Pendulum with a moving pivot
Carl Madigan
Nova Scotia Agricultural College
Truro, N.S. B2N 5E3
Introduction
The problem being considered is a non-linear pendulum where the point of suspension is moving. Damping is ignored but can easily be included.
If X represents the horizontal and Y the vertical components of the motion of the pivot then by resloving the accelerations along the pendulum we have
where g is the acceleration due to gravity.
the pendulum's



Setting F = ma and equating
elliminating T from these two equations we have



simplifying
We will assume L =1 and consider three types of motion for the pivot a) horizontally
b) vertically X = 0 
c) circular
In the examples below XX(t) and YY(t) are used to define the pivot
Example 1 Horizontal motion of the pivot
Plot of the positon wrt time
animation of the motion for this pendulum









Example 2 Vertical motion
Plots of the position with respect to time and also of the phase plane for this example
animation of the motion of this pendulum.









Example 3 Circular motion

plots of the position with respect to time and of the phase plane
animation of the motion for this pendulum










A Procedure for drawing the pendulums
The procedure is called drad and has the following imputs
L = length ,
angl = inital displacement angle,
vel = initial velocity
a = the x component of the path for the pivot
b = the y component of the pivot's path
n = the number of iterations used to draw the annimations
examples for horizontal motion try a =
for vertical motion try a = 0 and b =
for circular motion try a =
and b = sin(3t - π/2)
experiment with other paths such as a = sin(2.25t - π/2) b = cos(2t + π/4) etc try varying the lenght and the initial conditions. Have Fun with it!!!

























Example 1. pivot moving along a curve
Additional examples
Example 1 horizontal motion of the pivot
Example 2 vertical motion of the pivot
Example 3 cicular motion of the pivot
Drawing the pendulums
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