Suppose A is the position of the bob at any instant of time (Fig. 2.14). From A we drop a perpendicular AB on the z-axis. We have

which shows that z is a small quantity of second order. The potential energy of the bob at A is

Force on the bob along the x-direction is

and the force along the y-direction is

Therefore, we have two uncoupled differential equations along x-and y-directions.

These are simple harmonic motions. These equation can be solved independently:

The constants A1, A2, ϕ1 and ϕ2 are determined by the initial conditions of displacement and velocity in the x-and y-directions. The complete motion can be thought of as a superposition of the motions i x and j y when we neglect the motion in the z-direction. Depending on the phase relationship between ϕ1 and ϕ2 we get an ellipse or a straight line for the path of the bob. For the x- and y-modes of vibrations we have the same frequency ω; the two modes are then said to be ‘degenerate’.