Atomic Structure
Syllabus Unit: Physical Chemistry
Why it matters
Chapter overview
Atomic structure traces the ~50-year dismantling of Dalton's 'indivisible atom' — from Thomson's electron and Rutherford's nucleus to Bohr's quantized orbits and finally the full quantum-mechanical picture of orbitals and quantum numbers. JEE builds every periodic-trend and bonding question on this model, so the postulates, formulas (En, rn) and quantum number rules here are non-negotiable foundations.
1Discovery of Electron, Proton & Neutron
Three experiments across 46 years replaced Dalton's solid, indivisible atom with a structure of charged, weighable parts.
Learning Objectives
- Describe Thomson's cathode ray tube experiment and what it revealed about the electron.
- Describe Millikan's oil drop experiment and its role in fixing the electron's exact charge.
- Describe Goldstein's canal ray experiment that led to the discovery of the proton.
- Describe Chadwick's experiment that discovered the neutron and explain why it was needed.
Key Terms
Between 1886 and 1932, four experiments dismantled Dalton's idea of a solid, indivisible atom, replacing it piece by piece with electron, proton and neutron.
Electron: J.J. Thomson (1897)
- In a cathode ray discharge tube, rays travelling from cathode to anode bent toward a positive plate — proving they carried negative charge.
- Thomson measured e/m = 1.7588 × 10¹¹ C/kg, and found this value identical regardless of the gas or electrode material — the electron is a universal subatomic particle.
Fixing the electron's charge: Millikan (1909)
Millikan's oil drop experiment balanced gravity against an applied electric field on charged oil droplets, finding that charge always appeared as an integer multiple of **1.602 × 10⁻¹⁹ C**. Combined with Thomson's e/m, this gave the electron's mass: 9.1 × 10⁻³¹ kg.
Proton and neutron
- Goldstein's canal rays (1886) — positively charged rays moving opposite to cathode rays; their mass depended on the gas used, and the lightest (from hydrogen) was the proton, mass 1.6726 × 10⁻²⁷ kg.
- Chadwick (1932) bombarded beryllium with alpha particles, producing a neutral, highly penetrating radiation — the neutron, mass close to the proton's, confirming the 'missing' mass in the nucleus.