6. Therefore the charge density at a point on the surface of radius r is inversely proportional to r. In other words a small r (a sharply curved surface) has a greater charge density than a surface with large R.
Think of two spheres of different radii
charged to the same potential. If they are joined together by a wire no charge will flow
between them (same potential) but the charge density on each will be different. Now instead
of a wire fit a charged conducting surface (same potential as the spheres) between them to
form the shape shown in the following figure. Again there will be no charge flow and the
charge distribution will therefore be different at different points on the surface.
(Note that
the lines of the electric field will always be at right angles to the
surface).