description of the user interface
The four buttons on the right side are used to control the Demonstration. The reset button brings the Demonstration back to the initial conditions. There are two main sets of control variables. One set is for setting the initial conditions for the top spring, and the second set is used for setting the initial conditions for the lower spring. The "relax" check box for the lower spring is used to put the spring into the relaxed position. For the top spring the relaxed position is set at
, while the lower spring is assumed to have zero relaxed length located at the point where the two springs are joined. You can see a trace of the bob motion using the "trace" check box. You can see the location of the center of mass (CM) of the whole system using the "show CM" checkbox.
The result has three parts. The counters show the current state. The field labeled "energy" is the sum of the potential energy (P.E.) and the kinetic energy (K.E.). The field labeled
is the total angular momentum of the system. The field labeled
is the current extension of the top spring measured from its relaxed position. You can see different plots by selecting the plot type using the pop-up menu labeled "plot type". The main display shows the pendulum itself as it swings.
A pop-up menu labeled "test case" is used to select one of three preconfigured parameters. Click the run button after selecting a test case to start the Demonstration.
The Demonstration runs with no throttling by using a single dynamic variable called "gTick
" that is updated at the end of each Manipulate
expression evaluation so that the Manipulate
expression is reevaluated again immediately. This lets the Demonstration run at the maximum speed. A slider labeled "speed" can be used to adjust the speed of the Demonstration as needed.
The Demonstration runs continuously until you stop it. All units used are in SI.
derivation of equations of motion
The equations of motion are derived using the Lagrangian procedure. Raleigh's method is used for the top spring such that the effective mass used is
of the top spring mass. This effective mass is added to the bob mass to account for the vertical displacement of the top spring. The bob has three degrees of freedom: the distance
is along the length of lower spring where
is the location where the top pendulum attached to the lower pendulum, the angle of rotation
, the vertical displacement of the top spring. For more information on the derivation of the equations of motion, please see the author's report
 David Morin, Introduction to Classical Mechanics: With Problems and Solutions,
New York: Cambridge University Press, 2008.
 REA's Problem Solver's Mechanics Static and Dynamics,
New Jersey: Research and Education Association, 2002.
 D. A. Wells, Lagrangian Dynamics
, New York: Schaums' Outline, 1967.
 S. Timoshenko, Vibration Problems In Engineering,
New York: D. Van. Nostrand, 1937.