Let's solve the problem step by step by analyzing the effects of bringing sphere C in contact with sphere A and then sphere B. Initially, the charge on both spheres A and B is \(q\). The force of repulsion between them is given by:
\( F = k \frac{q^2}{d^2} \)
where \(k\) is the Coulomb's constant and \(d\) is the distance between the centers of the spheres.
1. Contacting C with A: Sphere C is initially uncharged. When C is touched to A, the charges will redistribute equally because they are identical spheres. Therefore, the charge on each sphere after contact becomes \( \frac{q + 0}{2} = \frac{q}{2} \).
Now, sphere A has a charge of \( \frac{q}{2} \), and sphere C also has a charge of \( \frac{q}{2} \).
2. Contacting C with B: Sphere C with charge \( \frac{q}{2} \) is now touched to sphere B with charge \( q \). Again, the charges will distribute equally. The total charge is \( \frac{q}{2} + q = \frac{3q}{2} \).
The charge on each sphere after contact is \( \frac{\frac{3q}{2}}{2} = \frac{3q}{4} \).
After C is removed, sphere A has a charge of \( \frac{q}{2} \) and sphere B has a charge of \( \frac{3q}{4} \).
3. New Force Calculation: The new force of repulsion between A and B is:
\( F' = k \frac{\left( \frac{q}{2} \right) \left( \frac{3q}{4} \right)}{d^2} = k \frac{\frac{3q^2}{8}}{d^2} = \frac{3F}{8} \)
Thus, the new force of repulsion between spheres A and B is \( \frac{3F}{8} \).
The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.