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Related Concept Videos

Sound Waves: Resonance01:14

Sound Waves: Resonance

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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...
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Design Example: Underdamped Parallel RLC Circuit01:17

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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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Concept of Resonance and its Characteristics01:19

Concept of Resonance and its Characteristics

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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...
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Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:
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Parallel Resonance01:23

Parallel Resonance

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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:
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Resonance and Hybrid Structures02:16

Resonance and Hybrid Structures

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According to the theory of resonance, if two or more Lewis structures with the same arrangement of atoms can be written for a molecule, ion, or radical, the actual distribution of electrons is an average of that shown by the various Lewis structures.
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The Lewis structure of a nitrite anion (NO2−) may actually be drawn in two different ways, distinguished by the locations of the N–O and N=O bonds.
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Correction: Kang et al. Fluid Flow to Electricity: Capturing Flow-Induced Vibrations with Micro-Electromechanical-System-Based Piezoelectric Energy Harvester. <i>Micromachines</i> 2024, <i>15</i>, 581.

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Controlling Resonator Nonlinearities and Modes through Geometry Optimization.

Amal Z Hajjaj1, Nizar Jaber2

  • 1Wolfson School of Mechanical, Electrical and Manufacturing Engineering, Loughborough LE11 3TU, UK.

Micromachines
|November 27, 2021
PubMed
Summary

This study presents a novel hybrid micro-electro-mechanical system (MEMS) resonator design for controlling nonlinearities. Geometry optimization and axial stress tuning enable precise control over resonator dynamics for advanced applications.

Keywords:
MEMS resonatorsgeometry optimizationnonlinearity tailoring

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Area of Science:

  • Micro-Electro-Mechanical Systems (MEMS)
  • Nonlinear Dynamics
  • Resonator Design

Background:

  • Controlling nonlinearities in MEMS resonators is crucial for applications like sensing, signal conditioning, and filtering.
  • Existing methods may lack sufficient control over the complex dynamical behavior of these devices.

Purpose of the Study:

  • To develop a passive technique using geometry optimization to control MEMS resonator nonlinearities and dynamics.
  • To explore active tuning of axial stress as a complementary control method.
  • To investigate a novel hybrid resonator shape for enhanced control.

Main Methods:

  • Proposed a hybrid microbeam design combining straight and initially curved sections.
  • Employed the Galerkin method to solve the beam equation and analyze design parameters.
  • Investigated the effects of geometry on frequency ratios, nonlinearities, symmetry breaking, and linear coupling phenomena (crossing, veering, mode hybridization).

Main Results:

  • Demonstrated the ability to achieve strong quadratic or cubic effective nonlinearities by selecting appropriate structural parameters.
  • Showcased control over symmetry breaking and various linear coupling phenomena.
  • Confirmed the possibility of tuning vibration mode frequencies to achieve commensurate ratios for internal resonance activation.

Conclusions:

  • The proposed hybrid resonator design offers a simple, fabricable, and highly controllable approach to managing MEMS resonator nonlinearities.
  • This method provides a wide range of tunability for sensor nonlinearities and dynamical response.
  • Enables precise control over resonator behavior for advanced MEMS applications.