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

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SUMMARY

The electric field inside a cavity within a charged sphere can be determined using Gauss' Law. For a solid sphere with a uniform charge density of +ρ C/m³ and a cavity created by removing a smaller sphere, the electric field inside the cavity is given by the equation E = (ρ/3ε₀) * a, where 'a' is the distance from the center of the larger sphere to the center of the cavity. The solution provided by the user was confirmed as correct, aligning with established principles in electrostatics.

PREREQUISITES
  • Understanding of Gauss' Law
  • Familiarity with electric fields and charge density concepts
  • Knowledge of vector calculus
  • Basic principles of electrostatics
NEXT STEPS
  • Study the application of Gauss' Law in various geometries
  • Explore the superposition principle in electrostatics
  • Learn about electric fields in non-conducting materials
  • Investigate the effects of different charge distributions on electric fields
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Students of physics, particularly those studying electromagnetism, educators teaching electrostatics, and anyone interested in understanding electric fields in charged systems.

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
 
wrong thread :P
 

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