How Do Magnetic Fields Relate to Current Density in Physics?

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    Maxwell's equations
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Discussion Overview

The discussion revolves around the relationship between magnetic fields and current density, specifically examining the implications of the curl of the magnetic field in the context of a long straight wire carrying current. Participants explore theoretical aspects and clarify concepts related to magnetic fields and their mathematical representation.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the curl of the magnetic field is proportional to the current density at a point, as expressed in the equation ∇XB(x) = μ0j(x).
  • One participant points out that outside a long straight wire, the current density is zero, which raises questions about the implications for the curl of the magnetic field.
  • Another participant argues that while the curl of the magnetic field is constant around the wire, it does not vanish outside the wire, suggesting a misunderstanding of the relationship between curl and current density.
  • Some participants clarify that the curl is a differential operator acting on vector fields, not a second derivative, addressing a misconception about terminology.
  • One participant acknowledges a misunderstanding regarding the relationship between the magnetic field and current density, noting that it is the curl of the magnetic field that is proportional to current density, not the magnetic field itself.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of the curl of the magnetic field outside the wire and its relationship to current density. The discussion remains unresolved, with multiple competing interpretations present.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the behavior of magnetic fields and current density in different regions, particularly outside the wire. The distinction between curl and other mathematical operations is also a point of confusion.

ObsessiveMathsFreak
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the final equation

∇XB(x) = μ0j(x)


But this means that the curl of the magnetic field at any point is proportional to the current density at that point.

But take the case of a long straight wire carrying current.

The magnetic field surrounding the wire is circular and hence its curl is everywhere constant in value.

But that means that the current density is everywhere constant in value, even at a million miles away from the wire.

what's with that?
 
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yeah, a million miles from the wire the current density is constant, it's zero. Anywhere outside the wire, the current density is zero.

JMD
 
Originally posted by ObsessiveMathsFreak
the final equation

∇XB(x) = μ0j(x)


But this means that the curl of the magnetic field at any point is proportional to the current density at that point.

But take the case of a long straight wire carrying current.

The magnetic field surrounding the wire is circular and hence its curl is everywhere constant in value.

Outside the wire the curl vanishes since outside the wire j(x) = 0.

Pete
 
But the curl doesn't vanish. outside the wire the magnetic field is circular, meaning it has a constant curl.
 
Curl is zero where there is no current, pmb is correct. Curl and integral over extended loop are different quantities. Whan you integrate over loop you have to include sources (currents) if the loop includes them.
 
Try computing the curl of a circular field somewhere other than the axis.
 


But this means that the curl of the magnetic field at any point is proportional to the current density at that point.

I think I see the problem now. The magnetic field is *not* proportional to current density - the *curl* of the magnetic field is. Sorry I din't note that earlier.

Pmb
 
Man, you guys call the second derivative "curl"?

blegch
 
Originally posted by KillaMarcilla
Man, you guys call the second derivative "curl"?

blegch

No, the curl is the differential operator:

[nab]×

which acts on vector fields. It is not the second derivative.
 
  • #10
Oh, right, I think I know what you're talking about now

Sorry, I had Math 126 about two years ago, and haven't used most of it since then (except for the geometric series approximations)

h0 h0, I look like quite the f00l now
 

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