Angular Momenta and Magnetic Dipole Moments — Question 9

Section 40-3 · Physics pages 6628–6629

Question 9 A complete magnetic multiplet cancels its vector moment A model subshell contains one electron in every (ml, ms) state for fixed l, with ml = −l, . . . , l and ms = ±1/2. Use µz = −µB(ml + 2ms). Treat the shell as filled; exclusion will be developed separately. Schematic; labels, not drawing lengths, specify the data. (a) Sum the orbital and spin z moments. (b) For l = 1, calculate ∑ i µ2 zi and explain why it differs from the square of the total z moment.
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Question 9 - Solution A complete magnetic multiplet cancels its vector moment (a) Method and calculation ∑ i µLz,i = −2µB l ∑ m=−l m = 0 . ∑ i µsz,i = −2µB(2l + 1)(1/2 −1/2) = 0 . (b) Interpretation and further calculation l = 1 : µzi/µB = 2, 1, 0, 0, −1, −2 ⇒ ∑ i µ2 zi = 10µ2 B . ( ∑ i µzi)2 = 0 ; 2 ∑ i<j µziµzj = −10µ2 B. Physical check Cancellation concerns the total vector, including cross terms when squared. A sum of individual squared components does not measure the net moment.

Question 9

A complete magnetic multiplet cancels its vector moment

A model subshell contains one electron in every (ml,ms)(m_l,m_s) state for fixed l, with ml=−l,…,lm_l=-l,\ldots,l and ms=±1/2m_s=\pm1/2. Use μz=−μB(ml+2ms)\mu_z=-\mu_B(m_l+2m_s). Treat the shell as filled; exclusion will be developed separately.

Diagram shown in the original SVG worksheet.

  1. Sum the orbital and spin z moments.

  2. For l=1l=1, calculate ∑iμzi2\sum_i\mu_{zi}^2 and explain why it differs from the square of the total z moment.

Question 9 - Solution

A complete magnetic multiplet cancels its vector moment

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∑iμLz,i=−2μB∑m=−llm=0.\sum_i\mu_{Lz,i}=-2\mu_B\sum_{m=-l}^lm=\boxed{0}.∑iμsz,i=−2μB(2l+1)(1/2−1/2)=0.\sum_i\mu_{sz,i}=-2\mu_B(2l+1)(1/2-1/2)=\boxed{0}.

(b) Interpretation and further calculation

l=1:μzi/μB=2,1,0,0,−1,−2⇒∑iμzi2=10μB2.l=1:\quad\mu_{zi}/\mu_B=2,1,0,0,-1,-2\Rightarrow\boxed{\sum_i\mu_{zi}^2=10\mu_B^2}.(∑iμzi)2=0;2∑i<jμziμzj=−10μB2.\boxed{(\sum_i\mu_{zi})^2=0};\quad 2\sum_{i<j}\mu_{zi}\mu_{zj}=-10\mu_B^2.

Physical check

Cancellation concerns the total vector, including cross terms when squared. A sum of individual squared components does not measure the net moment.