Introduction to Quantum Mechanics
1. Why Quantum Is Needed — Failures of Classical Physics
By 1900, classical physics explained planetary motion, waves, thermodynamics, but failed at microscopic / high-frequency:
- Blackbody radiation: Rayleigh-Jeans predicted at high (ultraviolet catastrophe) vs observed peak and fall.
- Photoelectric effect: electrons ejected only if (work function), kinetic , independent of intensity — classical wave predicted ∝ intensity and no threshold.
- Compton scattering: X-ray photon scatters with wavelength shift — particle-like momentum.
- Atomic spectra: discrete lines, not continuous; Rutherford atom unstable classically (orbiting electron should radiate and collapse).
- Specific heats at low drop, not constant .
All point to energy quantization.
2. Planck's Breakthrough (1900)
Planck's hypothesis: oscillators in cavity emit/absorb energy in quanta
with J·s. Then average energy not , giving Planck's law:
which fits blackbody spectrum, reduces to Rayleigh-Jeans for and Wien for .
3. Einstein's Steps (1905–1917)
- Photon: light itself is quanta
— explains photoelectric: .
- A & B coefficients (1917) — stimulated emission already covered, quantized fields.
4. Bohr Model Prelude
Bohr quantized angular momentum () for hydrogen to get discrete levels . Useful but ad hoc; true quantum mechanics replaces orbits with wavefunctions.
5. Core Ideas Ahead (preview next topics)
- De Broglie (1924): matter has wavelength .
- Heisenberg: , no simultaneous exact position/momentum.
- Schrödinger equation: wave equation for whose is probability.
6. Exam Points
- List failures of classical physics (blackbody, photoelectric, Compton, atomic spectra) — 5 marks, very frequent (almost certain to ask "why quantum needed").
- State Planck's and Planck's law — 5 marks, frequent.
- Photoelectric equation — 3-5 marks, frequent.
- Distinguish Rayleigh-Jeans vs Planck — 3 marks.