Step 1: The electric flux through the surface is given by the formula:
\[
\Phi_E = \vec{E} \cdot \vec{A}
\]
where \( \vec{A} = A \hat{n} \) is the area vector. Since the surface is square with side length 1 cm, the area is:
\[
A = (1 \, \text{cm})^2 = 1 \times 10^{-4} \, \text{m}^2
\]
Step 2: The electric flux is:
\[
\Phi_E = E A \cos \theta
\]
where \( E = 100 \, \text{N/C} \), \( A = 1 \times 10^{-4} \, \text{m}^2 \), and \( \theta \) is the angle between the electric field vector and the unit normal vector to the surface.
Step 3: To find \( \cos \theta \), we use the dot product of \( \vec{E} \) and \( \hat{n} \):
\[
\cos \theta = \frac{\vec{E} \cdot \hat{n}}{|\vec{E}|}
\]
\[
\vec{E} = 100 \, \hat{i} \, \text{N/C}, \quad \hat{n} = 0.8 \hat{i} + 0.6 \hat{k}
\]
\[
\vec{E} \cdot \hat{n} = (100)(0.8) + (0)(0.6) = 80
\]
\[
|\vec{E}| = 100 \, \text{N/C}
\]
\[
\cos \theta = \frac{80}{100} = 0.8
\]
Step 4: Now, calculate the electric flux:
\[
\Phi_E = 100 \times 1 \times 10^{-4} \times 0.8 = 8 \times 10^{-3} \, \text{N m}^2/\text{C}
\]
Thus, the electric flux through the surface is \( 8 \times 10^{-3} \, \text{N m}^2/\text{C} \).