Angular Momentum
Angular momentum in quantum mechanics is quantized in units of ℏ. Both orbital angular momentum L and spin S are characterized by quantum numbers ℓ and s, with z-components restricted to integer or half-integer multiples of ℏ.
Key Concepts
- L² eigenvalues: ℓ(ℓ+1)ℏ²; Lz = mℓℏ
- Electron spin: s=1/2, ms = ±1/2
- Spin angular momentum: |S| = √(3/4)ℏ
- Addition of angular momenta: |j₁-j₂| ≤ j ≤ j₁+j₂
- Spin-orbit coupling splits energy levels (fine structure)
Key Equations
Example Problem
An electron has orbital quantum number ℓ=2. Find |L| in units of ℏ.
|L| = √(ℓ(ℓ+1))ℏ = √6 ℏ ≈ 2.449 ℏ.
Exercises
7 problemsUse the angular momentum cone model to find |L| for ℓ = 3 in units of ℏ.
The cone model shows L precessing around the z-axis for ℓ = 3. The vector magnitude |L| = √(ℓ(ℓ+1)) ℏ is shown. Enter |L| in units of ℏ.
For ℓ = 2, count the distinct quantized values of Lz shown in the diagram. How many are there?
The diagram shows all quantized Lz states for a given ℓ. Click each level to count them. For ℓ = 2, how many distinct mℓ values are there?
Find the magnitude of the electron spin angular momentum |S| in units of ℏ.
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Upgrade to Pro →Two electrons have s₁=1/2 and s₂=1/2. What are the possible values of total spin S?
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Upgrade to Pro →An electron in hydrogen has ℓ=1 and mℓ=1. Find Lz in units of ℏ.
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Upgrade to Pro →For j=3/2, find |J| in units of ℏ.
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Upgrade to Pro →Combine ℓ=1 and s=1/2. What are the possible values of j?
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Upgrade to Pro →Key Takeaways
- Angular momentum is quantized: |L| = √(ℓ(ℓ+1))ℏ
- The z-component is restricted to 2ℓ+1 discrete values
- Electron spin is an intrinsic quantum number with no classical analog
- Addition of angular momenta follows the Clebsch-Gordan rules