What Is the Electric Field Inside a Cavity Within a Charged Sphere?

AI Thread Summary
The discussion centers on calculating the electric field inside a cavity within a charged sphere using Gauss' Law and the superposition principle. The proposed solution involves determining the electric field from the larger sphere and the negative charge of the removed smaller sphere, resulting in an expression for the electric field inside the cavity. The calculated electric field is given as E = (ρ/3ε₀) * a, which the poster believes is correct but has been deemed wrong by their teacher. A confirmation from another participant suggests that the solution is indeed accurate, indicating potential miscommunication or misunderstanding with the teacher's feedback.
sloane729
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Homework Statement


If I have a solid sphere of radius R and charge density +\rho \, C/m^3 and I then remove a smaller sphere of radius b and is a distance a from the center of the larger sphere, what is the electric field inside the cavity?
I get an answer which I think is right. I've look at the math over and over and can't quite figure out what the teacher did.

Homework Equations


Gauss' Law:
\oint \vec{E} \cdot d\vec{S} = \frac{q_{encl}}{\epsilon_0}



The Attempt at a Solution


I know this is a classic problem using the superposition principle.
First I apply GL to the large sphere at a distance r<R from the center and get an electric field
\vec{E} = \frac{ \rho }{3 \epsilon_0} \vec{r}

Then I do the same except with a charge density of -\rho \, C/m^3 so
\vec{E'} = - \frac{\rho }{3 \epsilon_0} \vec{r'} = -\frac{\rho}{3 \epsilon_0} (\vec{r} - \vec{a})

Now I just sum the two fields
\begin{align}<br /> \vec{E} + \vec{E&#039;} &amp; = \frac{ \rho }{3 \epsilon_0} \vec{r} -\frac{\rho}{3 \epsilon_0} (\vec{r} - \vec{a}) \\ &amp;= \frac{ \rho }{3 \epsilon_0} \vec{r} -\frac{\rho}{3 \epsilon_0} \vec{r} +\frac{\rho}{3 \epsilon_0} \vec{a} \\ &amp;=\frac{\rho}{3 \epsilon_0} \vec{a} \end{align}

This is my solution which is supposedly wrong.
 
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sloane729 said:

Homework Statement


If I have a solid sphere of radius R and charge density +\rho \, C/m^3 and I then remove a smaller sphere of radius b and is a distance a from the center of the larger sphere, what is the electric field inside the cavity?
I get an answer which I think is right. I've look at the math over and over and can't quite figure out what the teacher did.

Homework Equations


Gauss' Law:
\oint \vec{E} \cdot d\vec{S} = \frac{q_{encl}}{\epsilon_0}

The Attempt at a Solution


I know this is a classic problem using the superposition principle.
First I apply GL to the large sphere at a distance r&lt;R from the center and get an electric field
\vec{E} = \frac{ \rho }{3 \epsilon_0} \vec{r}

Then I do the same except with a charge density of -\rho \, C/m^3 so
\vec{E&#039;} = - \frac{\rho }{3 \epsilon_0} \vec{r&#039;} = -\frac{\rho}{3 \epsilon_0} (\vec{r} - \vec{a})

Now I just sum the two fields
\begin{align}<br /> \vec{E} + \vec{E&#039;} &amp; = \frac{ \rho }{3 \epsilon_0} \vec{r} -\frac{\rho}{3 \epsilon_0} (\vec{r} - \vec{a}) \\ &amp;= \frac{ \rho }{3 \epsilon_0} \vec{r} -\frac{\rho}{3 \epsilon_0} \vec{r} +\frac{\rho}{3 \epsilon_0} \vec{a} \\ &amp;=\frac{\rho}{3 \epsilon_0} \vec{a} \end{align}

This is my solution which is supposedly wrong.

Your solution is correct. See, for example http://jkwiens.com/2007/10/24/answe...nonconducting-sphere-with-a-spherical-cavity/
What did your teacher do?

ehild
 
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