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Physics Question on Electric charges and fields

The figures below depict two situations in which two infinitely long static line charges of constant positive line charge density λ\lambda are kept parallel to each other. In their resulting electric field, point charges qq and q-q are kept in equilibrium between them. The point charges are confined to move in the xx direction only. If they are given a small displacement about their equilibrium positions, then the correct statements(s) is(are)

A

Both charges execute simple harmonic motion.

B

Both charges will continue moving in the direction of their displacement.

C

Charge +q executes simple harmonic motion while charge -q continues moving in the direction of its displacement.

D

Charge -q executes simple harmonic motion while charge +q continues moving in the direction of its displacement.

Answer

Charge +q executes simple harmonic motion while charge -q continues moving in the direction of its displacement.

Explanation

Solution

If q is displaced slightly along x axis it will come back to original position
FnetF_{net} on q on displacing by small displacement x = restoring force = λq2πε0(rx)λq2πε0(r+x)\frac{\lambda q}{2\pi\varepsilon_{0}\left(r-x\right)}-\frac{\lambda q}{2\pi \varepsilon _{0}\left(r+x\right)}
F=qλ2πε0[1rx1r+x]\Rightarrow\, F = \frac{q\lambda}{2\pi\varepsilon_{0}} \left[\frac{1}{r-x}-\frac{1}{r+x}\right]
F=qλ×2x2πε0(r2x2)\Rightarrow\,F = \frac{q\lambda\times2x}{2\pi\varepsilon_{0}\left(r^{2}-x^{2}\right)} \quad neglecting x
Frestoring=qλxπε0r2F_{restoring} = \frac{q\lambda x}{\pi\varepsilon_{0}r^{2}}
a=qλxπε0r2a = \frac{q\lambda x}{\pi\varepsilon_{0}r^{2}}
a=qλxmπε0r2a = \frac{q\lambda x}{m\pi\varepsilon_{0}r^{2}}
a?xa ? x so q will do SHM
- q will not able to oscillation as FnetF_{net} on - q will not send it back to its original equilibrium position. - qcontinue moving in direction of its displacement.