Validation of an accurate vibrating-wire densimeter: Density and viscosity of liquids over wide ranges of temperature and pressure

A new vibrating-wire instrument for the meaasurement of the density of fluids at high pressures was described in a previous paper. The technique makes use of the buoyancy force on a solid sinker and detect, this force with a vibrating wire placed inside the measuring cell. Owing to the simple geometry of the oscillating element there exists a complete theoretical description of its resonance characteristics. enabling the calculation of the density of the fluid from their measurement. In the present paper a new method for the determination of the cell constants is outlined which permits the operation of the densimeter essentially as an absolute instrument. Furthermore. it is shown that the viscosity ol the fluid can be measured Simultaneously with the density. New results for three fluids are presented: for cyclohexane at temperatures from 298 to 348 K and pressures up to 40 MPa. for 2,2,4-trimethylpentane between 197 and 348 K at 0.1 MPa, and for 1,1,1,2-tetrafluoroethane from 197 to 298 K close to saturation. The sets of measurements where chosen with the intention of testing the performance of the apparatus. complementing previous work at higher pressures. The densities and viscosities measured exhibit the same accuracy for all of the three fluids over the entire temperature and pressure ranges and were obtained using the same set of cell parameters The precision of the densities is ±0.03% and their estimated accuracy is ±0.05%. File viscosities have a precision of ±0.6%, and an estimated accuracy of ±2%.

[1]  J. Kestin,et al.  Feasibility of simultaneous viscosity and density measurements of a fluid from the motion of an oscillating disk , 1987 .

[2]  S. Richardson,et al.  The theory of a vibrating-rod densimeter , 1986 .

[3]  N. B. Vargaftik Tables on the thermophysical properties of liquids and gases: In normal and dissociated states , 1975 .

[4]  R. Reid,et al.  The Properties of Gases and Liquids , 1977 .

[5]  Yoshiaki Tanaka,et al.  Viscosity and density of binary mixtures of cyclohexane with n-octane, n-dodecane, and n-hexadecane under high pressures , 1991 .

[6]  W. Wakeham,et al.  A vibrating-wire densimeter for liquids at high pressures: The density of 2,2,4-trimethylpentane from 298.15 to 348.15 K and up to 100 MPa , 1994 .

[7]  Stephen P. Timoshenko,et al.  Vibration problems in engineering , 1928 .

[8]  J. D. Isdale,et al.  Transport properties of nonelectrolyte liquid mixtures—VII. Viscosity coefficients for isooctane and for equimolar mixtures of isooctane + n-octane and isooctane + n-dodecane from 25 to 100°C at pressures up to 500 MPa or to the freezing pressure , 1985 .

[9]  L. Woolf,et al.  Thermodynamic properties of 2,2,4-trimethylpentane , 1990 .

[10]  Marc J. Assael,et al.  Vibrating-wire viscometers for liquids at high pressures , 1992 .

[11]  D. K. Ward,et al.  Thermodynamic properties of two alternative refrigerants : 1,1-dichloro-2,2,2-trifluoroethane (R123) and 1,1,1,2-tetrafluoroethane (R134a) , 1991 .

[12]  K. E. Bett,et al.  A vibrating-rod densimeter , 1989 .

[13]  W. Wakeham,et al.  The viscosity of liquid R134a , 1993 .

[14]  Iain G. Main,et al.  Vibrations and Waves in Physics , 1985 .

[15]  M. Dix,et al.  A vibrating-wire densimeter for measurements in fluids at high pressures , 1991 .

[16]  John H. Dymond,et al.  The Tait equation: 100 years on , 1988 .

[17]  H. Baehr,et al.  An International Standard Formulation for the Thermodynamic Properties of 1,1,1,2‐Tetrafluoroethane (HFC‐134a) for Temperatures from 170 K to 455 K and Pressures up to 70 MPa , 1994 .

[18]  G. C. Benson,et al.  A Micrometer Syringe Dilatometer: Application to the Measurement of the Excess Volumes of some Ethylbenzene Systems at 298.15 K , 1975 .

[19]  Haruki Sato,et al.  Saturated liquid densities of HCFC 123 and HFC 134a , 1990 .

[20]  D. P. Wilson,et al.  Thermophysical properties of 1,1,1,2-tetrafluoroethane (R-134a) , 1989 .