Difficulty: Easy
Correct Answer: True
Explanation:
Introduction / Context:
Atomic states are labeled by quantum numbers. Among them, the magnetic quantum number (commonly m_l for orbital angular momentum) is directly connected to the projection of angular momentum along a chosen axis, usually the z-axis. Understanding this mapping is fundamental for topics like Zeeman splitting and selection rules in spectroscopy.
Given Data / Assumptions:
Concept / Approach:
The magnetic quantum number m_l takes integer values from −l to +l. It specifies the eigenvalue of the angular momentum operator's z-component. The total magnitude of orbital angular momentum depends only on l, while the component along the quantization axis depends on m_l. This distinction explains spectral line splitting under magnetic fields (Zeeman effect), where different m_l states shift differently.
Step-by-Step Solution:
Angular momentum magnitude L depends on l via L = sqrt(l(l+1)) * ħ (conceptual relation).The quantized component along z is L_z = m_l * ħ.Therefore, m_l determines the specific allowed component of angular momentum along the chosen axis and explains directional properties of atomic orbitals in fields.
Verification / Alternative check:
Experimental Zeeman splitting patterns confirm that energy shifts are proportional to m_l (and g-factors), matching the interpretation that m_l labels the axial component.
Why Other Options Are Wrong:
“False” ignores core quantum principles. “True only for spin” is incorrect; both orbital (m_l) and spin (m_s) have axial projections. Statements claiming it sets only the magnitude or only the energy misunderstand the roles of l and m_l.
Common Pitfalls:
Final Answer:
True
Discussion & Comments