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Related Concept Videos

Parallel Resonance01:23

Parallel Resonance

The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
Concept of Resonance and its Characteristics01:19

Concept of Resonance and its Characteristics

If a driven oscillator needs to resonate at a specific frequency, then very light damping is required. An example of light damping includes playing piano strings and many other musical instruments. Conversely, to achieve small-amplitude oscillations as in a car's suspension system, heavy damping is required. Heavy damping reduces the amplitude, but the tradeoff is that the system responds at more frequencies. Speed bumps and gravel roads prove that even a car's suspension system is not immune...
Sound Waves: Resonance01:14

Sound Waves: Resonance

Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...
Forced Oscillations01:06

Forced Oscillations

When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
Linear Approximation in Frequency Domain01:26

Linear Approximation in Frequency Domain

Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear.
Design Example: Underdamped Parallel RLC Circuit01:17

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...

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Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements
14:18

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Published on: February 28, 2016

Weak-periodic stochastic resonance in a parallel array of static nonlinearities.

Yumei Ma1, Fabing Duan, François Chapeau-Blondeau

  • 1College of Automation Engineering, Qingdao University, Qingdao, People's Republic of China.

Plos One
|March 19, 2013
PubMed
Summary

This study shows that increasing the size of nonlinear element arrays always improves signal-to-noise ratio (SNR) gain. Stochastic resonance does not occur with optimal nonlinearities, but can be achieved with simpler threshold nonlinearities.

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Area of Science:

  • Nonlinear dynamics
  • Signal processing
  • Statistical physics

Background:

  • Investigating methods to enhance signal transmission in noisy environments.
  • Understanding the behavior of parallel arrays of nonlinear elements.

Purpose of the Study:

  • To derive an explicit expression for the output-input signal-to-noise ratio (SNR) gain in uncoupled parallel arrays of static nonlinear elements.
  • To analyze the SNR gain as a function of array size and nonlinearity.
  • To explore the conditions under which stochastic resonance occurs or is precluded.

Main Methods:

  • Derivation of an explicit expression for SNR gain in the small-signal limit.
  • Mathematical analysis of SNR gain as a function of array size and nonlinearity.
  • Investigation of locally optimal and threshold nonlinearities.

Main Results:

  • SNR gain is a monotonically increasing function of array size for any static nonlinearity.
  • Locally optimal nonlinearity provides an upper bound for SNR gain.
  • Stochastic resonance does not occur with locally optimal nonlinearity.
  • Stochastic resonance can occur in arrays of suboptimal threshold nonlinearities, potentially exceeding unity SNR gain.

Conclusions:

  • Array size is a key factor in improving SNR gain for nonlinear systems.
  • The choice of nonlinearity critically affects SNR gain and the occurrence of stochastic resonance.
  • Threshold nonlinearities offer a practical approach for achieving stochastic resonance and high SNR gain in specific scenarios.