gracy
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ehild said:NO. Why do you think so?
ehild said:NO. Why do you think so?
Once again, that +2q charge is on the surface of the outer conductor, not in the space between conductors.gracy said:
Ok.I finally understand.Can we proceed?Doc Al said:that +2q charge is on the surface of the outer conductor, not in the space between conductors.
It would be - 2q/4πε0r^2ehild said:What is the electric field at radius r in the region between the shells?
zero.ehild said:Consider a sphere inside the outer pink region. It is conductor, the field is zero. How much is the enclosed charge then?
+2qehild said:This sphere encloses the small shell and the inner surface of the big shell. How much is the charge that compensates the charge of the inner shell?
on the outer surface.ehild said:It can not leave the shell. Where is it?
+2q.Now I understood the complete setup of the problem.ehild said:If there is some charge on the inner surface of the big shell, how much is on the outer surface?

The outer radius of the inner shell is b. The charge distributes on the outer surface of the inner shell. It is "surface charge". How far is the surface of a sphere from the centre of the sphere?gracy said:Wait.
what is the distance of -2q (distributed throughout the outer surface of inner conductor) from the center of inner shell?How can it be b?
The answer is b.ehild said:How far is the surface of a sphere from the centre of the sphere?
It is distributed on the outer surface of the shell. Again: at what distance are the points of the surface of a sphere from the centre of the sphere?gracy said:Because -2q is distributed how it can have only one distance from the center of inner shell?
So all charge on the surface is at b distance from the centre. Are you satisfied?gracy said:The answer is b.
gracy said:I was asking we take the +2q as a whole in spite of the fact that they are distributed.
The whole charge is -2q, and it is distributed evenly on the outer surface of the inner shell.gracy said:I was asking we take the +2q as a whole in spite of the fact that they are distributed.
+2q &-2q cancel each other.gracy said:Charge enclosed is zero.
There is discontinuity of the field at r=c. E is not zero for r<c and E= at r>cgracy said:But at r= c why Electric field s not zero?Charge enclosed is zero.
so how to deal with it?with that formula ;given by blueleaf 7?but I have something to ask about it.ehild said:There is discontinuity of the field at r=c. E is not zero for r<c and E= at r>c
The 2q and -2q cancel each other inside a Gaussian sphere which radius is greater than c. It might by greater only by the size of an atom, but it must be grater.gracy said:+2q &-2q cancel each other.
you mean +2q is at distance which might by greater only by the size of an atom, but it must be grater than cehild said:The 2q and -2q cancel each other inside a Gaussian sphere which radius is greater than c
Blueleaf said that E=0 inside the metal shell, for<r<d. r = c is the boundary between the empty space and the body of the metallic shell. E is defined at both sides of this boundary, but these values are not equal. E is not a continuous function.gracy said:so how to deal with it?with that formula ;given by blueleaf 7?but I have something to ask about it.
NO. That 2q is at distance c from the centre, but the Gaussian surface must be a bit farther inside the shell. Its radius is r>c. It can be greater than c by the size of an atom, but it must be greater.gracy said:you mean +2q is at distance which might by greater only by the size of an atom, but it must be grater than c
why?ehild said:but the Gaussian surface must be a bit farther inside the shell
But in my graph #19 it has been given magnitude of 1/4πε0.-2q c^2ehild said:electric field is not defined at r=c