Electric potential in regions of concentric thin, conducing, spherical shells

In summary, the conversation discusses the concept of potential due to a spherical shell and how it differs from potential due to a point charge. It is stated that according to Gauss' law, a spherical shell does not contribute to the potential inside it. The equations for potential inside and outside the shell are given and it is mentioned that two shells can be treated using the superposition principle. A disagreement is also presented, stating that if you are inside the shell, the potential should be 0, which is argued against.
  • #1
yanyin
21
0
two thin conducting spherical shells as shown below. the inner shell has a radius of r1=15.0cm and a charge of 10.0nC. the outer shell has a radius r2 = 30.0cm and a charge of -15.0nC. find the electric potential V in regions R1, R2, and outside the outer shell, with V = 0 at r = infinite.
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  • #2
What is the expression for Potential due to a Spherical shell

In General

[tex] V=\frac{Q}{4\pi \epsilon_0 R} **&\mbox{for}** r \leq R[/tex]

AND

[tex] V=\frac{Q}{4\pi \epsilon_0 r} **&\mbox{for}** r \geq R[/tex]
 
Last edited:
  • #3
I disagree with the above equations. From Gauss' law, a spherical shell does not contribute at all to the potential inside it--it's easier to think about with gravity: if the Earth were hollow, you could float around in it; you wouldn't be attracted to any point on the shell.

So if you're inside the shell, you don't see it; if you're outside the shell then (again by an application of Gauss' law) it affects you in the same way that a concentric point charge of the same total charge would, i.e., a one over R potential.

That should get you started; you treat two shells with the superposition principle (i.e., add the two potentials together.)

P
 
  • #4
WHY it is not true

so if you're inside the shell, you don't see it
=> 0 which is not true.
 

1. What is the definition of electric potential in regions of concentric thin, conducting, spherical shells?

Electric potential in regions of concentric thin, conducting, spherical shells refers to the measure of electric potential energy per unit charge at any point within the region. It is also known as the potential difference between two points within the region, and is measured in volts (V).

2. How is the electric potential calculated in regions of concentric thin, conducting, spherical shells?

The electric potential in regions of concentric thin, conducting, spherical shells is calculated using the equation V = kQ/r, where V is the electric potential, k is the Coulomb's constant, Q is the charge of the shell, and r is the distance from the center of the shell to the point of interest.

3. What is the relationship between electric potential and electric field in regions of concentric thin, conducting, spherical shells?

The electric potential and electric field in regions of concentric thin, conducting, spherical shells are directly proportional. This means that as the electric potential increases, the electric field also increases, and vice versa. The relationship is given by E = -dV/dr, where E is the electric field and dV/dr is the change in electric potential with distance.

4. How does the electric potential change as you move from one shell to another in regions of concentric thin, conducting, spherical shells?

In regions of concentric thin, conducting, spherical shells, the electric potential remains constant as you move from one shell to another. This is because the electric potential is determined by the charge and distance from the center, which remains the same for all shells within the region.

5. What are some real-world applications of electric potential in regions of concentric thin, conducting, spherical shells?

Electric potential in regions of concentric thin, conducting, spherical shells has various real-world applications. Some examples include the Van de Graaff generator, which uses concentric conducting spheres to create high-voltage electric fields, and lightning rods, which use the same concept to protect buildings from lightning strikes. It is also used in electrostatic painting and electroplating processes.

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