Abstract
Calculation of an equation of state and thermodynamic functions is the starting point for a whole set of calculations of thermophysical properties of a substance under strong shock compression and heating [1–6]. Thermodynamic calculation is also an inherent part of hydrodynamic simulation of shock compression. The feature of this interrelation is that the thermodynamic data employed as input information for a very wide and important class of hydrodynamic flows such as adiabatic flows (irreversible shock compression, reversible isentropic compression and expansion, throttling, etc.) are limited in principle by the use of a reduced caloric equation of state that is incomplete from the thermodynamic point of view. This equation of state is an expression for the internal energy (or enthalpy) as a function, U(P, V), of the conjugate thermodynamic variables, pressure and specific volume.
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Gryaznov, V.K., Iosilevskiy, I.L., Fortov, V.E. (2004). Thermodynamic Properties of Shock-Compressed Plasmas Based on a Chemical Picture. In: Fortov, V.E., Al’tshuler, L.V., Trunin, R.F., Funtikov, A.I. (eds) High-Pressure Shock Compression of Solids VII. High-Pressure Shock Compression of Condensed Matter. Springer, New York, NY. https://doi.org/10.1007/978-1-4757-4048-6_14
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