We will resolve the problem by systematically examining the interactions when sphere C contacts sphere A, followed by sphere B. Both spheres A and B initially possess a charge of \(q\). The initial repulsive force between them is defined as:
\( F = k \frac{q^2}{d^2} \)
where \(k\) represents Coulomb's constant and \(d\) denotes the separation between the sphere centers.
1. Interaction with A: Sphere C begins with no charge. Upon contact with sphere A, charge distribution occurs equally due to their identical nature. Consequently, the charge on each sphere post-contact becomes \( \frac{q + 0}{2} = \frac{q}{2} \).
Sphere A now holds a charge of \( \frac{q}{2} \), and sphere C also carries a charge of \( \frac{q}{2} \).
2. Interaction with B: Sphere C, now charged at \( \frac{q}{2} \), makes contact with sphere B, which has a charge of \( q \). Again, charges will be distributed equally. The combined charge is \( \frac{q}{2} + q = \frac{3q}{2} \).
The charge on each sphere after this contact is \( \frac{\frac{3q}{2}}{2} = \frac{3q}{4} \).
After sphere C is separated, sphere A retains a charge of \( \frac{q}{2} \) and sphere B has a charge of \( \frac{3q}{4} \).
3. Recalculation of Force: The new repulsive force between spheres A and B is calculated as:
\( F' = k \frac{\left( \frac{q}{2} \right) \left( \frac{3q}{4} \right)}{d^2} = k \frac{\frac{3q^2}{8}}{d^2} = \frac{3F}{8} \)
Therefore, the updated repulsive force between spheres A and B is \( \frac{3F}{8} \).