Thermophysical properties of 1-hexanol over the temperature range from 303 K to 503 K and at pressures from the saturation line to 400 MPa

[1]  L. Hansen,et al.  n-hexane as a model for compressed simple liquids , 1994 .

[2]  S. Randzio,et al.  An isothermal scanning calorimeter controlled by linear pressure variations from 0.1 to 400 MPa. Calibration and comparison with the piezothermal technique , 1994 .

[3]  J. Grolier,et al.  Excess molar heat capacities and enthalpies for 1-alkanol + N-alkane binary mixtures. New measurements and recommended data , 1993 .

[4]  P. D. Desai,et al.  Thermophysical properties of stainless steels , 1993 .

[5]  J. Grolier,et al.  Thermal expansivities ofn-hexane,n-hexanol and their mixtures over the temperature range from 303 K to 503 K at pressures up to 400 MPa , 1992 .

[6]  M. Zábranský,et al.  Heat Capacities of Organic Compounds in the Liquid State I. C1 to C18 1‐Alkanols , 1990 .

[7]  T. Makita,et al.  Volumetric properties of 1-alkanols at temperatures in the range 298–348 K and pressures up to 40 MPa , 1989 .

[8]  L. Hansen,et al.  An automated calorimeter for the measurement of isobaric expansivities and of isothermal compressibilities of liquids by scanning pressure from 0.1 to 400 MPa at temperatures between 303 and 503 K , 1988 .

[9]  S. Randzio.  An attempt to explain thermal properties of liquids at high pressures , 1986 .

[10]  P. Pruzan,et al.  Thermodynamic properties of water under pressure up to 5 kbar and between 28 and 120 °C. Estimations in the supercooled region down to −40 °C , 1981 .

[11]  M. D. Peña,et al.  Isothermal compressibilities of n-1-alcohols from methanol to 1-dodecanol at 298.15, 308.15, 318.15, and 333.15 K , 1979 .

[12]  F. Lovas,et al.  Microwave Spectra of Molecules of Astrophysical Interest: II Methylenimine , 1973 .

[13]  S. T. Bowden,et al.  The temperature variation of orthobaric density difference in liquid‐vapour systems. III. Alcohols , 1959 .