A thin spherical shell of radius R and surface charge density \( \sigma \) is placed in a cube of side 5R with their centers coinciding. The electric flux through one face of the cube is (\( \epsilon_o \) = Permittivity of free space)
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Symmetry arguments are crucial in Gauss's Law problems. If a charge distribution is symmetric with respect to the enclosing surface faces, simply divide the total flux by the number of faces.
According to Gauss's Law, the total electric flux \( \phi_{\text{total}} \) through a closed surface enclosing a charge \( q \) is \( \frac{q}{\epsilon_o} \). Due to the symmetry of the cube with the sphere at its center, the flux is distributed equally among the 6 faces.
Step 2: Key Formula or Approach:
1. Total charge on shell: \( q = \text{Surface Area} \times \sigma = 4\pi R^2 \sigma \).
2. Total Flux: \( \phi_{\text{total}} = \frac{q}{\epsilon_o} \).
3. Flux through one face: \( \phi_{\text{face}} = \frac{1}{6} \phi_{\text{total}} \).
Step 3: Detailed Explanation:
Calculate the total charge \( q \):
\[ q = \sigma (4\pi R^2) \]
Total flux through the cube:
\[ \phi_{\text{total}} = \frac{4\pi R^2 \sigma}{\epsilon_o} \]
Since the sphere is centered in the cube, flux through each of the 6 faces is identical.
\[ \phi_{\text{face}} = \frac{1}{6} \times \frac{4\pi R^2 \sigma}{\epsilon_o} \]
\[ \phi_{\text{face}} = \frac{2\pi R^2 \sigma}{3 \epsilon_o} \]
Step 4: Final Answer:
The flux through one face is \( \frac{2\pi R^2 \sigma}{3 \epsilon_o} \).