| 000 | 01830nam a2200217Ia 4500 | ||
|---|---|---|---|
| 003 | MX-MdCICY | ||
| 005 | 20250625160157.0 | ||
| 040 | _cCICY | ||
| 090 | _aB-16736 | ||
| 245 | 1 | 0 | _aThermoelastic analysis of 3D generally anisotropic bodies by the boundary element method |
| 490 | 0 | _vEuropean Journal of Computational Mechanics, 25(1-2), p.91-108, 2016 | |
| 520 | 3 | _aIn 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). | |
| 650 | 1 | 4 | _aANALYTICAL VOLUME-TO-SURFACE INTEGRAL TRANSFORMATION |
| 650 | 1 | 4 | _aBOUNDARY ELEMENT METHOD |
| 650 | 1 | 4 | _aTHREE-DIMENSIONAL ANISOTROPIC THERMOELASTICITY |
| 700 | 1 | 2 | _aShiah, Y.C. |
| 700 | 1 | 2 | _aTan, C.L. |
| 856 | 4 | 0 |
_uhttps://drive.google.com/file/d/1Hav4MbfmULpbp-anquR0Y3zMdYZAGdTN/view?usp=drivesdk _zPara ver el documento ingresa a Google con tu cuenta: @cicy.edu.mx |
| 942 |
_2Loc _cREF1 |
||
| 008 | 250602s9999 xx |||||s2 |||| ||und|d | ||
| 999 |
_c50903 _d50903 |
||