Given an electric field \( \vec{E} = (10x + 5) \hat{i} \) N/C, where \( x \) denotes the position along the x-axis. The electric flux \( \Phi_E \) through a closed surface is calculated using Gauss's law as \( \Phi_E = \oint \vec{E} \cdot d\vec{A} \), which equates the net flux to the enclosed charge divided by \( \epsilon_0 \). Here, \( d\vec{A} \) is the vector area element of the cube's surface.
Step 1: Electric Field Representation
The electric field is defined as \( \vec{E} = (10x + 5) \hat{i} \). This indicates the field has an x-component that varies with the x-coordinate.
Step 2: Flux Calculation per Face
A cube has six faces. The flux through each face is determined by the dot product of the electric field and the face's area vector \( \vec{E} \cdot d\vec{A} \). The area vector is normal to the surface. The flux through a face is given by \( \Phi_{\text{face}} = \vec{E} \cdot A \), where \( A \) is the face area. Since \( \vec{E} \) is purely in the x-direction, only the faces perpendicular to the x-axis (at \( x = 0 \) and \( x = L \)) contribute to the net flux.
Step 3: Flux at \( x = 0 \) and \( x = L \)
1. Face at \( x = 0 \):
At \( x = 0 \), \( \vec{E} = 5 \hat{i} \) N/C. The face area is \( A = L^2 \). The area vector points in the negative x-direction. Thus, the flux is:
\[\Phi_1 = E_x \cdot A = 5 \times L^2 = 5L^2\]
2. Face at \( x = L \):
At \( x = L \), \( \vec{E} = (10L + 5) \hat{i} \) N/C. The area vector points in the positive x-direction. Thus, the flux is:
\[\Phi_2 = E_x \cdot A = (10L + 5) \times L^2 = (10L + 5) L^2\]
Step 4: Total Flux
The total flux is the difference between the flux through the face at \( x = L \) and the face at \( x = 0 \):
\[\Phi_{\text{total}} = \Phi_2 - \Phi_1 = (10L + 5) L^2 - 5L^2\]
\[\Phi_{\text{total}} = 10L^3\]
The net electric flux through the cube is \( \Phi_{\text{total}} = 10L^3 \, \text{Nm}^2/\text{C} \).