Schrödinger's Equation and the Hydrogen Atom — Question 1

Section 39-8 · Physics pages 6552–6553

Question 1 The hydrogen quantum-number restrictions determine spatial degeneracy Treat hydrogen with a fixed nucleus, a nonrelativistic Coulomb potential and no spin, fine structure or external field. Write the Bohr length as a. Allowed orbital quantum numbers satisfy n = 1, 2, . . ., ℓ= 0, . . . , n −1 and mℓ= −ℓ, . . . , ℓ. ℓ= 0 1 ℓ= 1 3 ℓ= 2 5 ℓ= 3 7 states in each ℓsector Schematic; labels, not drawing lengths, specify the data. (a) List the allowed ℓvalues for n = 4 and count the spatial states. (b) Assess the proposed triples (3, 3, 0) and (3, 2, 3), and derive the general spatial count at fixed n.
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Question 1 - Solution The hydrogen quantum-number restrictions determine spatial degeneracy ℓ= 0 1 ℓ= 1 3 ℓ= 2 5 ℓ= 3 7 states in each ℓsector (a) Method and calculation n = 4 : ℓ= 0, 1, 2, 3 , g4 = 1 + 3 + 5 + 7 = 16 . ℓ= 0, 1, 2, 3 ⇒2ℓ+ 1 = 1, 3, 5, 7 allowed mℓvalues respectively. (b) Interpretation and further calculation (3, 3, 0) : ℓ̸ ≤n −1; (3, 2, 3) : |mℓ| > ℓ⇒both invalid . gn = n−1 ∑ ℓ=0 (2ℓ+ 1) = n2 . Physical check This counts spatial Coulomb eigenstates only. Spin and the ways corrections split the ideal degeneracy belong to the following chapter.

Question 1

The hydrogen quantum-number restrictions determine spatial degeneracy

Treat hydrogen with a fixed nucleus, a nonrelativistic Coulomb potential and no spin, fine structure or external field. Write the Bohr length as a. Allowed orbital quantum numbers satisfy n=1,2,…n=1,2,\ldots, ℓ=0,…,n−1\ell=0,\ldots,n-1 and mℓ=−ℓ,…,ℓm_\ell=-\ell,\ldots,\ell.

Diagram shown in the original SVG worksheet.

  1. List the allowed ℓ\ell values for n=4n=4 and count the spatial states.

  2. Assess the proposed triples (3,3,0)(3,3,0) and (3,2,3)(3,2,3), and derive the general spatial count at fixed n.

Question 1 - Solution

The hydrogen quantum-number restrictions determine spatial degeneracy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

n=4:ℓ=0,1,2,3,g4=1+3+5+7=16.n=4:\quad\boxed{\ell=0,1,2,3},\qquad g_4=1+3+5+7=\boxed{16}.ℓ=0,1,2,3⇒2ℓ+1=1,3,5,7allowed mℓ values respectively.\ell=0,1,2,3\Rightarrow 2\ell+1=1,3,5,7\quad\text{allowed }m_\ell\text{ values respectively}.

(b) Interpretation and further calculation

(3,3,0):ℓ≰n−1;(3,2,3):|mℓ|>ℓ⇒both invalid.(3,3,0):\ \ell\not\le n-1;\qquad(3,2,3):\ |m_\ell|>\ell\Rightarrow\boxed{\text{both invalid}}.gn=∑ℓ=0n−1(2ℓ+1)=n2.\boxed{g_n=\sum_{\ell=0}^{n-1}(2\ell+1)=n^2}.

Physical check

This counts spatial Coulomb eigenstates only. Spin and the ways corrections split the ideal degeneracy belong to the following chapter.