Charge density in a resistor issue

AI Thread Summary
The discussion revolves around calculating the electric field and charge density in a resistor connected to a voltage source. The participant initially believes the electric field at the center of the resistor is zero but is guided to consider the local variation of Ohm's law and Maxwell's equations for a more accurate understanding. They explore the relationship between electric field, current density, and charge density, concluding that the charge density is not zero. The conversation highlights the importance of the continuity equation in maintaining the integrity of the solution. Ultimately, the participant expresses satisfaction with the insights gained from the discussion.
oronanschel
Messages
13
Reaction score
0

Homework Statement



given simple circuit with V the voltage connected to a resistor
with area A, length d and electrical conductance: b*e^-2x/d
after my computations the resistance

R=d*(e^2-1)/(2bA)


Homework Equations



what is the electrical field E in the center of the resistor?

The Attempt at a Solution



i think it must be 0 because i can't think of
why it will be charged
 
Physics news on Phys.org
Hey,
Since you didn't provide any formulae, as to how you'd reached your result, let me ask you this: are you familiar with the relation: \sigma E = j?(Local variation of Ohm's law) Where sigma is the conductance, and j is the current density.
Since the voltage is constant, E must be uniform, simple integration should yield what you're looking for...
I hope that helps somewhat,
Daniel
P.S
Clearly, by following the steps above, you can find that the density won't be zero, per se
The "continuity equation", however, if you recall, is still satisfied(naturally), and generates that equilibrium we all seek...
 
Last edited:
yeah..oops, this is the second question and I managed that one
I know the formula :

\sigma E = j(Local variation of Ohm's law)

the 3rd question was the charge density
in the center of the resistor

that i couldn't figure out..
 
Have you tried Maxwell's equation->\overrightarrow{\nabla} \cdot \overrightarrow{E} = \frac{\rho}{\epsilon_0}
Does that get you any closer?
Daniel
 
becasue E is E(x), can i say that

\overrightarrow{\nabla} \cdot \overrightarrow{E} = \frac{\rho}{\epsilon_0}
is
\frac{dE(x)}{dx} = \frac{\rho(x)}{\epsilon_0}

?
then problem is solved
 
Absolutely! But of course, this could only work by stating that the area(A) is also only dependant on x... so long as that's maintained, you're prefectly correct.
Did you end-up reaching the desired answer?
I hope was I able to provide some aid,
Daniel
 
it doesn't say what is the correct answer but it satisfy me.

so any resistor is also charged (when connected to voltage)? sound weird to me
because out of symmetry why it would be charged positively
and not the opposite?
 
Since the current travels via a relative value known as the "drift velocity", the charges that encounter the most resistance will also tend to accumulate more in the region where that applies(where the resistivity is greater). This is a phenomenon which is typically observed, but in a different case, as "Skin effects":http://en.wikipedia.org/wiki/Skin_effect"
Be sure however to note that the most valuable equation for conserving the physical aspect of this problem, the "continuity equation" is left unchanged:
\overrightarrow{\nabla} \cdot \overrightarrow{j} = -\frac{\partial \rho}{\partial t} which ensures the integrity of the solution.
I pray that shed some light on the issue at hand,
Daniel
 
Last edited by a moderator:
I love physics

thank u very much Daniel
 
Back
Top