Given: The radii of the two charged conducting spheres are a and b.
The ratio of electric fields of sphere A and B is given as,
E A E B = Q A 4π ε 0 a 2 × 4π ε 0 b 2 Q B
Where, the charge on sphere A is Q A , the charge on sphere B is Q B the electric field of sphere A is E A and the electric field of sphere B is E B .
Further simplify the above equation as,
E A E B = b 2 a 2 × Q A Q B (1)
The ratio of charges is given as,
Q A Q B = C A V C B V
Where, the capacitance of sphere A is C A , the capacitance of sphere B is C B and the potential is V.
Further simplify the above equation as,
Q A Q B = C A C B (2)
Since, C A C B = a b .
By substituting the given value in the equation (2), we get
Q A Q B = a b (3)
By substituting the result of equation (3) in equation (1), we get
E A E B = b 2 a 2 × a b = b a
Thus, the ratio of electric fields at the surface of s is b a and the sharp and pointed end of a conductor can be considered as a sphere of very small radius. The flat portion of the conductor behaves as a sphere of much larger radius so the charge density on the sharp and pointed ends of a conductor is much higher than on the flatter portions of the conductors.