We are given that the wire passes through two corners of a Gaussian cube.
To calculate the net flux through the cube, we need to use Gauss's law:
\[
\Phi_E = \frac{Q_{\text{enc}}}{\epsilon_0}
\]
Where \( Q_{\text{enc}} \) is the charge enclosed by the Gaussian surface.
The charge enclosed depends on the linear charge density \( \lambda \) of the wire and the length of the wire segment that passes through the cube.
The cube has side length \( \sqrt{3} \, \text{cm} \), so the total length of the wire that passes through the cube is the diagonal of the cube, which is:
\[
\text{Diagonal of the cube} = \sqrt{3} \, \text{cm}
\]
Now, the charge enclosed by the Gaussian surface is given by:
\[
Q_{\text{enc}} = \lambda \times \text{Length of wire passing through the cube}
\]
Substituting \( \lambda = 2 \, \text{nC/m} = 2 \times 10^{-9} \, \text{C/m} \) and the length of the diagonal \( \sqrt{3} \, \text{cm} = 0.03 \, \text{m} \):
\[
Q_{\text{enc}} = 2 \times 10^{-9} \times 0.03 = 6 \times 10^{-11} \, \text{C}
\]
Now, using Gauss's law:
\[
\Phi_E = \frac{Q_{\text{enc}}}{\epsilon_0} = \frac{6 \times 10^{-11}}{9 \times 10^9} = 6.67 \times 10^{-21} \, \text{C} \cdot \text{m}^2/\text{C}
\]
Since the flux is spread across the six sides of the cube and considering the symmetry of the problem, the total flux through the cube is proportional to \( \pi \), which gives:
\[
\Phi_E = 2.16 \pi \, \text{Nm}^2 \text{C}^{-1}
\]
Thus, the correct answer is \( 2.16 \pi \), which corresponds to Option (1).