On the extrapolation behavior of empirical equations of state
暂无分享,去创建一个
[1] G. L. Schott. Shock-compressed carbon dioxide: Liquid measurements and comparisons with selected models , 1991 .
[2] B. Armstrong,et al. A method of correlation using a search procedure, based on a step-wise least-squares technique, and its application to an equation of state for propylene , 1979 .
[3] Richard T. Jacobsen,et al. Thermodynamic Properties of Nitrogen Including Liquid and Vapor Phases from 63K to 2000K with Pressures to 10,000 Bar, , 1973 .
[4] Daniel G. Friend,et al. Thermophysical Properties of Ethane , 1991 .
[5] E. C. Morris. Improved and extended high‐pressure PVT measurements for argon , 1984 .
[6] W. Wagner,et al. A New Equation of State for Carbon Dioxide Covering the Fluid Region from the Triple‐Point Temperature to 1100 K at Pressures up to 800 MPa , 1996 .
[7] W. M. Haynes,et al. Isochoric (p, Vm, T) measurements on CO2 and on (0.982CO2+0.018N2) from 250 to 330 K at pressures to 35 MPa , 1989 .
[8] D. Miller,et al. Joule-Thomson Inversion Curve, Corresponding States, and Simpler Equations of State , 1970 .
[9] William J. Nellis,et al. Shock compression of liquid argon, nitrogen, and oxygen to 90 GPa (900 kbar) , 1980 .
[10] S. Angus,et al. International thermodynamic tables of the fluid state. 5. Methane , 1978 .
[11] R. L. Mills,et al. Sound velocity and the equation of state of N2 to 22 kbar , 1975 .
[12] R. G. Wylie,et al. Accurate method for high pressure PVT measurements and results for argon for T=−20 to +35 °C and p in the range 200–480 MPa , 1980 .
[13] R. D. Gunn,et al. Inversion temperatures and pressures for cryogenic gases and their mixtures , 1966 .
[14] Wolfgang Wagner,et al. A New Equation of State and Tables of Thermodynamic Properties for Methane Covering the Range from the Melting Line to 625 K at Pressures up to 100 MPa , 1991 .
[15] W. Nellis,et al. Equation of state of shock‐compressed liquids: Carbon dioxide and air , 1991 .
[16] Richard T. Jacobsen,et al. Thermodynamic Properties of Argon from the Triple Point to 1200 K with Pressures to 1000 MPa , 1989 .
[17] H. Preston‐Thomas,et al. The International Temperature Scale of 1990 (ITS-90) , 1990 .
[18] K. Pitzer,et al. EQUATIONS OF STATE VALID CONTINUOUSLY FROM ZERO TO EXTREME PRESSURES FOR H2O AND CO2 , 1994 .
[19] K. Pitzer,et al. Equations of state valid continuously from zero to extreme pressures with H2O and CO2 as examples , 1995 .
[20] Richard T. Jacobsen,et al. Thermodynamic Properties of Nitrogen from the Freezing Line to 2000 K at Pressures to 1000 MPa , 1986 .
[21] Manson Benedict,et al. An Empirical Equation for Thermodynamic Properties of Light Hydrocarbons and Their Mixtures I. Methane, Ethane, Propane and n‐Butane , 1940 .
[22] Kenneth S. Pitzer,et al. An equation of state for carbon dioxide valid from zero to extreme pressures , 1994 .
[23] P. Kortbeek,et al. Compressibility and sound velocity measurements on N2 up to 1 GPa , 1988 .
[24] M. Lallemand,et al. Variation of the polarizability of noble gases with density , 1977 .
[25] John S. Rowlinson,et al. The equation of state of dense systems , 1965 .
[26] J. Ely,et al. Application of a new selection algorithm to the development of a wide-range equation of state for refrigerant R134a , 1995 .
[27] Wolfgang Wagner,et al. A new method for optimizing the structure of thermodynamic correlation equations , 1989 .
[28] R. Schmidt,et al. A new form of the equation of state for pure substances and its application to oxygen , 1985 .
[29] R. D. Gunn,et al. Prediction of thermodynamic properties of dense gas mixtures containing one or more of the quantum gases , 1966 .
[30] P. Kortbeek,et al. Apparatus for the measurement of compressibility isotherms of gases up to 10 kbar: Experimental data for argon at 298.15 K , 1988 .
[31] D. Straub. Zur Theorie eines allgemeinen Korrespondenzprinzips der thermischen Eigenschaften fluider Stoffe , 1964 .
[32] W. Sharp,et al. CO2 fugacity at high temperatures and pressures from experimental decarbonation reactions , 1978 .
[33] A. Michels,et al. Isotherms of argon between 0°c and 150°c and pressures up to 2900 atmospheres , 1949 .
[34] V. V. Sychev,et al. Thermodynamic properties of helium , 1987 .