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NEET PHYSICSMedium

Charges +q+q and q-q are placed at points A and B, respectively, which are at a distance 2L2L apart. C is the midpoint between A and B. The work done in moving a charge +Q+Q along the semicircle CRD is:

A

qQ4πϵ0L\frac{qQ}{4\pi\epsilon_0 L}

B

qQ2πϵ0L\frac{qQ}{2\pi\epsilon_0 L}

C

qQ6πϵ0L\frac{qQ}{6\pi\epsilon_0 L}

D

qQ6πϵ0L-\frac{qQ}{6\pi\epsilon_0 L}

Step-by-Step Solution

  1. Conservative Nature: The work done by the electrostatic force is independent of the path taken and depends only on the potential difference between the final and initial points [NCERT Class 12, Sec 2.1]. Thus, the work done moving charge QQ from C to D is W=Q(VDVC)W = Q(V_D - V_C).
  2. Potential at C (Midpoint): Point C is equidistant (LL) from +q+q and q-q. The potential VCV_C is the sum of potentials due to individual charges: VC=14πϵ0(+qL+qL)=0V_C = \frac{1}{4\pi\epsilon_0} \left( \frac{+q}{L} + \frac{-q}{L} \right) = 0
  3. Location of D: While the diagram is not provided, the options and the nature of the problem (AIPMT 2007) imply that D is a point on the axis of the dipole, situated at distance LL from B (outside the dipole). Thus, the distance from +q+q (at A) is 3L3L and from q-q (at B) is LL.
  4. Potential at D: VD=14πϵ0(+q3L+qL)=q4πϵ0L(131)=q4πϵ0L(23)=q6πϵ0LV_D = \frac{1}{4\pi\epsilon_0} \left( \frac{+q}{3L} + \frac{-q}{L} \right) = \frac{q}{4\pi\epsilon_0 L} \left( \frac{1}{3} - 1 \right) = \frac{q}{4\pi\epsilon_0 L} \left( -\frac{2}{3} \right) = -\frac{q}{6\pi\epsilon_0 L}
  5. Work Done: W=Q(VDVC)=Q(q6πϵ0L0)=qQ6πϵ0LW = Q(V_D - V_C) = Q \left( -\frac{q}{6\pi\epsilon_0 L} - 0 \right) = -\frac{qQ}{6\pi\epsilon_0 L}
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