Field Angular Momentum (Thomson Dipole)

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Septim
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Homework Statement


I have attached the question as jpg to this post. Typing these were too time consuming and I uploaded the relevant sections as image files, thanks for your understanding.

Homework Equations



mu_0*epsilon_0*Poynting Vector = Momentum density

Position vector X Momentum density = Angular momentum density

The Attempt at a Solution


These too are attached in png format.

I have found out that angular momentum density has two components, one in the z direction and one in the x direction. According to the books solution the x component integrates to zero but I was unable to verify this and I am highly skeptical about this topic. Any help would be appreciated. I have attached the relevant information to this post.
 
Attachments
  • Handwritten derivation of a radial integral from a Thomson dipole field calculation, with substitutions for u = cos θ and changes of variable, ending in an expression involving ln terms and (1-u^2).
    Attempt_page2.jpg
    13.8 KB · Views: 674
  • Textbook problem 8.12 text: find the total angular momentum in the fields of an electric charge qe and magnetic monopole qm separated by distance d, with E = (1/4πε0)(qe/r^2) r-hat and B = (μ0/4π)(qm/r^2) r-hat.
    Question.png
    13.4 KB · Views: 721
  • Handwritten derivation of the field angular momentum for a Thomson dipole, showing the Coulomb field, Poynting vector, vector identities and an integral over all space.
    Attempt_page1.jpg
    15.5 KB · Views: 600
In constructing your equation (8), note that ##\hat{r}## will generally have a ##\hat{y}## component as well as ##\hat{x}## and ##\hat{z}## components: ##\hat{r} = (\hat{r} \cdot \hat{x}) \hat{x} + (\hat{r} \cdot \hat{y}) \hat{y} + (\hat{r} \cdot \hat{z}) \hat{z}##.

##\hat{r} \cdot \hat{x} = sin\theta cos\phi##, etc.

See what you get for the x and y components of the angular momentum when you integrate over ##\phi##.
 
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