Magnetic Flux Q: How Is Flux Independent of Surface?

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SUMMARY

The discussion clarifies that magnetic flux, defined as \Phi = \int \vec B \cdot d\vec a, is independent of the surface used when the divergence of the magnetic field \vec B is zero (\vec \nabla \cdot \vec B = 0). This condition allows the application of Stokes' theorem, confirming that the flux through a loop remains consistent across different surfaces bounded by the same loop. The participants emphasize that while flux is typically defined through a surface, the unique properties of magnetic fields ensure that the flux calculation is unambiguous.

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  • Understanding of magnetic fields and their properties
  • Familiarity with surface integrals in vector calculus
  • Knowledge of Stokes' theorem and its applications
  • Basic concepts of divergence and curl in vector fields
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This question might seem rather naive.
We define the magentic flux through a loop by \Phi = \int \vec B \cdot d\vec a. But an infinite number of different surfaces can be fitted to a given boundary line...so how is the flux independent of the nature of the surface used?
 
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In general, flux isn't defined through a loop (to my knowlegde), it is always defined through a surface. (It's a surface integral). Different surfaces bounding the same loop will in general give different answers.

Exception: If the divergence of the field F is zero everywhere:\vec \nabla \cdot \vec F =0, then we can write \vec F=\vec \nabla \times <br /> \vec A for some field A. Now you can use Stokes' theorem to prove that for a given boundary line, the flux is independent of the surface bounded by that line. Since div B=0 always and everywhere, you can unambigously talk about the magnetic flux through a loop (although I would still never say 'flux through a loop')
 
Thanks for the reply.
So, that means \vec \nabla \cdot \vec B = 0 guarantees that \int \vec B \cdot d\vec a is the same for all surfaces within a given boundary?
 
Yes...
 

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