flyingpig said:
But inside there clearly is a charge 6nC, which is almost like an insulating sphere with a charge of 6nC
The net charge on the conductor (why do they say net charge and not just charge?) is -4nC
I still don't understand
They say
net charge because each atom of the conductor has a positively charged nucleus surrounded by a cloud of negatively charged electrons. There are lots and lots of atoms making up the conductors, so the total amount of positive charge is huge. So is the total amount of negative charge. For the most part these charges cancel.
The author uses the term
net charge to emphasize this point.
flyingpig said:
Sammy, there is one thing I don't understand very well.
When they say "Qin", where is it enclosed? My book [STRIKE]deducts[/STRIKE] deduces that the E = 0 inside the conductor and hence the Gaussian Surface has enclosed a charge of 0? How do they deduct the fact there is a -6nC and a +6nC?
Yes, Serway makes a rather convincing argument that the electric field within a conducting material is zero (E = 0) under static conditions. Also, he concludes that any excess (net) charge must reside on the surface of a conductor.
Once the fact that E=0 in the conducting material, your author (Serway) uses that fact ( E = 0) for a Gaussian surface which is completely embedded in the conductor to know that the flux through that surface is zero. Therefore, according to Gauss's Law, the
net charge, Q
in enclosed by this surface is zero.
(The reason he says net charge: There likely are billions of billions of coulombs of positive charge (and a similar amount of negative) enclosed within this surface.)
Since there is an isolated sphere with a net charge of 6 nC at the center of the shell, there must be a charge of ‒6 nC on the inner surface of the spherical shell. There's no other place it
can be & it's the only way to get Q
in = 0 .
Is this beginning to make sense? It's important to understand the order in which elements of this argument build on each other.