Electric field inside whole volume of charged conductor is zero.
∵ E = \(-\frac{d V}{d r}\)
E = 0 ⇒ V = constant
(Electric potential is uniform in whole volume)
Inside conductor the work done in bringing any test charge from inside point to surface will be zero.
W = q0(VB – VA)
VB – VA = 0
∴ VA = VB
Potential of both points will be equal.