How Do You Calculate Electrostatic Potential in a Decaying Electric Field?

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Homework Help Overview

The discussion revolves around calculating the electrostatic potential in a decaying electric field described by the equation E = (E0)*e^(kx) V/m for the region x ≥ 0, with the potential defined as zero at infinity.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between electric fields and potentials, questioning the correctness of integration limits and the presence of minus signs in equations. There is an exploration of deriving electric fields from potentials and verifying calculations.

Discussion Status

Participants are actively engaging with each other's attempts, checking for correctness and clarifying concepts. Some have provided guidance on verifying results through derivation, while others reflect on their integration limits and calculations.

Contextual Notes

There is mention of potential definitions and the relationship between electric fields and potentials, with some participants noting initial errors in integration limits.

Alex_Neof
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Homework Statement



What is the electrostatic potential for the electric field in the region x ≥ 0 where:

E
= (E0)*e^(kxi) V/m, with E0 a constant?

(The potential at x → infinity is defined to be zero).

Homework Equations


b
v = v_a - v_b = - ∫ E . dl
a


The Attempt at a Solution



0
v = - ∫ (E0)*e^(kx) dx = (E0)/k.
infinity

Is this correct?

Kind regards.
 
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Helo Alex,

You can check for yourself if this is correct: how do you derive an electric field from a potential ? Does that work OK for your answer ?

Oh, and did I miss a minus sign somewhere ?
 
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Thank you BvU !
 
Does that mean you found a potential ##E_o\over k## V gives an electric field ## \vec E = E_0 \; e^{kx} \; {\bf \hat\imath} \ ## V/m ?
 
Does that mean you found a potential ##E_o\over k## V gives an electric field ## \vec E = E_0 \; e^{kx} \; {\bf \hat\imath} \ ## V/m ?
 
So I was given the electric field:

##\overrightarrow{E} = {E_0} e^{-kx}\hat i. ##

Which is completely in the x-direction.

Now using:

## V = {V_a} - {V_b} = - \int_a^b \overrightarrow{E}.\overrightarrow{dl}, ##

with the above electric field we have:

## V = - \int_\infty^x {E_0} e^{-kx}dx = \frac{E_0} {k} e^{-kx}.##

Then using what BvU suggested:
BvU said:
Helo Alex,

You can check for yourself if this is correct: how do you derive an electric field from a potential ? Does that work OK for your answer ?

Oh, and did I miss a minus sign somewhere ?

I remembered from my notes that the electric field is related to the potential as follows:

##\overrightarrow{E} = - \nabla V.##

So to test if the potential I found is correct, I just plug it in and find:

##- (\frac{\partial V} {\partial x})=-(-{E_0} e^{-kx}\hat i) ##

Which gives us back our original Electric Field:

##\overrightarrow{E} = {E_0} e^{-kx}\hat i.##

Thanks again BvU, much appreciated!
 
well done !
 
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Initially my limits for integration were wrong, I had them from ##\infty## to 0.
 

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