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A boundary element method for anisotropic coupled thermoelasticity

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Summary

A boundary element formulation is presented for the solution of the equations of fully coupled thermoelasticity for materials of arbitrary degree of anisotropy. By employing the fundamental solutions of anisotropic elastostatics and stationary heat conduction, a system of equations with time-independent matrices is obtained. Since the fundamental solutions are uncoupled and time-independent, a domain integral remains in the representation formula which contains the time-dependence as well as the thermoelastic coupling. This domain integral is transformed to the boundary by means of the dual reciprocity method. By taking this approach, the use of dynamic fundamental solutions is avoided, which enables an efficient calculation of system matrices. In addition, the solution of transient processes as well as, free and forced vibration analysis becomes straightforward and can be carried out with standard time-stepping schemes and eigensystem solvers. Another important advantage of the present formulation is its versatility, since it includes a number of simplified thermoelastic theories, viz. the theory of thermal stresses, coupled and uncoupled quasi-static thermoelasticity, and stationary thermoelasticity. The accuracy of the new thermoelastic boundary element method is demonstrated by a number of example problems.

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Correspondence to L. Gaul.

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Support by the Deutsche Forschungsgemeinschaft (DFG) of the Graduate Collegium ‘Modelling and discretization methods for continua and fluids’ (GKKS) at the University of Stuttgart is gratefully acknowledged.

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Kögl, M., Gaul, L. A boundary element method for anisotropic coupled thermoelasticity. Archive of Applied Mechanics 73, 377–398 (2003). https://doi.org/10.1007/s00419-003-0289-2

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  • DOI: https://doi.org/10.1007/s00419-003-0289-2

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