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Question
On the axial line of a dipole (θ = 0°), the electric potential is:
Options
0
\[\frac{2p}{4\pi\varepsilon_0 r^2}\]
\[+\frac{p}{4\pi\varepsilon_0 r^2}\]
\[\pm\frac{p}{4\pi\varepsilon_0 r^2}\]
MCQ
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Solution
On the axial line, θ = 0° at the positive charge end and θ = 180° at the negative charge end. Using \[V = \frac{p\cos\theta}{4\pi\varepsilon_0 r^2}\], we get \[V = +\frac{p}{4\pi\varepsilon_0 r^2}\] on one end and \[-\frac{p}{4\pi\varepsilon_0 r^2}\] on the other, hence the ± notation.
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