Solved: Griffiths Ex. 3.6 - Is There Charge Inside the Sphere?

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SUMMARY

In Griffiths' Example 3.6, it is established that there is no charge inside the hollow sphere, which is inferred from the absence of explicit mention of internal charge. The term "hollow" indicates that the charge is only on the surface, allowing for the application of Laplace's equation under the condition of zero charge density within the sphere. The discussion clarifies that while charges may exist externally, they do not contribute to the net charge inside, which is crucial for solving the problem correctly.

PREREQUISITES
  • Understanding of Griffiths' "Introduction to Electrodynamics"
  • Familiarity with Laplace's equation and its applications
  • Knowledge of electric fields and charge distributions
  • Basic concepts of potential in electrostatics
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  • Review Griffiths Example 3.7 for clarification on charge assumptions
  • Study Laplace's equation and its implications in electrostatics
  • Examine charge distribution in conductive materials
  • Explore the relationship between electric fields and potential in hollow spheres
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Students of electromagnetism, physics educators, and anyone studying electrostatics, particularly those using Griffiths' textbook for reference.

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[SOLVED] Griffiths Example 3.6

Homework Statement


Please stop reading unless you have Griffiths E and M book.

In Example 3.6, we must assume that there is no charge inside the sphere even though it does not explicitly state that? Or is that what "hollow" means?


Homework Equations





The Attempt at a Solution

 
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No hollow simply means in this case the potential is only in tin shell on the surface rather then being throughout which would make A_l obsolete. As long as it not specifically stated that there is net charge or not we assume there isn't. All the charges are positioned homogeneously throughout
 
So you are saying that we do assume there is no charge inside the sphere, correct?

He explicitly says that the charge is on the surface? What does "hollow" add to the problem?
 
No, what happens is that there is no NET charge. There is still charge around, but the overall contribution is such that the charges chancel each other out. look at example 3.8 and see how the electric field causes the charges to accumulated and "charge" even though it is an "uncharged" metal sphere.

Hollow is simply saying that there is a potential within the thing, else there would not be from what i understand.
 
But Laplace's equation does not apply unless there not only no net charge but exactly 0 charge density everywhere inside the sphere. And if Laplace's equation does not apply, neither do the solutions (eqn 3.65) that he uses.
 
Read Section 3.1.1 and look at the example 3.3, 3.4, 3.5. It states that we don't need a charge to have a potential. There is no net charge. LaPlace is equal to 0. The same is true for this section if you look at Eqn 3.53 from which Eqn 3.65 are derived
 
I don't think you understand my question.

In Example 3.7, Griffiths says "assuming there is no charge there". Why does he not say that in Example 3.6? I contend that he made a mistake and that he should have said it in Example 3.6. If that assumption is not made, then everything in Example 3.6 makes no sense.

Please confirm this.
 
He means no free charge OUTSIDE the sphere, else it would influence the result, as the boundary conditions would change. With only the sphere as a source of potential the normal boundary conditions can be used
 
I still think you don't understand my question.

I am asking about the assumptions we are making in Example 3.6. In Example 3.7, Griffiths says explicitly that there is no charge anywhere outside of the sphere. In Example 3.6, he does not say that there is no charge inside the sphere. But that is an assumption that is necessary in order to use the solutions to Laplace's equations.
Someone please confirm this.
 
  • #10
Yes there is no charge inside, cause else he would state it. The problem of the charge inside comes later in a different version, dipole in dielectric
 
  • #11
OK. That's all. Thanks.
 

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