Oscillation of a point charge perpendicular to field lines

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Homework Help Overview

The problem involves two charged particles A and B, each with charge Q, separated by a distance D, and a third particle C with charge q and mass m positioned at the midpoint between A and B. The focus is on determining the time period of oscillation for particle C when it is displaced perpendicularly from the line connecting A and B.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • Participants discuss the expression for the force acting on particle C and question its dependence on the separation distance D. There is an exploration of the components of the force and how they interact when particle C is displaced.

Discussion Status

Some participants have pointed out potential errors in the original force equation and are examining the implications of these errors. There is an ongoing inquiry into the nature of the forces involved and the assumptions made regarding their cancellation.

Contextual Notes

There is a noted concern regarding the dimensional correctness of the force equation and its behavior as particle C approaches the midpoint, specifically when x approaches zero. Participants are questioning the assumptions about the forces acting on particle C and how they relate to the fixed charges A and B.

CrazyNeutrino
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Homework Statement


Two particles A and B each carry a charge Q and are separated by a fixed distance D. A particle c with charge q and mass m is kept at the midpoint of A and B. If C is displaced perpendicular to AB by a distance x where x<<<D,
find the time period of the oscillation of the charge.

Homework Equations


$$F=\frac{Qq}{4 \pi \epsilon_0 x^3} \cdot \hat{x}$$
$$a=-\omega^2 x$$

The Attempt at a Solution


I started off by trying to find an expression for the force acting on the particle. Since the components of the force parallel to AB cancel out because the charges at A & B are the same, I took the vector sum of the perpendicular force in the ##\hat{x}## direction.
$$ma=-\frac{2Qq}{4\pi\epsilon_0 x^3}\cdot \hat{x}$$

I then solved for ##a## and plugged the coefficients into ##a=\omega^2 x##.
This gives:
$$\omega^2=\frac{Qq}{4 \pi \epsilon_0 x^3}$$
$$ \frac{2\pi}{T}=\sqrt{\frac{Qq}{4 \pi \epsilon_0 x^3}} $$
$$ T = \sqrt{\frac{8\pi^3\epsilon_0 x^3 m}{qQ}}$$

This is wrong.
 
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Your equation $$F=\frac{Qq}{4 \pi \epsilon_0 x^3} \cdot \hat{x}$$ is incorrect. There should be dependence on D, the separation between the fixed charges. It's also dimensionally incorrect and predicts that F is infinite when x = 0. Actually, F = 0 when x = 0.
 
kuruman said:
Your equation $$F=\frac{Qq}{4 \pi \epsilon_0 x^3} \cdot \hat{x}$$ is incorrect. There should be dependence on D, the separation between the fixed charges. It's also dimensionally incorrect and predicts that F is infinite when x = 0. Actually, F = 0 when x = 0.
I understand the dimensionality argument. How and why does the force depend on the charge separation though? Wouldn’t those components cancel each other out?
 
CrazyNeutrino said:
How and why does the force depend on the charge separation though?
What is the magnitude of the force exerted by one charge Q? What direction is it in? What component is left after cancellation by the force from the other charge?
 

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