TY - JOUR
T1 - Thermoelastic analysis of 3D generally anisotropic bodies by the boundary element method
AU - Shiah, Y. C.
AU - Tan, C. L.
N1 - Funding Information:
This work was supported by the Ministry of Science and Technology of Taiwan [No. 102-2221-E-006-290-MY3].
Publisher Copyright:
© 2016 Informa UK Limited, trading as Taylor & Francis Group.
PY - 2016/3/3
Y1 - 2016/3/3
N2 - In the boundary element method (BEM) for stress analysis, it is well known that thermal loads give rise to an additional volume integral in the primary form of the boundary integral equation (BIE). This volume integral needs to be further transformed to surface ones in order to retain the characteristic of the BEM as a boundary solution technique. In this study of the BEM for 3D thermoelasticity in general anisotropy, the fundamental solutions are expressed as Fourier series with coefficients calculated using an explicit-form Green’s function. In the exact volume-to-surface integral transformation associated with the term for the thermal effects in the BIE, a new kernel function is constructed. All formulations are implemented in an existing BEM code for 3D elastostatic analysis. Some numerical examples are presented to demonstrate the veracity of the formulations and the implementation, where the numerical results are compared with those obtained using the finite element method (FEM).
AB - In the boundary element method (BEM) for stress analysis, it is well known that thermal loads give rise to an additional volume integral in the primary form of the boundary integral equation (BIE). This volume integral needs to be further transformed to surface ones in order to retain the characteristic of the BEM as a boundary solution technique. In this study of the BEM for 3D thermoelasticity in general anisotropy, the fundamental solutions are expressed as Fourier series with coefficients calculated using an explicit-form Green’s function. In the exact volume-to-surface integral transformation associated with the term for the thermal effects in the BIE, a new kernel function is constructed. All formulations are implemented in an existing BEM code for 3D elastostatic analysis. Some numerical examples are presented to demonstrate the veracity of the formulations and the implementation, where the numerical results are compared with those obtained using the finite element method (FEM).
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U2 - 10.1080/17797179.2016.1181038
DO - 10.1080/17797179.2016.1181038
M3 - Article
AN - SCOPUS:84969265045
SN - 1779-7179
VL - 25
SP - 91
EP - 108
JO - European Journal of Computational Mechanics
JF - European Journal of Computational Mechanics
IS - 1-2
ER -