Atomic Structure

On this page
  1. Direct answer
  2. What you must remember
  3. Common confusion
  4. Exam-focused takeaway
  5. Frequently asked questions
  6. Related topics

Direct answer

Atomic structure rests on two pictures. The Bohr model treats the hydrogen atom as an electron in allowed circular orbits with energies E_n = -13.6 Z^2/n^2 eV and radii r_n = 52.9 n^2/Z pm, explaining the line spectrum through jumps between levels. Quantum mechanics replaces orbits with orbitals described by four quantum numbers, the de Broglie relation lambda = h/(mv) and the Heisenberg principle delta x × delta p >= h/(4 pi), while Aufbau, Pauli and Hund rules fix how orbitals fill.

What you must remember

  • Bohr relations: r_n = 52.9 n^2/Z pm; E_n = -13.6 Z^2/n^2 eV (-2.18 × 10^-18 J); hydrogen levels -13.6, -3.4, -1.51, -0.85 eV; ionisation energy of hydrogen = 13.6 eV.
  • Rydberg formula: wavenumber = R_H Z^2 (1/n1^2 - 1/n2^2), R_H = 109677 cm^-1; Lyman series ends at n1 = 1 (ultraviolet), Balmer at n1 = 2 (visible), higher series infrared; total lines from level n = n(n-1)/2.
  • Quantum numbers: n = 1, 2, 3...; l = 0 to n-1 (s, p, d, f); m_l = -l to +l; m_s = ±1/2. Shell n holds n^2 orbitals and 2n^2 electrons; a subshell holds 2(2l+1).
  • Nodes: radial = n - l - 1, angular = l, total = n - 1.
  • de Broglie lambda = h/p; Heisenberg delta x × delta p >= h/(4 pi); photoelectric: h nu = h nu0 + KE_max.
  • Filling rules: Aufbau by (n + l) then lower n; Pauli limits an orbital to two opposite spins; Hund's rule gives maximum unpaired electrons in degenerate orbitals.
  • Exceptions from exchange energy: Cr = [Ar]3d5 4s1 and Cu = [Ar]3d10 4s1 — half-filled and filled d subshells win.

Common confusion

The recurring error is stretching the Bohr model beyond hydrogen-like species (H, He+, Li2+): it fails for multi-electron atoms, where penetration and shielding split 2s and 2p energies. Students also quote a level's energy as the photon energy — the photon carries the gap between two levels — and miscount spectral lines by forgetting that every pair of levels below n contributes one. Half-filled stability is not a universal law but an exchange-energy effect that matters mainly for d subshells.

Exam-focused takeaway

JEE Main tests rapid-fire facts: allowed quantum numbers, nodes, configuration exceptions, direct Rydberg or Bohr-energy numericals. JEE Advanced prefers synthesis: identifying a transition from a wavelength, scaling to hydrogen-like ions, linking de Broglie wavelength to Bohr quantisation mvr = nh/(2 pi), and photoelectric problems binding KE_max to stopping potential. Sketch the energy ladder with numbers before answering transition questions — most errors are bookkeeping, not concept.

Frequently asked questions

What do the four quantum numbers specify?

n fixes the shell, l the subshell and shape, m_l the orbital orientation, m_s the spin — together they identify an electron uniquely.

Why do Cr and Cu have exceptional configurations?

Half-filled (3d5) and filled (3d10) subshells gain exchange energy and symmetry, outweighing the small cost of promoting a 4s electron.

What is the Heisenberg uncertainty principle?

delta x × delta p >= h/(4 pi): position and momentum of a microscopic particle cannot both be known exactly at once — it kills the idea of a definite orbit.

Which spectral series lies in the visible region?

Only the Balmer series, ending at n = 2; Lyman is ultraviolet, the higher series infrared.

How many spectral lines can an electron falling from level n emit?

Up to n(n-1)/2, one for each pair of levels between n and the ground state.

Where does the Bohr model fail?

For any atom or ion with more than one electron, and for fine structure and the Zeeman effect — cases where electron-electron repulsion and orbital shapes matter.

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