Question:

As shown in the figure, a surface encloses an electric dipole with charges ±6×106C \pm6 \times 10^{-6} \, {C} . The total electric flux through the closed surface is:


 

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Remember that for any closed surface enclosing a dipole, the net electric flux is always zero, regardless of the dipole's orientation within the surface. This is a direct result of Gauss's Law.
Updated On: Mar 13, 2025
  • +12×106Nm2C1 +12 \times 10^{-6} \, {Nm}^2{C}^{-1}
  • 12×106Nm2C1 -12 \times 10^{-6} \, {Nm}^2{C}^{-1}
  • Zero
  • +6×106Nm2C1 +6 \times 10^{-6} \, {Nm}^2{C}^{-1}
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The Correct Option is C

Solution and Explanation

Step 1: Apply Gauss's Law for a closed surface. Gauss's Law states that the total electric flux through a closed surface is proportional to the charge enclosed within that surface. For a dipole with charges ±6×106C \pm6 \times 10^{-6} \, {C} , the net charge enclosed is zero: Qenc=+6×106C+(6×106C)=0C Q_{{enc}} = +6 \times 10^{-6} \, {C} + (-6 \times 10^{-6} \, {C}) = 0 \, {C} Step 2: Calculate the electric flux. Since the net enclosed charge Qenc Q_{{enc}} is zero, the electric flux Φ \Phi through the surface is: Φ=Qencϵ0=0Cϵ0=0Nm2C1 \Phi = \frac{Q_{{enc}}}{\epsilon_0} = \frac{0 \, {C}}{\epsilon_0} = 0 \, {Nm}^2{C}^{-1}
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