Charged pendulum

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 θ 0 \theta_0 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 Δ θ = 0.01 \Delta \theta=0.01 radians and released. What is the period of the resulting oscillation in seconds ?

Details and assumptions

  • The acceleration of gravity is 9.8 m / s 2 -9.8~m/s^2 .


The answer is 1.42.

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1 solution

David Mattingly Staff
May 13, 2014

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 ) U=2mgL(1-cos \theta)+kq^2/(2Lsin \theta) , where k = 1 / ( 4 π ϵ 0 k=1/(4\pi\epsilon_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 + k q 2 2 L θ U=mgL\theta^2+\frac{kq^2}{2L\theta} .

We find the equilibrium position by minimizing U with respect to θ \theta , which yields

θ 0 3 = k q 2 4 m g L 2 \theta_0^3=\frac{kq^2}{4mgL^2} .

We now can expand the potential energy around this minimum by letting θ = θ 0 + Δ θ \theta=\theta_0+\Delta \theta . Doing so yields that the potential energy is

U = U 0 + m g L Δ θ 0 2 U=U_0+mgL\Delta \theta_0^2 .

Or, in terms of the horizontal x-displacement,

U = U 0 + m g L Δ x 2 U=U_0+\frac {mg}{L}\Delta x^2 .

However, this is just the potential for an harmonic oscillator. The period of such an oscillator is T = 2 π L 2 g = 1.42 s e c T=2\pi\sqrt{\frac{L}{2g}}=1.42~sec .

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