Why is the Charge Density Calculation Incorrect?

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SUMMARY

The charge density calculation for a static charge distribution producing a radial electric field, defined as E = A e^{-br}/r, is incorrect due to a misinterpretation of the electric field expression. The correct form should be E = A e^{-br}/r^2, leading to the charge density ρ = -ε₀Ab/r² e^{-br} + 4πε₀Aδ(r). The term 4πε₀Aδ(r) arises from applying Gauss's law with a spherical Gaussian surface and considering the limit as radius approaches zero, indicating a point charge at the origin.

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1. Homework Statement [/b]

A static charge distribution produces radial electric field as follows:

\stackrel{\rightarrow}{E}=A\frac{e^{-br}}{r}\stackrel{\rightarrow}{e_{r}}

A,b are constants,please compute the charge density.

Homework Equations



\nabla\cdot \stackrel{\rightarrow}{E}=\frac{\rho}{\epsilon}

The Attempt at a Solution



\nabla\cdot \stackrel{\rightarrow}{E}=\frac{1}{r^{2}}\frac{ \partial}{\partial r}(r^{2}A\frac{e^{-br}}{r})=\frac{1}{r^{2}}\frac{\partial}{\partial r}(Are^{-br})

But the result is wrong.Can you tell me why?
 
Last edited:
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1. Homework Statement [/b]

A static charge distribution produces radial electric field as follows:

\stackrel{\rightarrow}{E}=A\frac{e^{-br}}{r}\stackrel{\rightarrow}{e_{r}}

A,b are constants,please compute the charge density.

Homework Equations



\nabla\cdot \stackrel{\rightarrow}{E}=\frac{\rho}{\epsilon}

The Attempt at a Solution



\nabla\cdot \stackrel{\rightarrow}{E}=\frac{1}{r^{2}}\frac{ \partial}{\partial r}(r^{2}A\frac{e^{-br}}{r})=\frac{1}{r^{2}}\frac{\partial}{\partial r}(Are^{-br})

But the result is wrong.Can you tell me why?
 
Last edited:
What result did you get and what did you expect?
 
The reference answer is

\rho=\epsilon_{0}\nabla\cdot \stackrel{\rightarrow}{E}=-\frac{\epsilon_{0}Ab}{r^{2}}e^{-br}+4\pi\epsilon_{0}A\delta(r)
 
It looks like there's a typo in the expression for the electric field. I think it should be
\mathbf{E} = \frac{Ae^{-br}}{r^2}\mathbf{e}_r
 
But how can I get the term 4\pi\epsilon_{0}A\delta(r) ?
 
Apply the integral form of Gauss's law using a sphere of radius r as the Gaussian surface and take the limit as r goes to 0. From that result, you should be able to deduce a point charge has to reside at the origin.
 

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