A(t) = Ao e-λt cos(t)where A(t) is the amplitude as a function of time, Ao is the initial amplitude, and lambda (λ), called the log decrement, sets the rate of decay. I wrote about such damped harmonic oscillators in a previous article (Graphene Resonators, June 24, 2011). In a quartz crystal oscillator, the degree of decay, or damping, is related to the crystal's Q-factor; viz., Q = 2π(Energy Stored/Energy Lost per cycle).
Amplitude of a damped harmonic oscillator. In this case, the log decrement is 0.01, giving the equation shown on the plot. (Graph rendered with Gnumeric.) |
One representation of the chaos implicit in the Chua oscillator. This graph of its double scroll attractor is produced by plotting three different voltages in a simulation of the circuit. (Via Wikimedia Commons.)[3] |
Patterns of light distribution in a normal cavity resonator (left) and a chaotic cavity resonator (right). The extra resonant modes for the chaotic cavity are apparent.(York University image, Fratalocchi et al./Nature Photonics, used with permission.)[7] |
"Besides the obvious implications at the fundamental level, where we demonstrate the existence of a fundamental principle of thermodynamics in the framework of Photonics, our results also have real-world practical implications."[7]One practical application would be to increase the interaction time of solar radiation in photovoltaic cells to increase the energy conversion efficiency. York university is already pursuing a program relating to commercial devices.[7-8]