Vector potential with current density

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The discussion focuses on calculating the vector potential \(\vec{A}(\vec{r})\) from a given current density \(\vec{j}\). The user is uncertain about the integration process and whether certain variables should be primed. It is clarified that the calculation can leverage symmetry, particularly since the current density is axially symmetric about the z-axis. The potential \(\vec{A}(z)\) must be perpendicular to the z-axis and rotationally invariant, leading to a unique solution for its direction. Overall, understanding the symmetry simplifies the problem significantly.
Faust90
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Homework Statement


Hey,
I got the current density \vec{j}=\frac{Q}{4\pi R^2}\delta(r-R)\vec{\omega}\times\vec{r} and now I should calculate the vector potential:
\vec{A}(\vec{r})=\frac{1}{4\pi}\int\frac{j(\vec{r})}{|r-r'|}.


Homework Equations


The Attempt at a Solution


here my attempt till now:
http://phymat.de/physics.png
I'm really not sure how to go on now. Is this right what I wrote there?
 
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In the second equation of the notes, should the vector r in the numerator have a prime?

[EDIT: Also, do \theta and \phi refer to the unprimed position or the primed position?]
 
Last edited:
TSny said:
In the second equation of the notes, should the vector r in the numerator have a prime?

[EDIT: Also, do \theta and \phi refer to the unprimed position or the primed position?]

Hi,

thanks for your answer. I think they should all have primes.

Edit: I should only calculate the potential A(r) on the z-axis (for r=z e_z). But I don't know how this can be helpful.
 
Last edited:
Faust90 said:
I should only calculate the potential A(r) on the z-axis (for r=z e_z).

Ahh. If ##\vec{\omega}## is also along the z-axis, then life is looking Wunderbar!
 
TSny said:
Ahh. If ##\vec{\omega}## is also along the z-axis, then life is looking Wunderbar!

Hi, thanks,
Yes Omega is also along the z-Axis, but I don't know how this could help me. Didn't I have to solve the integral first?
 
Faust90 said:
Hi, thanks,
Yes Omega is also along the z-Axis, but I don't know how this could help me. Didn't I have to solve the integral first?

I don't think so. You can get the answer from symmetry considerations. Note that the current ##\vec{j}(r') d^3r'## in a small volume element makes an infinitesitmal contribution to the vector potential at ##r## of amount ##d\vec{A}(r)##, and ##d\vec{A}(r)## has the same direction as ##\vec{j}(r')##.

Do you see that each nonzero value of ##\vec{j}(r') d^3r'## is parallel to the xy plane? So, the total value of ##\vec{A}(r)## must be parallel to the xy plane at any observation point ##r##.

For this problem the observation point is at some z on the z-axis. Note that the current distribution ##\vec{j}(r')## is axially symmetric about the z axis. So ##\vec{A}(z)## would have to point perpendicular to the z-axis and yet be rotationally invariant about the z-axis. There is only one possibility for the value of ##\vec{A}## at z.
 

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