Related Experiment Video
Updated: Jul 11, 2026

11:44
Real-Time DC-dynamic Biasing Method for Switching Time Improvement in Severely Underdamped Fringing-field Electrostatic MEMS Actuators
Published on: August 15, 2014
Controlling transitions in a Duffing oscillator by sweeping parameters in time
1Caltech, Pasadena, California 91125, USA. oleg@caltech.edu
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 13, 2007
Summary
A frequency sweep in a Duffing oscillator can control transitions between system states. This occurs via a long-lasting transient near an unstable point, with lifetime dependent on sweep rate.
Area of Science:
- Nonlinear Dynamics
- Oscillator Physics
Background:
- Duffing oscillators exhibit complex behaviors under external driving frequencies.
- Understanding state transitions is crucial for controlling nonlinear systems.
Purpose of the Study:
- To investigate controlled state transitions in a high-Q Duffing oscillator using a time-varying driving frequency.
- To analyze the role of unstable fixed points in mediating these transitions.
Main Methods:
- Simulating a weakly nonlinear Duffing oscillator with a frequency sweep from sigma i to sigma f at rate r.
- Analyzing the system's dynamics, focusing on transient behavior near saddle-type fixed points.
Main Results:
- Controlled transitions between two stable states were achieved via frequency sweeping.
- Transitions proceed through a long-lived transient state near a saddle-type unstable fixed point.
- The transient lifetime was found to scale as -(ln|r-rc|)lambda r, where rc is the critical sweep rate and lambda r is the repulsive eigenvalue.
Conclusions:
- Frequency sweeping offers a method for controlled state transitions in Duffing oscillators.
- The dynamics near unstable saddle points significantly influence the transition process.
- The derived scaling law provides insights into the transient behavior and its dependence on system parameters.
Related Concept Videos
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...
Although friction and other non-conservative...
Design Example: Underdamped Parallel RLC Circuit
Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
Starting with a fixed...
Types of Damping
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
RLC Circuit as a Damped Oscillator
An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
Time-Domain Interpretation of PD Control
Proportional-Derivative (PD) control is a widely used control method in various engineering systems to enhance stability and performance. In a system with only proportional control, common issues include high maximum overshoot and oscillation, observed in both the error signal and its rate of change. This behavior can be divided into three distinct phases: initial overshoot, subsequent undershoot, and gradual stabilization.
Consider the example of control of motor torque. Initially, a positive...
Consider the example of control of motor torque. Initially, a positive...
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