Consider two identical metallic spheres of radius R each having charge Q and mass m. Their centers have an initial separation of 4R. Both the spheres are given an initial speed of u towards each other. The minimum value of u, so that they can just touch each other is:
Q. Consider two identical metallic spheres of radius \(R\) each having charge \(Q\) and mass \(m\). Their centers have an initial separation of \(4R\). Both the spheres are given an initial speed of \(u\) towards each other. The minimum value of \(u\), so that they can just touch each other is:

(Take \(k = \frac{1}{4\pi\varepsilon_0}\) and assume \(kQ^2 > Gm^2\) where \(G\) is the Gravitational constant)
A. \( \sqrt{\frac{kQ^2}{4mR}\left(1 + \frac{Gm^2}{kQ^2}\right)} \)
B. \( \sqrt{\frac{kQ^2}{2mR}\left(1 - \frac{Gm^2}{2kQ^2}\right)} \)
C. \( \sqrt{\frac{kQ^2}{2mR}\left(1 - \frac{Gm^2}{kQ^2}\right)} \)
D. \( \sqrt{\frac{kQ^2}{4mR}\left(1 - \frac{Gm^2}{kQ^2}\right)} \)
Correct Answer: \( \sqrt{\frac{kQ^2}{4mR}\left(1 - \frac{Gm^2}{kQ^2}\right)} \)

Explanation (Energy Conservation)

Initial separation = 4R

Final separation when just touching = 2R

Total initial kinetic energy:

\[ K_i = 2 \times \frac{1}{2}mu^2 = mu^2 \]

Electrostatic potential energy:

\[ U_e = \frac{kQ^2}{r} \]

Gravitational potential energy:

\[ U_g = -\frac{Gm^2}{r} \]

Total potential energy:

\[ U = \frac{kQ^2}{r} - \frac{Gm^2}{r} \]

Initial potential energy at r = 4R:

\[ U_i = \frac{kQ^2}{4R} - \frac{Gm^2}{4R} \]

Final potential energy at r = 2R:

\[ U_f = \frac{kQ^2}{2R} - \frac{Gm^2}{2R} \]

Using energy conservation (just touching → final KE = 0):

\[ mu^2 + U_i = U_f \]

\[ mu^2 = U_f - U_i \]

\[ mu^2 = \left(\frac{kQ^2}{2R} - \frac{Gm^2}{2R}\right) - \left(\frac{kQ^2}{4R} - \frac{Gm^2}{4R}\right) \]

\[ mu^2 = \frac{kQ^2}{4R} - \frac{Gm^2}{4R} \]

\[ u^2 = \frac{1}{m}\left(\frac{kQ^2 - Gm^2}{4R}\right) \]

\[ u = \sqrt{\frac{kQ^2}{4mR}\left(1 - \frac{Gm^2}{kQ^2}\right)} \]

Final Answer matches Option D

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