Simplified Maxwell's Equation Proof

In summary, the conversation is about trying to prove the equation \frac{{\partial}B}{{\partial}x}=-\mu_{o}\epsilon_{o}\frac{{\partial}E}{{\partial}t} and the solution so far involves integrating over a rectangular loop and equating equations to find dE. The conversation also mentions seeking advice and provides a link to the Wikipedia page for the electromagnetic wave equation.
  • #1
Von Neumann
101
4
Problem:

I'm trying to crudely prove the following:

[itex]\frac{{\partial}B}{{\partial}x}[/itex]=-[itex]\mu_{o}[/itex][itex]\epsilon_{o}[/itex][itex]\frac{{\partial}E}{{\partial}t}[/itex]

Solution (so far):

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

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

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

Then,

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

Also,

[itex]\Phi_{E}=EA=E(dx)(l)[/itex]

∴[itex]\frac{\partial{\Phi_{E}}}{\partial{t}}=[/itex][itex]\frac{\partial{E}}{\partial{t}}dxl[/itex]

Equating the equations above,

[itex]dEl=[/itex][itex]\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}dxl[/itex]

[itex]dE=[/itex][itex]\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}dx[/itex]

[itex]\frac{\partial{E}}{\partial{x}}=[/itex][itex]\mu_{o}\epsilon_{o}\frac{\partial{E}}{\partial{t}}[/itex]

Any advice is greatly appreciated.
 
Physics news on Phys.org

1. What are Maxwell's equations?

Maxwell's equations are a set of four fundamental equations that describe the behavior of electric and magnetic fields in space. They were developed by physicist James Clerk Maxwell in the 1860s and are a cornerstone of electromagnetism.

2. What is the proof for simplified Maxwell's equations?

The proof for simplified Maxwell's equations is based on vector calculus and the principle of conservation of charge. It involves breaking down the original equations into their component parts and simplifying them using mathematical operations.

3. Why are simplified Maxwell's equations important?

Simplified Maxwell's equations are important because they provide a more concise and elegant form of the original equations, making it easier to understand and apply them in various fields of science and engineering. They also help to simplify calculations and make predictions about the behavior of electromagnetic fields.

4. How are simplified Maxwell's equations used in real-world applications?

Simplified Maxwell's equations have a wide range of applications, including in the design and analysis of electronic circuits, antennas, and other devices that use electromagnetic fields. They are also used in various fields such as telecommunications, optics, and materials science.

5. Are there any limitations to simplified Maxwell's equations?

While simplified Maxwell's equations are useful in many applications, they do have some limitations. They are only applicable to static or slowly varying electromagnetic fields and do not take into account relativistic effects. In some cases, more complex formulations of Maxwell's equations may be needed to accurately describe the behavior of electromagnetic fields.

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