hours
Marking+1 per correct answer
Score400 max (used for university admission)
RegistrationJanuary – February each year

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