Understanding Maxwell's Equations

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    Maxwell's equations
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Homework Help Overview

The discussion revolves around understanding Maxwell's Equations in the context of free space, specifically examining the conditions under which electric and magnetic fields exist and interact. Participants are analyzing specific equations and configurations to ensure they meet the criteria set by Maxwell's laws.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants are attempting to verify whether given electric and magnetic field configurations satisfy Maxwell's equations. Questions arise about the implications of free space conditions and the definitions of source-free fields.

Discussion Status

The discussion is active, with participants providing insights and questioning each other's interpretations of the equations. Some have offered clarifications regarding the implications of free space, while others are verifying mathematical results related to the fields.

Contextual Notes

There is a noted confusion regarding the definitions of free space and source-free conditions, as well as discrepancies in the mathematical evaluations of the fields. Participants are grappling with the implications of these definitions on the validity of their equations.

robert25pl
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I want to make sure that I understand this good.
Given E and B are possible in a region of free space (J=0) only if [tex]\triangledown \times E=0[/tex] and [tex]\triangledown \cdot B = 0[/tex]
 
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That [itex]\vec{B}[/itex] needs to be stationary (time independent)...Else [itex]\vec{E}[/itex] would not be a purely potential-derived field.

Daniel.
 
I have this two equations:

[tex]E=3\sin(3z-6t) \vec{k}[/tex]
[tex]B=- \frac{1}{15} \sin(3z-6t) \vec{j}[/tex]

So what should I do first?
 
Verify whether such a field configuration satisfies the eqn-s

[tex]\nabla\cdot\vec{B}=0[/tex]

[tex]\nabla\times\vec{E}=-\frac{\partial \vec{B}}{\partial t}[/tex]

Isn't this what u're supposed to do?:confused:

Daniel.
 
robert25pl said:
So what should I do first?

That depends on the question you're supposed to be answering. :confused:
 
"Free space" means [tex]\rho={\color{red}0}[/tex] and [tex]\vec\jmath={\color{red}\vec 0}[/tex].
So, in two of Maxwell's Equations, this means that
[tex]\nabla \cdot \vec E=\rho ={\color{red}\ 0}[/tex] and
[tex]\nabla \times \vec B=\vec \jmath + \frac{\partial \vec E}{\partial t}={\color{red}\ \vec 0} + \frac{\partial \vec E}{\partial t}[/tex].
Of course, [from the other two equations] we must always have
[tex]\nabla \cdot \vec B= 0[/tex] and
[tex]\nabla \times \vec E= -\frac{\partial \vec B}{\partial t}[/tex]

[Insert your own conventional constants]
 
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What?! When we were taught Maxwell's equations in free space, we were told that: [tex]\nabla \cdot \vec E=\frac{\rho}{\epsilon_{0}}[/tex], as free space meant in air not in any sort of medium.
 
Nylex said:
What?! When we were taught Maxwell's equations in free space, we were told that: [tex]\nabla \cdot \vec E=\frac{\rho}{\epsilon_{0}}[/tex], as free space meant in air not in any sort of medium.

So, maybe term I should have used is "source-free".
 
[tex]\nabla\cdot\vec{B}=0[/tex] I verified that

[tex]\nabla\times\vec{E}=\left|\begin{array}{ccc}\vec{i }& \vec{j} &\vec{k}\\\frac{\partial}{\partial x}& \frac{\partial}{\partial y}& \frac{\partial}{\partial z}\\ 0 & 0 & 3\sin (3z-6t) \end{array} \right|[/tex]


[tex]\triangledown \times E[/tex] gave me 0 and [tex]-\frac{\partial \vec{B}}{\partial t} =- \frac{2}{5} \cos(3z-6t) \vec{j}[/tex]

I think this wrong?
 
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  • #10
robert,

You say:

divB = 0, I agree

curlE = 0, I agree

-dB/dt = (-2/5)sin(3z - 6t)j, I think you've got a mistake here
 
  • #12
[tex]\frac{\partial \vec{B}}{\partial t} =-\frac{2}{5} \cos(3z-6t) \vec{j}[/tex]
So [tex]\nabla \times \vec E= -\frac{\partial \vec B}{\partial t}[/tex]
are nor equal and they are not possible in region of space?
 
  • #13
That's that.It is not possible.They should identically solve every equation from Maxwell's system...

Daniel.
 

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