Abstract
In this work, a model of two-temperature generalized thermoelasticity without energy dissipation for an elastic half-space with constant elastic parameters is constructed. The Laplace transform and state-space techniques are used to obtain the general solution for any set of boundary conditions. The general solutions are applied to a specific problem of a half-space subjected to a moving heat source with a constant velocity. The inverse Laplace transforms are computed numerically, and the comparisons are shown in figures to estimate the effects of the heat source velocity and the two-temperature parameter.
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Abbreviations
- λ, μ :
-
Lamé’s constants
- ρ :
-
density
- C E :
-
specific heat at constant strain
- t :
-
time
- T :
-
dynamical temperature
- T 0 :
-
reference temperature
- θ :
-
dynamical temperature increment (T−T 0)
- φ :
-
conductive temperature
- Q :
-
heat source
- α T :
-
coefficient of linear thermal expansion
- Γ :
-
stress-temperature coefficient (3λ+2μ)αT
- σ ij :
-
components of stress tensor
- e ij :
-
components of strain tensor
- u i :
-
components of displacement vector
- K*:
-
characteristic of theorem
- c 0 :
-
longitudinal wave speed \(\sqrt {\frac{{\lambda + 2\mu }} {\rho }}\)
- η :
-
thermal viscosity \(\frac{{\rho C_E }} {{K^* }}\)
- ɛ T :
-
dimensionless thermoelastic coupling constant \(\frac{{\gamma c_0^2 }} {{K^* }}\)
- C T :
-
dimensionless conductive-dynamical heat coupling constant ηc 20
- a :
-
two-temperature parameter
- β :
-
dimensionless two-temperature parameter ac 20 η 2
- b :
-
dimensionless mechanical coupling constant \(\frac{{\gamma T_0 }} {{\lambda + 2\mu }}\)
- v :
-
heat source velocity
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Youssef, H.M. State-space approach to two-temperature generalized thermoelasticity without energy dissipation of medium subjected to moving heat source. Appl. Math. Mech.-Engl. Ed. 34, 63–74 (2013). https://doi.org/10.1007/s10483-013-1653-7
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DOI: https://doi.org/10.1007/s10483-013-1653-7