Four electric charges +q, +q, -q and -q are placed at the corners of a square of side 2L (see figure). The electric potential at point A, mid-way between the two charges +q and +q, is
\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1+\frac{1}{\sqrt{5}})
\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1-\frac{1}{\sqrt{5}})
Zero
\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1+\sqrt{5})
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