The correct option is
A c=a+bThe potential at a distance r due to a uniformly charged spherical shell of radius R is given by
V=Q4πϵ0R for r<R and V=Q4πϵ0r for r>R
Here, Q=4πR2σ
A is the interior of all shells.
Thus, the potential at A due to the charges is VA=VA,A+VA,B+VA,C=σϵ0(a−b+c)
C is outside of the all shells.
Thus, the potential at C due to the charges is VC=VC,A+VC,B+VC,C=σϵ0c(a2−b2+c2)
Since no work is done for moving the charge between A and C, VA=VC
Thus, (a−b+c)c=a2−b2+c2⇒(a−b)c=a2−b2⇒c=a+b