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 \( \frac{3F}{8} \).
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :