Two point charges, each of charge q and mass m, are hung from 1 m long cords and constrained to move in a 2-d plane (so they can swing but not rotate). The charge and mass are chosen such that the when the charges are in their equilibrium position the angle the cords make with the vertical is 0.1 radians. The masses are placed in their equilibrium positions and then each is pulled out by some small angle radians and released. What is the period of the resulting oscillation in seconds ?
Details and assumptions
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The total potential energy of the system is given by a combination of the gravitational and electrostatic potential energies, U = 2 m g L ( 1 − c o s θ ) + k q 2 / ( 2 L s i n θ ) , where k = 1 / ( 4 π ϵ 0 and L is the length of the cords. Since all the angles are small, we can use the small angle approximation which yields
U = m g L θ 2 + 2 L θ k q 2 .
We find the equilibrium position by minimizing U with respect to θ , which yields
θ 0 3 = 4 m g L 2 k q 2 .
We now can expand the potential energy around this minimum by letting θ = θ 0 + Δ θ . Doing so yields that the potential energy is
U = U 0 + m g L Δ θ 0 2 .
Or, in terms of the horizontal x-displacement,
U = U 0 + L m g Δ x 2 .
However, this is just the potential for an harmonic oscillator. The period of such an oscillator is T = 2 π 2 g L = 1 . 4 2 s e c .