Chris P. answered 05/15/22
Honors Physics Undergraduate at University of Chicago
Hi Jessie!
a) Let's think about this conceptually. In physics when we talk about "equilibriums," we're typically talking about a state in which forces are balanced and (due to Newton's second law), there is no net acceleration of particles. As the electric field tells us how a test charge would accelerate when placed at a given location, we know the E field must be 0 inside a conductor in electrostatic equilibrium (so that nothing accelerates!). By Gauss' Law,
over an arbitrary "Gaussian surface." But because the E field is 0
everywhere inside the conductor,
any Gaussian surface we integrate over will give us 0 net charge enclosed! For this reason, all excess charge will remain on the surface on the conductor. Rearranging Gauss' Law, we can write Eout - Ein = Q/A/∈0 , but this is just the modulus value σ/∈0 !
2.Let's think about Gauss' Law again.
, where Q is the net charge enclosed. That's right- Gauss' Law doesn't care about anything outside of our Gaussian surface (i.e. external charges). Thus, a conductor "shields" its interior from outside charges (maintains 0 E field inside).
As for the second question, Let's draw a Gaussian surface that encapsulates the exterior of the conductor. By the Law, it again only cares about net charge enclosed. In this way, the E field will effectively disregard the conductor and reflect the total net charge contained within.
Jessie T.
Thank you!, this helps me a lot05/16/22