1 - 14 |
An excluded volume theory of lattice fluids part II-incorporating specific models of attractive and repulsive interaction energy Martinez GM |
15 - 36 |
Generalized equation of state for the cyclic hydrocarbons over a temperature range from the triple point to 700 K with pressures up to 100 MPa Grigor'ev B, Alexandrov I, Gerasimov A |
37 - 43 |
Improving thermodynamic consistency among vapor pressure, heat of vaporization, and liquid and ideal gas isobaric heat capacities through multi-property optimization Hogge JW, Messerly R, Giles N, Knotts T, Rowley R, Wilding WV |
44 - 49 |
Scaled equation of state and specific thermodynamic behavior of near-critical methane-pentane binary mixture Belyakov MY, Gorodetskii EE, Kulikov VD, Voronov VP, Grigoriev BA |
50 - 56 |
Thermodynamic consistency testing of PTx-data via the Gibbs-Helmholtz equation 2.: Methodology and limitations Olson JD |
57 - 61 |
The effects of Na addition on the density, surface tension and viscosity of liquid Sn-Zn alloys Gancarz T, Gasior W |
62 - 73 |
A Weeks-Chandler-Andersen based potential fitting procedure for molecular dynamics simulations of the calcite-water interface Sjoblom S, Kvamme B, Kuznetsova T |
74 - 87 |
A generalized cubic equation of state for non-polar and polar substances Forero LA, Velasquez JA |
88 - 93 |
Surface tension of silanes: A new equation Di Nicola G, Coccia G, Pierantozzi M |
94 - 99 |
Accurate density measurements on a binary mixture (carbon dioxide plus methane) at the vicinity of the critical point in the supercritical state by a single-sinker densimeter Yang XX, Wang Z, Li Z |
100 - 107 |
Computing bubble-points of CO2/CH4 gas mixtures in ionic liquids from Monte Carlo simulations Ramdin M, Balaji SP, Vicent-Luna JM, Torres-Knoop A, Chen Q, Dubbeldam D, Calero S, de Loos TW, Vlugt TJH |
108 - 118 |
Speed of sound measurement in ethyl tert-butyl ether and tert-amyl methyl ether by Brillouin light scattering Zheng X, Zhang Y, He MG |
119 - 124 |
Separation of 1,3-dioxolane from its azeotropic aqueous solution by using Good's buffer ionic liquid [TMA] [EPPS] Gupta BS, Fang MY, Lee MJ |
125 - 132 |
Measurements of the speed of sound in liquid and supercritical ethane El Hawary A, Meier K |
133 - 151 |
Fundamental equation of state correlation for hexamethyldisiloxane based on experimental and molecular simulation data Thol M, Dubberke FH, Rutkai G, Windmann T, Koster A, Span R, Vrabec J |
152 - 159 |
Free energy of solvation and Henry's law solubility constants for mono-, di- and tri-ethylene glycol in water and methane Olsen R, Kvamme B, Kuznetsova T |
160 - 174 |
Thermodynamic modeling of aqueous systems containing amines and amine hydrochlorides: Application to methylamine, morpholine, and morpholine derivatives Lencka MM, Kosinski JJ, Wang PM, Anderko A |
175 - 180 |
Speed of sound measurements in deuterium oxide (D2O) over the temperature range from (278.2 to 353.2) K at pressures up to 20 MPa Wegge R, Richter M, Span R |
181 - 191 |
Comparing the structure of different ionic liquid series: Bistriflamide v. hexafluorophosphate; pure v. equimolar mixtures Shimizu K, Lopes JNC |
192 - 197 |
Tris(2-ethylhexyl) trimellitate (TOTM) as a potential industrial reference fluid for viscosity at high temperatures and high pressures: New viscosity, density and surface tension measurements Diogo JCF, Avelino HMNT, Caetano FJP, Fareleira JMNA, Wakeham WA |
198 - 203 |
Measurements of the viscosities of Kr and Xe by the two-capillary viscometry Lin H, Che J, Zhang JT, Feng XJ |
204 - 223 |
Modeling and calculation of thermodynamic properties and phase equilibria of oil and gas condensate fractions based on two generalized multiparameter equations of state Gerasimov A, Alexandrov I, Grigoriev B |