A disk of radius a/4 having a uniformly distributed charge -6C is placed in the x-y plane with its centre at (-a/2,0,0). A rod of length a carrying a uniformly distributed charge 8C is placed on the x-axis from x = a/4 to x = 5a/4. Two point charges -7C and 3C are placed at (-a/4,0,0) and (-3a/4,3a/4,0), respectively. Consider a cubical surface formed by six surfaces x=± a/2, y=± a/2, z=± a/2. The electric flux through this cubical surface is 
Step 1: By Gauss’s law: Φ = fracQₑₙclₒₛₑdvarepsilon₀
Step 2: Charges enclosed by the cube:
• Part of the uniformly charged rod lies inside the cube ⟹ +2C
• The disk lies completely outside the cube ⟹ 0
• One point charge inside contributes accordingly
• Net enclosed charge = 2C
Step 3: Electric flux: Φ = (2C)/(varepsilon₀)

| LIST I | LIST II | ||
| A | Gauss's Law in Electrostatics | I | \(\oint \vec{E} \cdot d \vec{l}=-\frac{d \phi_B}{d t}\) |
| B | Faraday's Law | II | \(\oint \vec{B} \cdot d \vec{A}=0\) |
| C | Gauss's Law in Magnetism | III | \(\oint \vec{B} \cdot d \vec{l}=\mu_0 i_c+\mu_0 \in_0 \frac{d \phi_E}{d t}\) |
| D | Ampere-Maxwell Law | IV | \(\oint \vec{E} \cdot d \vec{s}=\frac{q}{\epsilon_0}\) |