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Electric Charges And Fields

Question
CBSEENPH12038990

Using Gauss’ laws deduce the expression for the electric field due to a uniformly charged spherical conducting shell of radius R at a point (i) outside and (ii) inside the shell.

Plot a graph showing variation of electric field as a function of r > R and r < R. (r being the distance from the centre of the shell). 

Solution

i) Consider a uniformly charged thin spherical shell of radius R carrying charge Q. To find the electric field outside the shell, we consider a spherical Gaussian surface of radius (r >R), concentric with given shell. If E is electric field outside the shell, then by symmetry electric field strength has same magnitude E0 on the Gaussian surface and is directed radially outward.

So, electric flux through Gaussian surface is given by, 
contour integral subscript s space equals space stack E subscript o with rightwards harpoon with barb upwards on top space. space d S with rightwards harpoon with barb upwards on top space

Therefore, 
contour integral space equals space E subscript o space d s space c o s space 0 space equals space E subscript o.4 pi r squared space 

Charge enclosed by the Gaussian surface is Q.

Therefore, using gauss’s theorem, we have
contour integral subscript s space equals space E with rightwards harpoon with barb upwards on top subscript o space d S space equals space 1 over epsilon subscript o space x space c h a r g e space e n c l o s e d

rightwards double arrow space E subscript o space 4 pi r squared space equals space 1 over epsilon subscript o x space Q

rightwards double arrow space space E subscript o italic space italic equals italic space fraction numerator italic 1 over denominator italic 4 pi epsilon subscript o end fraction Q over r to the power of italic 2 

Thus, electric field outside a charged thin spherical shell is the same as if the whole charge Q is concentrated at the centre.

ii) Electric field inside the shell:
 

The charge resides on the surface of a conductor. Thus, a hollow charged conductor is equivalent to a charged spherical shell. Let’s consider a spherical Gaussian surface of radius (r < R). If E is the electric field inside the shell, then by symmetry electric field strength has the same magnitude Ei on the Gaussian surface and is directed radially outward. 

Electric flux through the Gaussian surface is given by, 
equals space integral subscript S space E with rightwards harpoon with barb upwards on top subscript i. space d S with rightwards harpoon with barb upwards on top
 
integral E subscript i space d S space c o s space 0 space equals space E subscript i space. space 4 pi r squared
Now, Gaussian surface is inside the given charged shell, so charge enclosed by Gaussian surface is zero.

Therefore, using Gauss’s theorem, we have
space space space space space space integral subscript straight S space E with rightwards harpoon with barb upwards on top subscript i. space d S with rightwards harpoon with barb upwards on top space equals space 1 over epsilon subscript o x space c h a r g e space e n c l o s e d

rightwards double arrow space E subscript i.4 pi r squared space equals space 1 over epsilon subscript o space x space 0
rightwards double arrow space E subscript i space equals space 0 space 

Thus, electric field at each point inside a charged thin spherical shell is zero.
 

The graph above shows the variation of electric field as a function of R.