020509 Bandyopadhyay N;Roychoudhuri S K (Math Dep, Burdwan Univ, Golapbag, Burdwan, W.B.) : Thermo-elastic wave propagation without energy dissipation in an elastic half-space. Bull Calcutta Mathl Soc 2005, 97(6), 489-502.
Generalized dynamical theory of thermo-elasticity without energy dissipation (Type II) proposed by Green and Naghdi (GN) (1993) is used to study one dimensional thermo-elastic wave propagation in an elastic half space with plane boundary subjected to a (i) step-input of stress and zero temperature (ii) zero stress and step-input of temperature (iii) zero stress and suddenly applied temperature. The exact discontinuities of the fields at the wave fronts are studied analyzed in detail. The displacement is found to be continuous at both the wave fronts while temperature and stress suffer finite jump at these locations in cases (i) and (ii). In case (iii), displacement suffer finite discontinuity at the two wave fronts while temperature and stress suffer delta function singularity at both the elastic and thermal wave fronts. The results derived are compared with earlier results. In the temperature-rate dependent theory of thermo-elasticity (Green and Lindsay (GL) 1972), though the displacement and temperature are both continuous at both the wave fronts, in the GN theory of thermoelasticity, the temperature and stress suffer finite jumps at these locations in case (i). In case (iii), using GN theory, displacement is discontinuous at the two wave fronts while temperature and stress suffer delta function singularity at these locations. But in the temperature-rate dependent theory (GL theory), it is observed that displacement, temperature and stress-all exhibit delta function singularity at these locations. The thermo elastic theory without energy dissipation brings into light some results not encountered in the previous results obtained by using temperature rate dependent theory of GL. In case (ii), the temperature and stress suffer finite jumps at the two wave fronts in GN theory while the displacement is observed to be continuous at these locations.
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