Simplified Maxwell's Equation Proof

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SUMMARY

The discussion focuses on proving the relationship between the change in magnetic field B and the change in electric field E as described by Maxwell's equations, specifically the equation \(\frac{{\partial}B}{{\partial}x}=-\mu_{o}\epsilon_{o}\frac{{\partial}E}{{\partial}t}\). The user successfully derives the equation but struggles with the negative sign. Key steps include integrating around a rectangular loop and using the relationship between electric flux \(\Phi_{E}\) and electric field E. The final derived equation is \(\frac{\partial{E}}{\partial{x}}=\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}\).

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Von Neumann
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Problem:

I'm trying to crudely prove the following:

\frac{{\partial}B}{{\partial}x}=-\mu_{o}\epsilon_{o}\frac{{\partial}E}{{\partial}t}

Solution (so far):

I can get the derivation, but the minus sign eludes me somehow...

Integrating over a thing rectangular loop of length l and width dx, start with the following,

\oint{B{\cdot}dl}=\mu_{o}\epsilon_{o}\frac{\partial{\Phi_{E}}}{\partial{t}}

Then,

\oint{B{\cdot}dl}=(B+dE)l-Bl=dEl

Also,

\Phi_{E}=EA=E(dx)(l)

∴\frac{\partial{\Phi_{E}}}{\partial{t}}=\frac{\partial{E}}{\partial{t}}dxl

Equating the equations above,

dEl=\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}dxl

dE=\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}dx

\frac{\partial{E}}{\partial{x}}=\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}

Any advice is greatly appreciated.
 
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