Is E in a Vacuum Considered Free Space?

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The discussion focuses on whether the electric field E in a specified region can be considered free space or vacuum. It clarifies that while vacuum implies the presence of permittivity (ε₀) and permeability (μ₀), free space assumes no charge density (ρ = 0) and no current density (J = 0). The equations provided, including the curl and divergence of E and B, are essential for finding B, ρ, and J. It is noted that in the context of the problem, J may not equal zero, indicating the presence of sources in the vacuum. The conversation emphasizes the distinction between free space and vacuum in electromagnetic theory.
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Given E in a region of space ( \epsilon_{o} , \mu_{o})
I should think of it as a free space or vacuum?
 
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This is vacuum.
 
I have to find B, \rho and J

\nabla \times \vec E= -\frac{\partial \vec B}{\partial t}

\nabla \cdot D=\rho

In free space J = 0 so for J in vacuum I should use

\nabla \times H =J+ \frac{\partial D}{\partial t}

or something else?
 
robert25pl said:
I have to find B, \rho and J

\nabla \times \vec E= -\frac{\partial \vec B}{\partial t}

\nabla \cdot D=\rho

In free space J = 0 so for J in vacuum I should use

\nabla \times H =J+ \frac{\partial D}{\partial t}

or something else?

You probably want to use

D = \epsilon_{o} E

B = \mu_{o} H,

to eliminate D and H. Don't know if you will need it, but you can round out your set of equations with

\nabla \cdot B=0
 
I think I got B, D, H and \rho and using

\nabla \times H =J+ \frac{\partial D}{\partial t}

I get J

What is the difference between free space (J = 0) and vacuum?
 
Vacuum means \mu_{0},\epsilon_{0}.If you're speaking about "free space",then u should assume no charge density \rho=0 and no charge transport \vec{J}=0.

So we can have sources in vacuum.But not in free space.

Free space is typically a vacuum in which electromagetic waves (radiation far away from the sources) propagate.

Daniel.
 
Thanks, So in my problem I will get J not equal 0
 
Please post the text of your problem in its exact form.

Daniel.
 
In the region of space \epsilon_{o} , \mu_{o}
E = (6z\vec{i}+10y\vec{j})cos500t \vec{j}

Find B, \rho, J
 
  • #10
\nabla\cdot\vec{E}=\frac{\rho}{\epsilon_{0}} (1)

\nabla\times\vec{E}=-\frac{\partial\vec{B}}{\partial t} (2)

\nabla\times\vec{B}=\mu_{0}\vec{J}+\mu_{0}\epsilon_{0}\frac{\partial\vec{E}}{\partial t} (3)

Daniel.
 
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