Author's home page Physics of Oscillations – Contents Free Oscillations and Rotations of a Rigid Pendulum (A Virtual Lab for Undergraduate Students) The most familiar example of a nonlinear mechanical oscillatory system is an ordinary pendulum in the field of gravity, e.g., any rigid body that can swing and rotate about some fixed horizontal axis (a physical, or compound pendulum), or a massive small bob on a rigid rod or spoke of negligible mass (an ideal simple or mathematical pendulum). We exploit a rigid rod rather than a flexible string or wire in order to examine full revolutions of the pendulum as well as its swinging back and forth. A computer model of the pendulum is presented on this page. The Javaapplet requires some time to load, so please be patient while it is starting. After the applet loaded, you can switch to offline mode. Java applets are run by web browsers (with Java plugin installed) under security restrictions to protect the user. In case you have Java 7 or Java 8 installed on your machine, trying to run Java applications generates a message:
Instead of running the applet, you can download the executable jar file (Java archive) OscillationsE.jar in which several simulations are packaged. When you start it, the list of available simulations appears. Select the simulation Oscillations and Revolutions of the Rigid Pendulum from this list, and start it together with the presently opened web page, which gives the description of the simulated physical system. The model allows us to observe the motion of the pendulum. You can vary the time scale by moving the slider (named "Delay" – down on the panel to the left side of the pendulum) for convenient observation. The model allows you also to display the graphs of time dependence of the angle and angular velocity (by checking the corresponding checkboxes on the same panel), as well as the graphs of energy transformations and phase diagram. You can resize and drag with the mouse the panels with graphs and the phase trajectory to any convenient place on the screen. At first acquaintance with the program you can open the list of predefined examples (by using the checkbox under the image of the system). These examples illustrate the most typical kinds of motion of the simulated system. Choosing an example from the list, you need not enter the values of parameters required for the illustrated mode – they will be assigned automatically. A physical pendulum is characterized by its mass m, the moment of inertia I about the axis of rotation, and the distance a between the axis and the center of mass. The differential equation of motion for the physical pendulum is the same as the differential equation for a simple pendulum, whose length L equals I/ma. Consequently, these two systems are dynamically equivalent – they have common variety of possible motions, and it is sufficient to study the simple pendulum. If we use the period of indefinitely small oscillations of the pendulum as a time unit in our mathematical model, then the single parameter remains that completely defines all properties of the system, namely, the dimensionless quality factor Q, that characterises the intensity of viscous friction. The panel on the righthand side of the pendulum allows to vary parameters of the pendulum (absence or presence of viscous friction, and quality factor Q ), and also to change initial conditions of excitation (initial angle of deflection and initial angular velocity). You can change the values either by dragging the sliders, or by typing the desired values from the keyboard (editing the corresponding number fields). In the last case you should press "Enter" key after editing. The model will accept the new values after you press the button "Accept new values". Unlike a linear oscillator, the pendulum is not an isochronous system: its period the longer the larger the amplitude of oscillations. The shape of the graph of the angular deflection versus time at large oscillations differs considerably from a sine curve of oscillations in a linear system. The distinctions become especially evident if the swing approaches 180 degrees. If the total energy, received by the pendulum at the initial excitation, exceeds the maximum possible value of potential energy, the motion is rotational. To be sure, this rotation is periodic (in the absence of friction), but nonuniform: the angular velocity and kinetic energy reach maximum values when the pendulum passes through the lower equilibrium position, and they are minimums when the pendulum overcomes the potential barrier passing through the inverted position. At revolutions in the absence of friction the angular velocity changes periodically, retaining its sign, because the sense of rotation remains the same. Activities:
Principal goals of the lab:

Physics of Oscillations – a Virtual Lab 