Abstract
As in the case of thermomechanical and thermoelectric effects (Chaps. 19,20) we start our consideration of continuous hydrodynamics with a simple discrete model, see Fig. 28.1. A piston with mass m and cross section A can move between two equal parts (1) and (2) of a closed system (for instance a gas). It is impermeable to particles but permeable to heat.
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References
Brenig, W.: Statistische Theorie der Wärme I. Gleichgewicht, 2nd ed. ( Springer, Berlin, Heidelberg 1983 )
Landau, L.D., Placzek, G.: Phys. Z. Sowjetunion 5, 172 (1934)
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© 1989 Springer-Verlag Berlin Heidelberg
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Brenig, W. (1989). The Oscillator with Mechanical and Thermal Attenuation. In: Statistical Theory of Heat. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-74685-7_28
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DOI: https://doi.org/10.1007/978-3-642-74685-7_28
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