Step 1: Understanding the Question:
The question asks for the total electric flux passing through a cube when a point charge is located exactly at the center of one of its faces. This is a problem solvable using Gauss's Law and symmetry arguments.
Step 2: Key Formula or Approach:
1. Gauss's Law: The total electric flux (\(\Phi\)) through any closed surface (Gaussian surface) is given by:
\[ \Phi = \frac{Q_{enclosed}}{\epsilon_0} \]
Where \( Q_{enclosed} \) is the net charge enclosed by the surface, and \( \epsilon_0 \) is the permittivity of free space.
2. Symmetry for Partial Enclosure: If a charge is not fully enclosed by a single surface, we can construct a larger, perfectly symmetrical closed Gaussian surface by adding identical imaginary surfaces until the charge is completely enclosed. The flux through the original surface will then be a fraction of the total flux through the larger symmetrical surface.
Step 3: Detailed Explanation:
1. The point charge \(+q\) is placed at the center of one face of a cube. This means the charge is on the boundary of the cube, not entirely inside it.
2. To apply Gauss's Law, we need to enclose the charge symmetrically. We can imagine placing another identical cube directly adjacent to the first cube, such that the face on which the charge rests is common to both cubes. This effectively places the charge at the center of the combined, larger cubical volume formed by the two cubes.
3. The combined structure (two cubes) now perfectly encloses the charge \(+q\).
4. According to Gauss's Law, the total electric flux through this combined Gaussian surface (made of two cubes) is:
\[ \Phi_{total} = \frac{+q}{\epsilon_0} \]
5. By symmetry, the electric flux from the charge will pass equally through the two cubes. Therefore, the flux through the single cube in question will be half of the total flux:
\[ \Phi_{cube} = \frac{1}{2} \Phi_{total} = \frac{1}{2} \frac{+q}{\epsilon_0} = \frac{q}{2\epsilon_0} \]
Step 4: Final Answer:
The total electric flux passing through the cube is q/2\(\epsilon_0\).