Answer: 3h/2π.
- A h/2π
- B 2h/π
- C 3h/2π
- D 9h/2π
Correct answer: C. 3h/2π
Explanation: L = nh/2π = 3h/2π for n = 3.

The Geiger–Marsden alpha-scattering result: a few alpha particles bounce back at large angles, which rules out Thomson’s diffuse model and demands a tiny, massive, positively charged nucleus. Image: Kurzon, CC BY 3.0, via Wikimedia Commons.
Concept context
Thomson's plum-pudding model, Rutherford's nuclear model from alpha-scattering, Bohr's postulates and hydrogen spectrum, spectral series (Lyman to Pfund), Rydberg formula, and limitations of each model.