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.
Use a general proof. I know how to prove it assuming a point charge.
The discussion revolves around the proof of the relationship between electric flux density (D) and electric field (E), specifically the equation D = eE. Participants explore the definition of this relationship and the derivation of the formula, with some questioning the need for a proof.
Participants appear divided on whether D = eE requires proof, with some viewing it as a definitional statement and others seeking a derivation. The discussion remains unresolved regarding the necessity of proving the relationship.
There are references to specific mathematical expressions and definitions that may depend on the context of linear and isotropic materials, which could affect the understanding of the relationship between D, E, and polarization.
I'm not sure what you mean by "prove". That is simply a definition: D=eE because we say so.mym786 said:How to prove that D = eE.
Use a general proof. I know how to prove it assuming a point charge.
As I said in my previous post, by definition. There really is nothing to prove. The electric displacement field is simply defined that way.mym786 said:How did we get this formula ?
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]