Index
Chapter 1 · Item 1.12
Semi-classical quantization rule
Action integrals as early quantum conditions
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Guided reading

The semi-classical quantization rule generalizes the standing-wave idea. Instead of quantizing one circular orbit, it quantizes the action accumulated by each periodic coordinate: \(\oint p_i\,dq_i=n_i h\). The integral measures how much classical phase is accumulated over a closed cycle.

Use this as a method. First identify the periodic motion; then write the conjugate momentum; then integrate over a full cycle; finally solve the condition for the allowed energy, radius or orbit. The rule is not the final quantum theory, but it explains why boundary conditions and action become central.

The rule

The Sommerfeld-Wilson-Ishiwara rule quantizes the action accumulated over one complete cycle of a periodic coordinate. It is the natural generalization of "an integer number of wavelengths must fit" when the momentum is not constant.

\[\oint p_i\,dq_i=n_i h,\qquad n_i=1,2,3,\ldots\]

The index \(i\) allows more than one coordinate to be quantized, which is essential for orbital problems beyond a single circular motion.

Why action?

If momentum is constant, the standing-wave count is simply length divided by wavelength. Using de Broglie's relation gives

\[n=\frac{\text{closed path length}}{\lambda}\]
\[\lambda=\frac{h}{p}\quad \Rightarrow \quad \oint p\,dq=nh\]

When \(p\) changes along the path, the product \(p\,dq\) must be integrated. Action is the classical quantity that naturally measures accumulated phase, so quantizing action is an early way to impose wave self-consistency.

Practical recipe

The rule should be used as a calculation sequence:

  1. Identify the periodic coordinate \(q\).
  2. Write the conjugate momentum \(p(q)\).
  3. Evaluate the closed integral over one cycle.
  4. Set the result equal to \(nh\) and solve for the allowed energies or radii.

This recipe is why the next examples focus on \(p(x)=\sqrt{2m[E-V(x)]}\): the potential determines the momentum along the classical path.

Conceptual discussion

The rule is useful but not final. It gives good intuition for bound periodic systems, yet it misses effects that require full wave mechanics: zero-point shifts, degeneracy structure, spin and operator-based selection rules.

Use SCQR as a bridge: it teaches that allowed energies come from phase closure, but Chapter 2 replaces the orbit by a wave function.
Exercise-ready boundary

This page is designed to support short guided exercises on: Action integrals, allowed orbits and the logic behind early quantization rules.

  • Use from this page: the definitions, physical setup, highlighted equations and conceptual links needed to start a first calculation or explanation.
  • Keep in the book: complete derivations, extended historical discussion, worked solutions and the full textbook narrative remain in the original chapter and linked book resources.
  • Good exercise balance: ask the student to identify assumptions, apply one relation, and interpret the result physically, without requiring material not introduced on this page.
Practice anchors

Use these anchors to design compact exercises. The exercise should be answerable from this page plus standard algebra, while longer derivations, full worked examples and broader context should point back to the original book.

  • Focus: Action integrals, allowed orbits and the logic behind early quantization rules.
  • Conceptual check: state what the main result says physically before using it algebraically.
  • Equation: \[\oint p_i\,dq_i=n_i h,\qquad n_i=1,2,3,\ldots\]
  • Equation: \[n=\frac{\text{closed path length}}{\lambda}\]
  • Equation: \[\lambda=\frac{h}{p}\quad \Rightarrow \quad \oint p\,dq=nh\]
  • Boundary: use this page for setup and first-step reasoning; cite the book for longer derivations, complete experimental history or solved-problem detail.
  • Typical task: derive, interpret, or apply the relation above to a simple case without introducing topics outside this page.
Source note: Original auxiliary summary for this book-app, based on Chapter 1 of Mario Reis, Quantum Mechanics, Elsevier, 2026. Book text and figures are copyright © 2026 Elsevier Inc. No original book figure is reproduced on this page.