Mean Value Theorem of Electrostatics

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Homework Help Overview

The discussion revolves around the Mean Value Theorem of electrostatics as presented in an exercise from "Classical Electrodynamics" by J.D. Jackson. Participants are exploring the correct formulation and derivation of the theorem, particularly in relation to the average potential over a spherical surface.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss various formulations of the average potential, questioning the correctness of expressions and dimensions. There is an exploration of the implications of using different integrals and the definitions of terms like dΦ. Some participants propose alternative formulas for clarity.

Discussion Status

The discussion is active with multiple interpretations being explored. Participants are providing guidance on notation and conceptual understanding, but there is no explicit consensus on a single correct formulation. The original poster is seeking external resources for a derivation.

Contextual Notes

There is mention of homework constraints and the expectation that students engage with the material rather than simply seeking solutions. The age of the thread is noted, indicating a potential lack of engagement from the original poster.

pmb_phy
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In "Classical Electrodynamics - 3rd Ed.," J.D. Jackson has an exercise, 1.10, to derive the mean value theorem of electrostatics. Does anyone know of a derivation which is located on the web?

Pete
 
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Yes, this one

"The average value of the potential over the spherical surface is

[tex]\bar{\Phi} =\frac{1}{4\pi R}\int \Phi \ dA[/tex]

If u imagine the surface of the sphere as discretized, u can rewrite the integral as an infinite sum

[tex]\frac{1}{a}\int \ dA =\Sigma_{area}[/tex]

Then, takin the derivative wrt to R

[tex]\frac{d\bar{\Phi}}{dR}=\frac{d}{dR}\Sigma \Phi=\Sigma \frac{d\Phi}{dR}[/tex]

Convert the infinite sum back to an integral & get

[tex]\frac{d\bar{\Phi}}{dR}=\frac{1}{4\pi R^{2}} \int \frac{d\Phi}{dR} \ dA[/tex]

Now, using that

[tex]\frac{d\Phi}{dR}=-E[/tex] and Gauss's law (no charge inside the sphere) that gives

[tex]\frac{d\bar{Phi}}{dR}=0 \Rightarrow \bar{\Phi}_{surface}=\Phi_{center}[/tex]

Q.E.D.


Daniel.
 
dextercioby said:
"The average value of the potential over the spherical surface is
[tex]\bar{\Phi} =\frac{1}{4\pi R}\int \Phi \ dA[/tex]
No. It isn't. Its
[tex]\bar{\Phi} =\frac{1}{A}\int d\Phi[/tex]
where A is the area of the sphere.

Pete
 
This isn't quite right either.

pmb_phy said:
No. It isn't. Its
[tex]\bar{\Phi} =\frac{1}{A}\int d\Phi[/tex]
where A is the area of the sphere.
Pete

It isn't clear what you mean by [itex]\int d\Phi[/itex]
since usually the integral of an exact differential
is just the function evaluated at the endpoints.

Or alternatively
[tex]\int d\Phi = \int \frac{\partial \Phi}{\partial x} dx +<br /> \int \frac{\partial \Phi}{\partial y} dy +<br /> \int \frac{\partial \Phi}{\partial z} dz[/tex]
which is, of course, a line integral (which isn't what we
want).


dextercobi said:
[tex]\bar{\Phi} =\frac{1}{4\pi R}\int \Phi \ dA[/tex]

This doesn't have the right dimensions. On the left
we have dimensions of [Phi]; and on the right we have
dimensions of [Phi]x[Area]/[Length].

I propose another formula:
[tex] \bar{\Phi} = \frac{1}{4 \pi R^2} \int_A \Phi dA [/tex]

This also has the advantage that if Phi is constant
on the sphere we have
[tex] \bar{\Phi} = \frac{1}{4 \pi R^2} \int_A \Phi dA = <br /> \frac{1}{4 \pi R^2} \Phi \int_A dA = <br /> \frac{1}{4 \pi R^2} \Phi ( 4 \pi R^2 ) =<br /> \Phi[/tex]
 
qbert said:
This isn't quite right either.
It isn't clear what you mean by [itex]\int d\Phi[/itex]
since usually the integral of an exact differential
is just the function evaluated at the endpoints.
That would be true if you were talking about a line integral rather than in this case where the integral is a surface integral. What [itex]d\Phi[/itex] is? Hmmm. Perhaps you're right. I can't say that is a small element of [itex]\Phi[/itex] since that makes no sense to me at the moment. Thanks.

Pete
 
qbert said:
I propose another formula:
[tex] \bar{\Phi} = \frac{1}{4 \pi R^2} \int_A \Phi dA [/tex]
May I propose a more [notationally] precise formula:
[tex] \bar{\Phi} = \frac{1}{A} \int_A \Phi dA [/tex]
or a more [conceptually] precise formula for this average:
[tex] \bar{\Phi} = \frac{ \int_A \Phi dA } {\int_A dA} [/tex]
 
Ah, pedantry, thou most noble virtue. You are, of course, correct. Now the next person (who reads this thread) who needs a 2-D average will know the correct generalization.
 
Last edited:
I admit, it was R^2 in the denominator...

Daniel.
 
qbert said:
Ah, pedantry, thou most noble virtue. You are, of course, correct. Now the next person (who reads this thread) who needs a 2-D average will know the correct generalization.
This is a Homework subforum... and, in my experience, my students appreciate seeing the general idea in a consistent memorable notation rather than a special case. After all, there was some confusion with this formula.

Although the notation "A" [implicitly] suggests an area average, it is certainly not necessarily so.
 
  • #10
robphy said:
This is a Homework subforum... and, in my experience, my students appreciate seeing the general idea in a consistent memorable notation rather than a special case. After all, there was some confusion with this formula.
Although the notation "A" [implicitly] suggests an area average, it is certainly not necessarily so.
Hi Rob

Do you know where I can find a solution? Jackson seems to want the student to use Green's theorem to solve this.

Pete
 
  • #11
Hope this link helps

http://faculty.cua.edu/sober/536/meanvalue.pdf
 
Last edited by a moderator:
  • #12
You do realize that this post is coming onto 4 years old? That the original poster hasn't asked a question for well over a year?

There is usually no reason to resurrect threads that are more than 2 months old, let alone ones that are 4 years old.
 

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