Calculation the resistance of a spherical shape

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SUMMARY

The discussion focuses on calculating the resistance of nested spherical shells using Ohm's law. The user references the microscopic form of Ohm's law, J = σ_q E, and derives the current I as I = (4πr²)(σ_q E). The potential V is expressed as V = C/r + D, where C and D are constants. The user successfully calculates the resistance R as R = (b-a)/(4πabσ), confirming the solution to their query.

PREREQUISITES
  • Understanding of Ohm's law and its microscopic form
  • Familiarity with electric fields and potential difference
  • Knowledge of spherical coordinates in physics
  • Basic calculus for integration
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  • Study the derivation of electric fields in spherical coordinates
  • Learn about the applications of Ohm's law in different geometries
  • Explore advanced topics in electrostatics, such as Gauss's law
  • Investigate the relationship between resistance and material properties in conductors
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Physics students, electrical engineers, and anyone interested in understanding the principles of resistance in spherical geometries.

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hello there!
I was reading about ohm rule in a MIT physics course and they calculate the resistance of a nested spherical shells like this :

attachment.php?attachmentid=27628&stc=1&d=1282143758.jpg


and they but the microscopic form of ohm's law which is :
[tex]J=\sigma_q E[/tex]
and
[tex]I=A J[/tex]
so
[tex]I=(4 \pi r^2 ) (\sigma_q E)[/tex]
and
[tex]E=-\frac{\partial V}{\partial r}[/tex]
and he said that the potential must be like this form
[tex]V=\frac{C}{r}+D[/tex]
where : C and D are constant .
so my question is what is this form and why he did that and i could calculate the potential easily :
[tex]V_{ab}=\int E . dr[/tex].
thank you
 

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For symmetry, the electric field is directed radially. Since there are no charges inside the conductor, the flux

[tex]\Phi=4\pi r^2 E[/tex]

must be constant. The difference of potential between a and b is

[tex]\Delta V=\int_a^b\frac{\Phi dr}{4\pi r^2}=\frac{\Phi(b-a)}{4\pi ab}[/tex].

But, as you said, [tex]I=\sigma\Phi[/tex], so

[tex]\Delta V=\frac{I(b-a)}{4\pi ab\sigma}\equiv RI[/tex]

and hence

[tex]R=\frac{(b-a)}{4\pi ab\sigma}[/tex]
 
thank you i think it is solved now .
 

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