Magnetic Flux Q: How Is Flux Independent of Surface?

AI Thread Summary
Magnetic flux is defined through a surface integral, expressed as Φ = ∫ B · da, and can vary with different surfaces enclosing the same boundary. However, if the divergence of the magnetic field B is zero everywhere (∇ · B = 0), it allows the use of Stokes' theorem, demonstrating that the flux is independent of the surface chosen. This means that for a given boundary, the magnetic flux remains constant across any surface that fits that boundary. The discussion emphasizes that while flux is typically defined through surfaces, the unique properties of magnetic fields allow for consistent flux measurements through loops. Thus, the independence of magnetic flux from surface nature is guaranteed by the condition of zero divergence.
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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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