2019
DOI: 10.1002/zamm.201800232
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Fundamental solution for extended dislocation in one‐dimensional piezoelectric quasicrystal and application to fracture analysis

Abstract: In this paper, we derive a fundamental solution for extended dislocations of onedimensional (1D) hexagonal piezoelectric quasicrystals. Based on the Stroh formalism, the fundamental solutions for 1D hexagonal piezoelectric quasicrystals expressing by extended dislocations, including phonon, electric, and phason dislocations, are obtained. Then, by considering the continuously distributed dislocations to be a crack, the crack opening displacement, intensity factor, and energy release rate of the extended disloc… Show more

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Cited by 7 publications
(4 citation statements)
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“…For a 1D hexagonal piezoelectric quasicrystal, the anti-plane phonon field displacement u z and phason field displacement w z are coupled with the electric fields E x and E y in the plane and are irrelevant to the vertical co-ordinate z, i.e., u z = u z (x, y), w = w(x, y), E x = E x (x, y), and E y = E y (x, y). The basic equation is as follows [8,28,30].…”
Section: Basic Equationsmentioning
confidence: 99%
See 1 more Smart Citation
“…For a 1D hexagonal piezoelectric quasicrystal, the anti-plane phonon field displacement u z and phason field displacement w z are coupled with the electric fields E x and E y in the plane and are irrelevant to the vertical co-ordinate z, i.e., u z = u z (x, y), w = w(x, y), E x = E x (x, y), and E y = E y (x, y). The basic equation is as follows [8,28,30].…”
Section: Basic Equationsmentioning
confidence: 99%
“…Li and Liu [29] employed the Stroh formula to analyze the electroelasticity of icosahedral quasicrystals with straight dislocations. Fan et al [30] deduced a basic solution for extended dislocations in 1D hexagonal piezoelectric quasicrystals. Lou et al [31] studied a thin elastic inclusion in infinite 1D hexagonal quasicrystals using a hypersingular integral equation.…”
Section: Introductionmentioning
confidence: 99%
“…For 2D deformations in the x 1 x 2 plane, the phonon and phason displacements depend only on the x 1 and x 2 coordinates. Based on the Stroh formalism for a 1D hexagonal piezoelectric QC [24], the phonon and phason displacements u = ( u 1 u 2 u 3 w 2 ) T and the phonon and phason stress function vector Φ can be expressed as…”
Section: Basic Equations and Stroh Formalismmentioning
confidence: 99%
“…Due to these interesting properties, QCs can be used as sensors, actuators, coatings, thermoelectric converters and so on [5]. As such, the investigation on QCs' functions and behaviours has become an essential issue in the field of condensed matter physics, and many topics have been investigated, including defect problems [6][7][8][9][10][11], contact issues [12,13] and static as well as vibration analyses of layered QC structure [14][15][16]. In particular, Zhang et al [17] investigated a spheroidal inclusion embedded within an infinite matrix of a one-dimensional (1D) piezoelectric QC and obtained the explicit expressions.…”
Section: Introductionmentioning
confidence: 99%