Electrostatics

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195 of 311

Question 195 of 311

A two point charges 4q4q and –q–q are fixed on the xx -axis at x=−d2x=\dfrac{-d}{2} and x=d2x=\dfrac{d}{2}, respectively. If the third point charge ‘qq ’ is taken from the origin to x=dx=d along the semicircle as shown in the figure, the energy of the charge will:

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Answer: (D) decrease by 4q23π∈0d\dfrac{4{q}^{2}}{3\pi {\in }_{0}d}


Potential at origin
OO, the potential due to two charges is given by
V0=4q4πϵ0(d2)+(−q)4πϵ0(d2)=6q4πϵ0d{V}_{0}=\dfrac{4q}{4\pi {\epsilon }_{0}\left(\dfrac{d}{2}\right)}+\dfrac{\left(-q\right)}{4\pi {\epsilon }_{0}\left(\dfrac{d}{2}\right)}=\dfrac{6q}{4\pi {\epsilon }_{0}d}
Potential at
PP at a distance, x=dx=d is given by
VP=4q4πϵ0(3d2)+(−q)4πϵ0(d2)=q6πϵ0d{V}_{P}=\dfrac{4q}{4\pi {\epsilon }_{0}\left(\dfrac{3d}{2}\right)}+\dfrac{\left(-q\right)}{4\pi {\epsilon }_{0}\left(\dfrac{d}{2}\right)}=\dfrac{q}{6\pi {\epsilon }_{0}d}
Change in potential energy due the charge motion of charge
qq is given by
∆U=qΔV=q(Vf−Vi)∆U=q\Delta V=q\left({V}_{f}-{V}_{i}\right)
⇒∆U=q(VP−VO)\Rightarrow ∆U=q\left({V}_{P}-{V}_{O}\right)
∆U=q(q6πϵ0d−3q2πϵ0d)=−4q23πϵ0d∆U=q\left(\dfrac{q}{6\pi {\epsilon }_{0}d}-\dfrac{3q}{2\pi {\epsilon }_{0}d}\right)=-\dfrac{4{q}^{2}}{3\pi {\epsilon }_{0}d}

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