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Electric Flux and Field due to Long Charged Wire Piercing Spherical Shell

An infinitely long thin non-conducting line charge oriented parallel to the zz-axis has a uniform charge density λ\lambda. It pierces through a thin non-conducting spherical shell of radius RR such that the intercepted arc PQPQ subtends an angle of 120∘120^\circ at the shell's center OO, as illustrated in the figure. Let ϵ0\epsilon_0 be the permittivity of free space. Which of the following assertions is (are) correct?

Question Diagram 1

Options

A

The total electric flux passing through the spherical shell equals 3Rλ/ϵ0\sqrt{3}R\lambda / \epsilon_0

Correct
B

The zz-component of the electric field vector is zero across all points on the surface of the shell

Correct
C

The total electric flux passing through the spherical shell equals 2Rλ/ϵ0\sqrt{2}R\lambda / \epsilon_0

D

The electric field is perpendicular to the spherical shell surface at every point on it

Step-by-Step Solution

To determine the correct statements, we analyze each option using the principles of electrostatics and Gauss's Law:

  1. Total Electric Flux Through the Spherical Shell: According to Gauss's Law, the total electric flux ΦE\Phi_E passing through a closed surface is given by: ΦE=Qenclosedϵ0\Phi_E = \frac{Q_{\text{enclosed}}}{\epsilon_0} where QenclosedQ_{\text{enclosed}} is the total charge enclosed within the spherical shell.

    The length LL of the line charge segment PQPQ enclosed by the sphere can be calculated using the chord length formula for a circle of radius RR: L=2Rsin⁡(θ2)L = 2R \sin\left(\frac{\theta}{2}\right) Given that the intercepted arc subtends an angle θ=120∘\theta = 120^\circ at the shell's center OO: L=2Rsin⁡(60∘)=2R(32)=3RL = 2R \sin(60^\circ) = 2R \left(\frac{\sqrt{3}}{2}\right) = \sqrt{3}R

    The enclosed charge is therefore: Qenclosed=λL=3RλQ_{\text{enclosed}} = \lambda L = \sqrt{3}R\lambda

    Substituting QenclosedQ_{\text{enclosed}} into Gauss's Law gives: ΦE=3Rλϵ0\Phi_E = \frac{\sqrt{3}R\lambda}{\epsilon_0}

    Thus, Option (A) is correct, and Option (C) is incorrect.

  2. zz-component of the Electric Field: The line charge is infinitely long, straight, uniform, and oriented parallel to the zz-axis. The electric field E⃗\vec{E} at any point due to an infinitely long line charge is directed purely radially outward (or inward) in the plane perpendicular to the line charge (i.e., in the xyxy-plane).

    Consequently, the electric field has no component along the length of the line charge: Ez=0E_z = 0 This holds true for all points in space, including every point on the surface of the spherical shell.

    Thus, Option (B) is correct.

  3. Direction of the Electric Field Relative to the Shell Surface: The normal to the surface of a sphere at any point lies along the radius vector extending from its center OO. For the electric field to be normal to the surface of the shell at all points, the field vectors must be directed radially outward from OO.

    However, the electric field due to the line charge is directed radially outward from the line charge itself, not from the sphere's center OO. Therefore, the electric field vector is not perpendicular to the spherical shell's surface at all points.

    Thus, Option (D) is incorrect.

Correct Answer: (A) and (B)