Overview
High-rate heating of metallic films is a rapidly emerging area in heat transfer due to the advancement of short-pulse laser technologies and their applications in modern microfabrication technologies. The dual phase-lag (DPL) heat conduction equation [1, 2] has been introduced by including two phase-lags in Fourier law of heat conduction in order to take into account the microstructural effects that arise in high-rate heat transfer. In addition to its applications in the ultrafast pulse laser heating, temperature pulse propagation in liquid helium, nonhomogeneous lagging response in porous media, thermal lagging response in amorphous materials, the DPL heat conduction equation also arises in describing the effects of material defects and thermo-mechanical coupling due to ultrafast heating [3–7]. The dual phase-lag heat conduction model is extended to the dual phase-lag thermoelasticity (DPLTE) [3, 8]. The coupled dynamical thermoelasticity (CTE) theory was developed by Biot [9...
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Mukhopadhyay, S., Kothari, S., Kumar, R. (2014). Dual Phase-Lag Thermoelasticity. In: Hetnarski, R.B. (eds) Encyclopedia of Thermal Stresses. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-2739-7_706
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DOI: https://doi.org/10.1007/978-94-007-2739-7_706
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