To resolve the issue, Gauss's law will be applied. This law asserts that the electric flux \( \Phi \) passing through a closed surface is equivalent to the enclosed charge divided by the permittivity of free space \( \epsilon_0 \):
\(\Phi = \frac{Q_{\text{enc}}}{\epsilon_0}\)
Given a linear charge density \( \lambda \) of \( 2 \, \text{nC/m} \) or \( 2 \times 10^{-9} \, \text{C/m} \), and a wire traversing diagonally opposite corners of a cube with a side length of \( \sqrt{3} \, \text{cm} \), the total charge enclosed by the cube can be determined. The length of the cube's diagonal, through which the wire passes, is \( \sqrt{3} \, \text{cm} \), representing the distance within the cube.
The length of the wire segment within the cube equals the cube's side length: \( \sqrt{3} \, \text{cm} \), which is \( 0.03 \, \text{m} \).
The enclosed charge \( Q_{\text{enc}} \) within the cube is computed as:
\(Q_{\text{enc}} = \lambda \times l = 2 \times 10^{-9} \, \text{C/m} \times 0.03 \, \text{m} = 6 \times 10^{-11} \, \text{C}\)
The electric flux is then calculated using Gauss's law:
\(\Phi = \frac{Q_{\text{enc}}}{\epsilon_0} = \frac{6 \times 10^{-11} \, \text{C}}{8.85 \times 10^{-12} \, \text{C}^{2}/\text{Nm}^2}\)
The calculation yields:
\(\Phi = \frac{6 \times 10^{-11}}{8.85 \times 10^{-12}} \approx 6.78 \, \text{Nm}^2/\text{C}\)
Consequently, the flux is equivalent to \( 2.16\pi \, \text{Nm}^2/\text{C} \), corresponding to one of the provided options.
Therefore, the correct answer is \( 2.16\pi \).