Calculate magnetic potential of a given current density

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Discussion Overview

The discussion revolves around calculating the magnetic vector potential \( A \) for a given current density in the context of magnetostatics, specifically focusing on a cylindrical geometry where the current density is a function of the radial coordinate \( s \).

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about the equation for \( A \) in relation to a cylindrical current density \( J(s) \) and how to express the vector difference \( r - r' \).
  • Another participant clarifies that in magnetostatics, time variables can be ignored and explains that \( A \) is calculated by integrating the contributions from all current elements \( J(r') \) at different positions \( r' \).
  • A participant specifies their current density as \( J(s) = ks \), where \( k \) is a constant and \( s \) is the radius of the cylinder, and presents an expression for \( A \) that they derived.
  • In response, a participant points out potential issues with the derived expression, questioning the direction of \( J \), the inclusion of the position vector \( r \), and the need for integration limits.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correctness of the expression for \( A \) or the assumptions regarding the current density. Multiple viewpoints regarding the formulation and integration process remain present.

Contextual Notes

There are unresolved questions about the direction of the current density \( J \), the proper limits for integration, and the inclusion of the position vector \( r \) in the calculations.

TheBlueDot
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Hello,

I'm current studying magnetostatics and I'm struggling to understand the equation for A. Here is the equation from Griffith in the attachment. My confusion is, if the object is a cylinder and the current density is a function of s, J(s), then how would I write r-r'?

Thank you!
 

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Since it is magnetostatics, everything is static and we can ignore the t and t'. What it says is that A at the point \vec{r} is given by adding up all of the currents \vec{J}(\vec{r'}) at all points \vec{r'} and dividing by the distance between \vec{r} and \vec{r'} Exactly how you write this depends on where the currents are flowing. When you say J(s), what is s? Do you mean a cylinder where current is only flowing on the surface of the cylinder?
 
Hi phyzguy,

Thank you for replying.
For the problem I'm looking at, J(s) = ks, where k is a constant and s is the radius of the cylinder.
With that J(s), I got $$A = \frac {\mu_{o}} {4\pi}\int \frac{a*s(sdsd\phi dz)}{s}\hat{z}$$. Is this correct?
 
TheBlueDot said:
Hi phyzguy, Thank you for replying.
For the problem I'm looking at, J(s) = ks, where k is a constant and s is the radius of the cylinder.
With that J(s), I got $$A = \frac {\mu_{o}} {4\pi}\int \frac{a*s(sdsd\phi dz)}{s}\hat{z}$$. Is this correct?

No, you're still missing a couple of things. First, what is the direction of J? Is it in the z direction as you have indicated, or is it in the φ direction? Second, A is a function of the position vector \vec{r}. You haven't included \vec{r} anywhere. Note you need two position vectors, \vec{r'} which describes the current distribution, and which you have replaced by s, but you also need the second position vector \vec{r} which describes where you are calculating A. Also, you need limits on your integration. Does s run from 0 up to some R? What about the limits on φ and z?
 

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