The conducting sphere A is connected to the spherical conducting shell B by a thin wire. Since the shells are conductors, the potential on sphere A and shell B will be the same due to the flow of charge between them to maintain the same potential.
When the two spheres are connected by a wire, charge will flow from sphere A to shell B until both spheres reach the same potential. The total charge is redistributed between the two spheres.
The potential on sphere A and shell B is calculated using the formula for the potential of a spherical conductor:
\[
V = \frac{Q}{4 \pi \varepsilon_0 r}
\]
Where:
- \( Q \) is the charge on the conductor,
- \( r \) is the radius of the conductor.
Since both spheres reach the same potential, the charge is distributed in such a way that:
\[
V_A = V_B = \frac{Q_{\text{total}}}{4 \pi \varepsilon_0 (r + R)}
\]
Thus, the final potential on both sphere A and shell B is the same, and it depends on the total charge and the sum of the radii of the two conductors.