Proving Electric Flux Density: eE Determination

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mym786
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How to prove that D = eE.

Use a general proof. I know how to prove it assuming a point charge.
 
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mym786 said:
How to prove that D = eE.

Use a general proof. I know how to prove it assuming a point charge.
I'm not sure what you mean by "prove". That is simply a definition: D=eE because we say so.
 
How did we get this formula ?
 
mym786 said:
How did we get this formula ?
As I said in my previous post, by definition. There really is nothing to prove. The electric displacement field is simply defined that way.
 
Check out "Introduction to Electrodynamics" by Griffiths 3rd edition, page 175.

[tex]\epsilon_0 \nabla \cdot \vec E =\rho_v + \rho_{f} = \rho_v + \nabla \cdot \vec P[/tex]

[tex]\epsilon_0 \nabla \cdot \vec E + \nabla \cdot \vec P = \rho_{f} \;\Rightarrow \; \nabla \cdot (\epsilon_0 \vec E + \vec P) = \rho_{f}[/tex]

So we define:

[tex]\vec D = \epsilon_0 \vec E + \vec P \;\Rightarrow \; \nabla \cdot \vec D = \rho_{f}[/tex]

For linear and isotropic material:

[tex]\vec P= \epsilon_0 \chi_e \vec E \;\Rightarrow \; \vec D = \epsilon_0(1+ \chi_e) \vec E[/tex]

We define:

[tex]\epsilon_r = 1+ \chi_e \;\hbox { and } \epsilon = \epsilon_0 \epsilon_r \;\Rightarrow \vec D = \epsilon \vec E[/tex]
 
Last edited:
Hi yungman

I think you have a typo; your first line should go

[tex]\epsilon_0 \nabla \cdot \vec E =\rho_v + \rho_{f} = - \nabla \cdot \vec P + \rho_{f}[/tex]
 
dgOnPhys said:
Hi yungman

I think you have a typo; your first line should go

[tex]\epsilon_0 \nabla \cdot \vec E =\rho_v + \rho_{f} = - \nabla \cdot \vec P + \rho_{f}[/tex]

Yes, sorry!