How Does Gauss' Law Apply to a Non-Uniformly Charged Hollow Sphere?

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SUMMARY

This discussion focuses on applying Gauss' Law to a hollow spherical shell with a charge density defined as \(\rho=k/r^2\) for the region \(a \leq r \leq b\). The participants analyze the electric field in three distinct regions: \(rb\). The key point of confusion revolves around calculating the enclosed charge \(Q_{\text{enc}}\) using the integral form of Gauss' Law, specifically whether to integrate from \(a\) to \(r\) or \(a\) to \(b\). The resolution clarifies that for the region \(a PREREQUISITES

  • Understanding of Gauss' Law in integral form
  • Familiarity with electric fields and charge density concepts
  • Knowledge of spherical coordinates and volume integrals
  • Basic calculus skills for evaluating integrals
NEXT STEPS
  • Study the derivation and applications of Gauss' Law in electrostatics
  • Learn about charge distributions and their effects on electric fields
  • Explore the concept of Gaussian surfaces and their selection criteria
  • Investigate the implications of non-uniform charge distributions on electric field calculations
USEFUL FOR

Students studying electromagnetism, physics educators, and anyone seeking to deepen their understanding of electric fields generated by non-uniform charge distributions.

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Homework Statement



A hollow spherical shell carries charge density \rho=k/r^2 in the region a\leq r\leq b. Use Gauss' Law in integral form to find the electric field in three regions: (i) r<a, (ii) a<r<b, (iii) r>b.

Homework Equations



Gauss' Law in integral form: \oint_{\text{surface}}\textbf{E}\cdot d\textbf{a}=\frac{1}{\epsilon_0}Q_{\text{enc}}

where Q_{\text{enc}}=\int_{\text{volume}}\rho\;d\tau is the total charge enclosed within the surface.

The Attempt at a Solution



I'm looking at (ii) to start. Due to symmetry we have \textbf{E}=|\textbf{E}|\hat r and so we can pull this out of the left term of the integral in Gauss' law. But I'm confused on how to compute Qenc. I would expect to take the radius part of the integral from a to b, this way:

Q_{\text{enc}}=\int_{\text{volume}}\rho\;d\tau= \int_{\text{surface}}\int_a^b \rho\;dr\;d\textbf{a}

However the solutions manual suggests that I should leave r as a variable and take the integral from a to r, this way:

Q_{\text{enc}}=\int_{\text{volume}}\rho\;d\tau= \int_{\text{surface}}\int_a^r \rho\;d\bar r\;d\textbf{a}

I don't understand this. Why do we get to ignore the field between r and b?

Thanks.
 
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well part ii) is asking for the electric field between a and b. So where will the Gaussian surface extend to?
 
BruceW said:
well part ii) is asking for the electric field between a and b. So where will the Gaussian surface extend to?

OH, I see now!

That was silly.

Thanks.
 
haha, no worries!
 

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