Permittivity values in conductors

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ksnf3000
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Hello All,

I am a masters student in electronics engg and reading technical electrodynamics. Please let me know when the electric current density becomes more than the displacement current (for a conductor ) why is the value of ε≈-jσ/ω

Quick replies will be highly appreciated!

Thanks and Regards,

ksnf3000
 
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ksnf3000 said:
Hello All,

I am a masters student in electronics engg and reading technical electrodynamics. Please let me know when the electric current density becomes more than the displacement current (for a conductor ) why is the value of ε≈-jσ/ω

Quick replies will be highly appreciated!

Thanks and Regards,

ksnf3000

High ksnf3000,

electric current density :

[itex]J=σE[/itex]

displacement current density :

[itex]J_{d}=\frac{\partial D}{\partial t}[/itex]

for a steady stead sinusoidal field,

[itex]J_{d}=jωD=jωεE[/itex]

the ratio is [itex]\frac{ωε}{σ}[/itex]

when [itex]ωε=σ[/itex], the magnitudes become the same. Considering typical values of the parameters, this happen at very high frequencies.

I hope that helps.
 
Thanks for your reply Hassan2.

The negative sign indicates the loss the imaginary part suffers, right??
 
ksnf3000 said:
Thanks for your reply Hassan2.

The negative sign indicates the loss the imaginary part suffers, right??

that j is not supposed to be there. The parameters are real, so, the right hand side must be real too. When comparing their magnitudes, j and also -1 becomes 1.