2009
DOI: 10.1016/j.cma.2009.04.014
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3D BEM for the general piezoelectric solids

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Cited by 12 publications
(2 citation statements)
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“…The BEM principally requires reduced surface discretizations, and may be regarded as an appealing alternative to the FEM for elastostatic problems (see for example, Banerjee and Henry (1992), Chen and Lin (2010), Cruse (1969), Denda and Wang (2009), Masters and Ye (2004), Milroy et al (1997), Mittelstedt and Becker (2006), Pan and Yuan (2000), Turco and Aristodemo (1998), Wang and Denda (2007), and Wu and Stern (1991), for 3D problems). As the BEM requires no domain discretization, fewer unknowns are needed to be stored.…”
Section: Introductionmentioning
confidence: 99%
“…The BEM principally requires reduced surface discretizations, and may be regarded as an appealing alternative to the FEM for elastostatic problems (see for example, Banerjee and Henry (1992), Chen and Lin (2010), Cruse (1969), Denda and Wang (2009), Masters and Ye (2004), Milroy et al (1997), Mittelstedt and Becker (2006), Pan and Yuan (2000), Turco and Aristodemo (1998), Wang and Denda (2007), and Wu and Stern (1991), for 3D problems). As the BEM requires no domain discretization, fewer unknowns are needed to be stored.…”
Section: Introductionmentioning
confidence: 99%
“…The generalized displacement vector contains the displacements and the electric potential . Using effective coefficients (elastic coefficients , piezoelectric coefficients , and dielectric coefficients ) and average state values (stress Cauchy tensor , strain tensor , electrical displacements , and electric fields ), the constitutive equations for homogeneous material can be expressed as [12][13][14] = − ,…”
Section: Boundary Element Formulationmentioning
confidence: 99%