The charge flows from the sphere at higher potential to the other at lower potential, till their potentials become equal. After sharing, the charges on two spheres would be
`(Q_(1))/(Q_(2)) = (C_(1) V)/(C_(2) V)` where `C_(1), C_(2)` are the capaciteres of two spheres.
But `(C_(1))/(C_(2)) = (a)/(b) :. (Q_(1))/(Q_(2)) = (a)/(b)`
Ratio of surface density of charge on the two spheres: `(sigma_(1))/(sigma_(2)) = (Q_(1))/(4pi a^(2)) . (4pi b^(2))/(Q^(2)) = (Q_(1))/(Q_(2)) . (b^(2))/(a^(2)) = (a)/(b) (b^(2))/(a^(2)) = (b)/(a)`
Hence ratio of electric fields at the surfaces of two spheres
`(E_(1))/(E_(2)) = (sigma_(1))/(sigma_(2)) = (b)/(a)`
A sharp and pointed end can be treated as a sphere of very small radius and a flat portion behaves as a sphere of much larger radius. Therefore, charge density on sharp and pointed ends of conductor is much higher than on its flatter portions.