Lamb waves propagation in functionally graded piezoelectric materials by Peano-series method

Morched Ben Amor1, Mohamed Hédi Ben Ghozlen1

  • 1Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, B.P.1171, 3000 Sfax, Tunisia.

Ultrasonics
|September 10, 2014
PubMed
Summary

This study explores how Lamb waves propagate in functionally graded piezoelectric materials (FGPMs) using the Peano-series expansion method. The material properties of aluminum nitride are assumed to change exponentially along the thickness direction. The researchers analyze the lowest-order symmetric (S0) and antisymmetric (A0) Lamb wave modes. They find that the S0 mode has a higher electromechanical coupling factor than the A0 mode. The coupling factor maxima shift toward higher frequencies as the gradient coefficient increases. The Peano-series method is validated as effective for FGPM analysis in MATLAB. The results suggest that FGPMs can be tailored for sensor applications by adjusting gradient properties. The findings may help design high-performance sensors working at different frequency ranges.

Frequently Asked Questions

Related Concept Videos

Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.7K
Sound as Pressure Waves01:17

Sound as Pressure Waves

Sound waves, which are longitudinal waves, can be modeled as the displacement amplitude varying as a function of the spatial and temporal coordinates. As a column of the medium is displaced, its successive columns are also displaced. As the successive displacements differ relatively, a pressure difference with the surrounding pressure is created. The gauge pressure varies across the medium.
The pressure fluctuation depends on the difference in displacements between the successive points in the...
3.3K
Traveling Waves: Lossless Lines01:27

Traveling Waves: Lossless Lines

The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx and a shunt capacitance CΔx.
559
Graphing the Wave Function01:13

Graphing the Wave Function

Consider the wave equation for a sinusoidal wave moving in the positive x-direction. The wave equation is a function of both position and time. From the wave equation, two different graphs can be plotted.
3.3K
The de Broglie Wavelength02:32

The de Broglie Wavelength

In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.5K
Propagation of Waves01:07

Propagation of Waves

When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
2.5K