Three charges on a ring Three particles of equal mass m are placed on a ring of radius R. Two of the particles have charge q and the third has a charge Q. (a) Find the equilibrium configuration of the charges for general q and Q. Be sure to consider both qQ> 0 and qQ <0. (You will find an equation that relates the angles between the particles and their charges. This equation can't be solved in general, however comment on special cases and check various limits.) (b) Solve the equation from part (a) for q = Q. For this case, consider small pertur- bations of the charges around their equilibrium positions. Find the frequencies and eigenmodes. Ignore friction.

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Three charges on a ring
Three particles of equal mass m are placed on a ring of radius R. Two of the particles
have charge q and the third has a charge Q.
(a) Find the equilibrium configuration of the charges for general q and Q. Be sure to
consider both qQ> 0 and qQ <0. (You will find an equation that relates the angles
between the particles and their charges. This equation can't be solved in general,
however comment on special cases and check various limits.)
(b) Solve the equation from part (a) for q = Q. For this case, consider small pertur-
bations of the charges around their equilibrium positions. Find the frequencies and
eigenmodes. Ignore friction.
Transcribed Image Text:Three charges on a ring Three particles of equal mass m are placed on a ring of radius R. Two of the particles have charge q and the third has a charge Q. (a) Find the equilibrium configuration of the charges for general q and Q. Be sure to consider both qQ> 0 and qQ <0. (You will find an equation that relates the angles between the particles and their charges. This equation can't be solved in general, however comment on special cases and check various limits.) (b) Solve the equation from part (a) for q = Q. For this case, consider small pertur- bations of the charges around their equilibrium positions. Find the frequencies and eigenmodes. Ignore friction.
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(a) The force on each charge due to the other two charges can be found using Coulomb's law. The force on each charge will be a vector sum of the forces due to the other two charges. The direction of the force will be radially inward or outward, depending on whether the charges have the same or opposite sign. In general, the angle between the charges and the force on each charge will depend on the specific values of q and Q.

 

In the case where qQ>0, the charges will repel each other and will be arranged such that the angle between them is maximized. In the case where qQ<0, the charges will attract each other and will be arranged such that the angle between them is minimized.

 

find the equilibrium configuration of the charges, we need to consider the electrostatic forces acting on each particle. Since the charges are placed on a ring, we can assume that the particles are fixed at the vertices of an equilateral triangle with side length 2R.

 

The electrostatic force on a charge q due to the other two charges is given by F = kqQ/r^2, where k is Coulomb's constant, Q is the charge of the other particle, and r is the distance between the two particles.

 

We can use the law of cosines to relate the angles between the particles and the distance between them.

 

Let theta be the angle between the charges q and Q, and phi be the angle between the charge Q and the third charge.

 

The distance between charges q and Q is Rsqrt(3) * cos(theta)

 

The distance between charges Q and the third charge is Rsqrt(3) * cos(phi)

 

The distance between charges q and the third charge is R*sqrt(3) * cos(pi - theta - phi)

 

Using these equations and the fact that the charges are in equilibrium (i.e., the net force on each charge is zero), we can derive a transcendental equation that relates the angles theta and phi to the charges q and Q.

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