Abstract
The poroelasticity theory presented so far assumes an isothermal condition, that is, temperature remains unchanged during the deformation and diffusion process. In practice, however, temperature of a porous medium can change. Not only it can change if it is in contact with a body of different temperature, and heat is transferred by conduction, but also the deformation itself can generate internal heat. In addition, heat can be transported in and out of the porous medium by a fluid flow.
If two corpuscles of a body lie infinitely close and have different temperature, the warmer corpuscle transmits a certain amount of its heat to the other one; and this heat—given from the warmer corpuscle to the colder one at a given time and during a given moment—is proportional to the temperature difference, if the difference has a small value.
—Joseph Fourier (1822)
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Notes
- 1.
McTigue [47] used the notations \((\alpha '_{s},\,\alpha ''_{s},\,\alpha _{f})\) for coefficient of thermal expansion. The correspondences with the current notations are α′ s  = β d and ϕ(α f −α″ s ) = β v . In the table, McTigue further assumed α′ s  = α″ s  = α s , which corresponds to the ideal porous medium model of K ψ  = β ψ  = 0. These assumptions lead to the consistent result of β d  = β s and β v  = ϕ(β f −β s ) in (11.54) and (11.60) in the current model. Also, the value of α e ( = b′ of McTigue) for rock salt has been corrected in the table.
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Cheng, A.HD. (2016). Porothermoelasticity. In: Poroelasticity. Theory and Applications of Transport in Porous Media, vol 27. Springer, Cham. https://doi.org/10.1007/978-3-319-25202-5_11
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