Step 1: Understanding the concept.
The electrostatic potential energy of a system of charges is the sum of the potential energies for all distinct pairs of charges. For two point charges \(q_1\) and \(q_2\) separated by a distance \(r\), the potential energy is
\[
U = \frac{1}{4\pi \varepsilon_0} \frac{q_1 q_2}{r}
\]
Step 2: Apply to the given system.
In an equilateral triangle, all three sides are equal to \(L\).
There are 3 distinct pairs of charges: (1,2), (2,3), and (3,1).
Hence, the total potential energy is the sum of potential energies of these three pairs:
\[
U = 3 \times \frac{1}{4\pi \varepsilon_0} \frac{q^2}{L}
\]
Step 3: Simplify the expression.
\[
U = \frac{3}{4\pi \varepsilon_0} \frac{q^2}{L}
\]
Step 4: Conclusion.
The electrostatic potential energy of three identical charges at the vertices of an equilateral triangle is \(\dfrac{3q^2}{4\pi \varepsilon_0 L}\).
In a coaxial cable, the radius of the inner conductor is 2 mm and that of the outer one is 5 mm. The inner conductor is at a potential of 10 V, while the outer conductor is grounded. The value of the potential at a distance of 3.5 mm from the axis is: 
A sphere of radius \( R \) has a uniform charge density \( \rho \). A sphere of smaller radius \( \frac{R}{2} \) is cut out from the original sphere, as shown in the figure. The center of the cut-out sphere lies at \( z = \frac{R}{2} \). After the smaller sphere has been cut out, the magnitude of the electric field at \( z = -\frac{R}{2} \) is \( \frac{\rho R}{n \epsilon_0} \). The value of the integer \( n \) is: 