Derive an expression for the radial charge distribution of an E field

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Homework Help Overview

The discussion revolves around deriving an expression for the radial charge distribution related to an electric field, specifically focusing on the application of Gauss's law in a radial context.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the cancellation of certain terms in the divergence equation due to the directional nature of the electric field. Questions arise about isolating the charge density, ##\rho(r)##, using the differential form of Gauss's law.

Discussion Status

There is an ongoing exploration of the mathematical expressions involved, with some participants confirming the correctness of terms and suggesting further steps. A potential expression for ##\rho(r)## has been proposed, but no consensus on its validity has been reached.

Contextual Notes

Participants are navigating the implications of the electric field's directionality and the assumptions inherent in applying Gauss's law in this scenario.

Jaccobtw
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Homework Statement
Consider a spherical distribution of charge that creates a uniform, radial electric field described by: ##\vec{E}=E_o\hat{r}##

Use the differential form of Gauss's Law to derive an expression for the radial charge distribution, ##\rho##, that will create this field. You will need the divergence in spherical coordinates: ##\nabla \cdot \vec{V}=\frac{1}{r^2}\frac{\partial}{\partial{r}}(r^2 V_r)+\frac{1}{r\sin[{\theta}]}\frac{\partial}{\partial{\theta}}(\sin[{\theta}]V_{\theta})+\frac{1}{r\sin[{\theta}]}\frac{\partial}{\partial{\phi}}(V_{\phi})##
Enter your mathematical expression for ρ(r) in terms of ##\epsilon_o, E_o ##, and ##r##
Relevant Equations
$$\nabla \cdot \vec{V}=\frac{1}{r^2}\frac{\partial}{\partial{r}}(r^2 V_r)+\frac{1}{r\sin[{\theta}]}\frac{\partial}{\partial{\theta}}(\sin[{\theta}]V_{\theta})+\frac{1}{r\sin[{\theta}]}\frac{\partial}{\partial{\phi}}(V_{\phi}) $$
I know we're supposed to attempt a solution but I'm honestly super confused here. I think the second an third terms of the del equation can be cancelled out because there is only an E field in the r hat direction, so no e field in the theta and phi directions. That leaves us with ##\nabla \cdot \vec{E}=\frac{1}{r^2}\frac{\partial}{\partial{r}}(r^2 E_r)##. The question says to write an expression for ##\rho (r)##. I know gauss' law has the differential form of itself equaling ##\frac{\rho}{\epsilon_o}##. would you isolate ##\rho## to get an expression for ##\rho (r)##? Thanks for your help
 
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Jaccobtw said:
I think the second an third terms of the del equation can be cancelled out because there is only an E field in the r hat direction, so no e field in the theta and phi directions.
Yes.

Jaccobtw said:
That leaves us with ##\nabla \cdot \vec{E}=\frac{1}{r^2}\frac{\partial}{\partial{r}}(r^2 V_r)##.
The symbol ##V_r## on the right side would be better written as ##E_r##.

Jaccobtw said:
The question says to write an expression for ##\rho (r)##. I know gauss' law has the differential form of itself equaling ##\frac{\rho}{\epsilon_o}##. would you isolate ##\rho## to get an expression for ##\rho (r)##?
Yes. See what you get.
 
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TSny said:
Yes.The symbol ##V_r## on the right side would be better written as ##E_r##.Yes. See what you get.
Thank you. I got ##\frac{2 E_o \epsilon_o}{r}##
 
Jaccobtw said:
Thank you. I got ##\frac{2 E_o \epsilon_o}{r}##
Looks good.
 
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