Per Bohr's quantization rule, an electron's angular momentum in a hydrogen atom is restricted to discrete values. This implies the electron is limited to specific energy levels.
Bohr's postulate states:
\[ L = n \cdot \frac{h}{2\pi} \quad \text{where } n = 1, 2, 3, \dots \] Consequently, the angular momentum is not arbitrary; it is an integer multiple of \( \frac{h}{2\pi} \), not \( h \).
Reasons for excluding other possibilities:
- (A) Quantized as multiples of \( h \): incorrect; the correct form is \( \frac{h}{2\pi} \).
- (B) Continuous: Bohr’s model fundamentally asserts quantization.
- (D) Equal to zero: inaccurate; the ground state exhibits non-zero angular momentum.