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Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
Oscillations about an Equilibrium Position01:04

Oscillations about an Equilibrium Position

Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so because...
Damped Oscillations01:07

Damped Oscillations

In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Time and frequency -Domain Interpretation of Phase-lag Control01:21

Time and frequency -Domain Interpretation of Phase-lag Control

Phase-lag controllers are widely used in control systems to improve stability and reduce steady-state errors. A dimmer switch controlling the brightness of a light bulb serves as a practical example of phase-lag control, gradually adjusting the bulb's brightness. Mathematically, phase-lag control or low-pass filtering is represented when the factor 'a' is less than 1.
Phase-lag controllers do not place a pole at zero, but instead influence the steady-state error by amplifying any finite,...
Graphical and Analytic Representation of Sinusoids01:20

Graphical and Analytic Representation of Sinusoids

Analyzing two sinusoidal voltages with equal amplitude and period but different phases on an oscilloscope, an instrument used to display and analyze waveforms, involves a three-step process.
The first step is measuring the peak-to-peak value, which is twice the amplitude of the sinusoid. This provides information about the maximum voltage swing of the waveform.
Secondly, the period and angular frequency are determined. The period is the time taken for one complete cycle of the waveform, while...
Time and frequency -Domain Interpretation of Phase-lead Control01:24

Time and frequency -Domain Interpretation of Phase-lead Control

Phase-lead controllers are commonly used in various control systems to enhance response speed and stability. Adjusting the brightness on a television screen offers a practical example of phase-lead control. When contrast is enhanced, a phase-lead controller is employed. Mathematically, phase-lead control is identified when the first parameter is smaller than the second.
The design of phase-lead control involves the strategic placement of poles and zeros to balance steady-state error and system...

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Related Experiment Video

Updated: Jun 17, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

Identical phase oscillators with global sinusoidal coupling evolve by Mobius group action.

Seth A Marvel1, Renato E Mirollo, Steven H Strogatz

  • 1Center for Applied Mathematics, Cornell University, Ithaca, New York 14853, USA. sam255@cornell.edu

Chaos (Woodbury, N.Y.)
|January 12, 2010
PubMed
Summary

The governing equations for N identical phase oscillators with global sinusoidal coupling are generated by the Mobius group. This reveals the underlying cause of low-dimensional dynamics, partitioning state space into invariant manifolds.

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Area of Science:

  • Complex Systems Dynamics
  • Mathematical Physics
  • Nonlinear Dynamics

Background:

  • Systems of N identical phase oscillators with global sinusoidal coupling exhibit low-dimensional dynamics.
  • The cause of this phenomenon has been a long-standing puzzle in the field for approximately 20 years.

Purpose of the Study:

  • To uncover the hidden structure responsible for the low-dimensional dynamics in these oscillator systems.
  • To mathematically prove the origin of the observed phenomenon.

Main Methods:

  • Proving that the governing equations are generated by the action of the Mobius group.
  • Demonstrating how the group action partitions the N-dimensional state space into three-dimensional invariant manifolds (group orbits).
  • Identifying N-3 functionally independent cross ratios of oscillator phases as constants of motion.

Main Results:

  • The Mobius group, a subgroup of fractional linear transformations, generates the system's equations.
  • The N-dimensional state space is foliated into three-dimensional invariant manifolds by the group action.
  • The N-3 cross ratios of oscillator phases are the functionally independent constants of motion, indicating no further general reduction is possible.

Conclusions:

  • The Mobius group action provides a fundamental explanation for the low-dimensional dynamics of coupled phase oscillators.
  • The identified invariant manifolds and constants of motion offer a new framework for analyzing these complex systems.
  • Numerical experiments suggest these invariant manifolds may contain regions of neutrally stable chaos, particularly in models like Josephson junction arrays.