Understanding Ohm's Law and Charge Units in Electrodynamics

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The discussion focuses on understanding Ohm's Law and charge units in electrodynamics, specifically referencing equations from Griffiths' "Introduction to Electrodynamics." It clarifies that the unit charge is indeed one coulomb, which is essential for deriving the relationship between current density (J), conductivity (σ), and electric fields (E) in the context of moving charges. The transition from the equation J = σ(E + v x B) to the simplified form f = E for a unit charge is confirmed, emphasizing that if the velocity of the charge is negligible, the magnetic force can be disregarded. Participants express clarity on these concepts, reinforcing the foundational principles of electrodynamics. Overall, the conversation highlights the simplicity of these relationships when understood correctly.
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This is referring to Chapter 7.1, page 285 of "Introduction of Electrodynamics" 3rd edition by David Griffiths.

\vec J = \sigma \vec f \;\; \;\;\;\;\;\;\;( \frac{C}{m^2\cdot sec}) (1)

Where f is force per unit charge. Is the unit charge one coulomb?.

Also

\vec J = \sigma(\vec E +\vec v X \vec B)\;\;\;\;\;\;\;\;\;\;\; (\frac{C}{m^2\cdot sec} ) (2)



My understanding is force:

\vec F = q(\vec E +\vec v X \vec B) \;\;\;\;\;\;\;\;\;\; \hbox {( N) }

For unit charge of one coulomb,

\vec f = (\vec E +\vec v X \vec B) (3)


How do I go from (2) to (3)

Thanks
 
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yup, the unit charge is a coulomb

Equation 1 shows how you get from 2 to 3
 
LostConjugate said:
yup, the unit charge is a coulomb

Equation 1 shows how you get from 2 to 3

Thanks for the reply.

So if \vec f is unit force which is the force of a coulomb charge.

\vec F = Q\vec E = 1\;X \;\vec E = \vec E \hbox { for Q = one coulomb }?

Therefore

\vec J \;=\; \sigma \vec E = \sigma \vec f

if the velocity of the unit charge is slow and

Q (\vec v X \vec B) is ignored.

Am I getting this right? Just that simple? What was I thinking!:cry::eek:

Thanks

Alan
 
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