How Does Gauss' Law Explain Charge Induction on a Shell from External Charges?

AI Thread Summary
Gauss' Law explains that external charges do not induce a charge on a conducting shell in a way that affects the electric field inside the shell. The charge distribution on the outer shell is influenced by external charges, while the inner cavity remains unaffected due to the zero electric field within the conducting material. This is demonstrated by considering a Gaussian surface entirely within the conductor, where the electric field is zero, leading to zero net charge enclosed. Consequently, any external electric fields cannot penetrate the shell, effectively decoupling the inner and outer regions. Thus, the conducting shell acts as a barrier, preventing external charges from influencing the electric field inside.
keemosabi
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Homework Statement



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The Attempt at a Solution


I know you use Gauss' Law, but why wouldn't the charges outside of the shell induce a charge on the shell, which would then affect the field at P?
 
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keemosabi said:
... but why wouldn't the charges outside of the shell induce a charge on the shell, which would then affect the field at P?
The charges outside the shell affect the charge distribution on the outer shell only. Likewise, the charge inside the shell affects the charge distribution on the inside surface of the shell only. What you do to the outside charges cannot be communicated to the cavity inside because the field in the conducting material is always zero and that decouples the two regions of space.

You can see this from Gauss's Law. If you draw a Gaussian surface so that it is entirely inside the conducting material, the field on it is zero everywhere which means that the flux through it is zero which means that the net charge is zero always and no matter what happens outside the shell.
 
kuruman said:
The charges outside the shell affect the charge distribution on the outer shell only. Likewise, the charge inside the shell affects the charge distribution on the inside surface of the shell only. What you do to the outside charges cannot be communicated to the cavity inside because the field in the conducting material is always zero and that decouples the two regions of space.

You can see this from Gauss's Law. If you draw a Gaussian surface so that it is entirely inside the conducting material, the field on it is zero everywhere which means that the flux through it is zero which means that the net charge is zero always and no matter what happens outside the shell.
I pretty much understand, I'm just wondering how Gauss' Law proves this. Can't a point outside of a Gaussian Surface still affect the E-field at a point on the surface? It just wouldn't be in included in the integral, right? So how would this say that the charge on the inner shell does not affect the E-field at point P?
 
keemosabi said:
I pretty much understand, I'm just wondering how Gauss' Law proves this. Can't a point outside of a Gaussian Surface still affect the E-field at a point on the surface?
Not if the Gaussian surface is entirely inside the conducting material. The integral is zero because the E-field is zero everywhere on the Gaussian surface regardless of what kind of charge you put outside or inside the shell anywhere you please. This then says that the net charge enclosed by the Gaussian surface (as defined above) is zero no matter what.
 
kuruman said:
Not if the Gaussian surface is entirely inside the conducting material. The integral is zero because the E-field is zero everywhere on the Gaussian surface regardless of what kind of charge you put outside or inside the shell anywhere you please. This then says that the net charge enclosed by the Gaussian surface (as defined above) is zero no matter what.
So it's like the conducting shell prevents the outer charges from affecting the E-field inside of the shell?
 
keemosabi said:
So it's like the conducting shell prevents the outer charges from affecting the E-field inside of the shell?
Yup.
 
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