Understanding Ohm's Law and Charge Units in Electrodynamics

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SUMMARY

This discussion centers on the application of Ohm's Law and charge units in electrodynamics as outlined in Chapter 7.1 of "Introduction to Electrodynamics" (3rd edition) by David Griffiths. The participants clarify that the unit charge is indeed one coulomb and explore the relationship between current density (\vec J), conductivity (\sigma), electric field (\vec E), and magnetic field (\vec B). They confirm that the transition from the equation \vec J = \sigma(\vec E + \vec v \times \vec B) to \vec f = (\vec E + \vec v \times \vec B) is valid when considering unit charge and slow velocities.

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  • Understanding of vector notation in physics
  • Familiarity with the concepts of electric fields and magnetic fields
  • Knowledge of current density and conductivity
  • Basic grasp of Newton's laws of motion
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This discussion is beneficial for physics students, electrical engineers, and anyone interested in the fundamentals of electrodynamics and the behavior of charged particles in electric and magnetic fields.

yungman
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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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