Step 1: Understand the orientation of the surface.
The rectangular surface is parallel to the x-z plane. This means that the normal vector to the surface is along the y-axis (either \( +\hat{j} \) or \( -\hat{j} \)). We can represent the area vector \( \vec{A} \) as \( \vec{A} = A \hat{j} \), where \( A \) is the area of the surface and \( \hat{j} \) is the unit vector in the y-direction.
Step 2: Use the formula for electric flux.
The electric flux \( \Phi \) through a surface is given by the dot product of the electric field \( \vec{E} \) and the area vector \( \vec{A} \):
\[
\Phi = \vec{E} \cdot \vec{A}
\]
Step 3: Substitute the given electric field and the area vector into the flux formula.
The electric field is \( \vec{E} = (2\hat{i} + 4\hat{j} + 6\hat{k}) \times 10^3 \, N/C \).
The area vector is \( \vec{A} = A \hat{j} \).
The flux is given as \( \Phi = 6.0 \, Nm^2C^{-1} \).
\[
6.0 = [(2\hat{i} + 4\hat{j} + 6\hat{k}) \times 10^3] \cdot (A \hat{j})
\]
The dot product of the unit vectors is \( \hat{i} \cdot \hat{j} = 0 \), \( \hat{j} \cdot \hat{j} = 1 \), and \( \hat{k} \cdot \hat{j} = 0 \).
\[
6.0 = (2 \times 10^3 \hat{i} \cdot A \hat{j}) + (4 \times 10^3 \hat{j} \cdot A \hat{j}) + (6 \times 10^3 \hat{k} \cdot A \hat{j})
\]
\[
6.0 = 0 + (4 \times 10^3 \times A \times 1) + 0
\]
\[
6.0 = 4 \times 10^3 A
\]
Step 4: Solve for the area \( A \) in \( m^2 \).
\[
A = \frac{6.0}{4 \times 10^3} \, m^2
\]
\[
A = 1.5 \times 10^{-3} \, m^2
\]
Step 5: Convert the area from \( m^2 \) to \( cm^2 \).
We know that \( 1 \, m = 100 \, cm \), so \( 1 \, m^2 = (100 \, cm)^2 = 10000 \, cm^2 = 10^4 \, cm^2 \).
\[
A = 1.5 \times 10^{-3} \, m^2 \times \frac{10^4 \, cm^2}{1 \, m^2}
\]
\[
A = 1.5 \times 10^{-3 + 4} \, cm^2
\]
\[
A = 1.5 \times 10^1 \, cm^2
\]
\[
A = 15 \, cm^2
\]
The area of the surface is \( 15 \, cm^2 \).