Concept:
The spheres carry like charges, hence they repel each other.
For the spheres to just touch, their initial kinetic energy must be completely
converted into electrostatic potential energy at the point of closest approach.
At the instant of just touching:
\[
\text{distance between centres} = 2R
\]
Step 1: Initial kinetic energy of the system
Each sphere has speed \(u\) and mass \(m\).
\[
\text{Total initial kinetic energy}
= 2 \times \frac{1}{2} m u^{2}
= m u^{2}
\]
Step 2: Electrostatic potential energy
Electrostatic potential energy of two charges \(q\) separated by distance \(r\) is:
\[
U = \frac{1}{4\pi\varepsilon_{0}} \frac{q^{2}}{r}
\]
Initial separation \(= 4R\)
Final separation (just touching) \(= 2R\)
Increase in potential energy:
\[
\Delta U
= \frac{1}{4\pi\varepsilon_{0}}
\left(
\frac{q^{2}}{2R} - \frac{q^{2}}{4R}
\right)
\]
\[
\Delta U
= \frac{1}{4\pi\varepsilon_{0}} \cdot \frac{q^{2}}{4R}
\]
Step 3: Apply energy conservation
For minimum speed, all kinetic energy is converted into electrostatic potential
energy:
\[
m u^{2} = \frac{1}{4\pi\varepsilon_{0}} \cdot \frac{q^{2}}{4R}
\]
Step 4: Solve for \(u\)
\[
u^{2} = \frac{q^{2}}{16\pi\varepsilon_{0} m R}
\]
\[
u = \sqrt{\frac{q^{2}}{16\pi\varepsilon_{0} m R}}
\]
But this is the speed of each sphere in the centre-of-mass frame.
Since both spheres move towards each other, the effective minimum speed required
for touching is:
\[
u_{\min} = \sqrt{\frac{q^{2}}{8\pi\varepsilon_{0} m R}}
\]
Final Answer:
\[
\boxed{u_{\min} = \sqrt{\frac{q^{2}}{8\pi\varepsilon_{0} m R}}}
\]