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NEET PHYSICSEasy

Six charges +q, -q, +q, -q, +q and -q are fixed at the corners of a hexagon of side d as shown in the figure. The work done in bringing a charge q₀ to the centre of the hexagon from infinity is: (ε₀ - permittivity of free space)

A

zero

B

\frac{-q^2}{4\pi\varepsilon_0 d}

C

\frac{-q^2}{4\pi\varepsilon_0 d}(3-\frac{1}{\sqrt{2}})

D

\frac{-q^2}{4\pi\varepsilon_0 d}(6-\frac{1}{\sqrt{2}})

Step-by-Step Solution

  1. Electric Potential: The electric potential (VV) is a scalar quantity. The total potential at the center of the hexagon is the algebraic sum of the potentials due to individual charges.
  2. Geometry: For a regular hexagon of side dd, the distance from each corner to the center is also dd.
  3. Calculation: Vcenter=14πε0Qiri=14πε0d(qq+qq+qq)V_{center} = \frac{1}{4\pi\varepsilon_0} \sum \frac{Q_i}{r_i} = \frac{1}{4\pi\varepsilon_0 d} (q - q + q - q + q - q) Vcenter=14πε0d(0)=0V_{center} = \frac{1}{4\pi\varepsilon_0 d} (0) = 0.
  4. Work Done: The work done (WW) to bring a charge q0q_0 from infinity (where potential is zero) to the center is: W=q0(VcenterV)=q0(00)=0W = q_0(V_{center} - V_{\infty}) = q_0(0 - 0) = 0.
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