153 - 163 |
The third industrial fluid properties simulation challenge Case FH, Brennan J, Chaka A, Dobbs KD, Friend DG, Frurip D, Gordon PA, Moore J, Mountain RD, Olson J, Ross RB, Schiller M, Shen VK |
164 - 168 |
Benchmarks for the third industrial fluid properties simulation challenge Gordon PA, Schiller M, Kao CPC, Bair S, Friend DG |
169 - 176 |
State conditions transferability of vapor-liquid equilibria via fluctuation solution theory with correlation function integrals from molecular dynamics simulation Christensen S, Peters GH, Hansen FY, O'Connell JP, Abildskov J |
177 - 182 |
Vapor pressure of R227ea+ethanol at 343.13 K by molecular simulation Eckl B, Huang YL, Vrabec J, Hasse H |
183 - 189 |
Prediction, fine tuning, and temperature extrapolation of a vapor liquid equilibrium using COSMOtherm Klamt A, Eckert F |
190 - 194 |
Modeling vapor-liquid equilibria of ethanol+1,1,1,2,3,3,3-heptafluoropropane binary mixtures using PC-SAFT Kleiner M, Sadowski G |
195 - 198 |
Bubble point pressure estimates from Gibbs ensemble simulations Yazaydin AO, Martin MG |
199 - 211 |
Prediction of the bubble point pressure for the binary mixture of ethanol and 1,1,1,2,3,3,3-heptafluoropropane from Gibbs ensemble Monte Carlo simulations using the TraPPE force field Rai N, Rafferty JL, Maiti A, Siepmann JI |
212 - 217 |
Prediction of shear viscosities using periodic perturbation method and OPLS force field Zhao LF, Wang XJ, Wang L, Sun H |
218 - 231 |
Prediction of viscosities and vapor-liquid equilibria for five polyhydric alcohols by molecular simulation Kelkar MS, Rafferty JL, Maginn EJ, Siepmann JI |
233 - 247 |
From restricted towards realistic models of salt solutions: Corrected Debye-Huckel theory and Monte Carlo simulations Abbas Z, Ahlberg E, Nordholm S |
248 - 261 |
Vapor pressure measurements in the range 10(-5) Pa to 1 Pa of four pentaerythritol esters - Density and vapor-liquid equilibria modeling of ester lubricants Razzouk A, Mokbel I, Garcia J, Femandez J, Msakni N, Jose J |
262 - 265 |
Liquid-liquid equilibria of ternary mixture (propargyl alcohol plus diisopropyl ether plus water) Ye KM, Wu H, Deng G |
266 - 274 |
Thermodynamic representation of phase equilibrium behavior of aqueous solutions of amino acids by the modified Wilson model Sadeghi R |
275 - 278 |
The thermal conductivity of alumina nanoparticles dispersed in ethylene glycol Beck MP, Sun TF, Teja AS |
279 - 286 |
Diffusion coefficients of 2-fluoroanisole, 2-bromoanisole, allylbenzene and 1,3-divinylbenzene at infinite dilution in supercritical carbon dioxide Suarez-Iglesias O, Medina I, Pizarro C, Bueno JL |
287 - 294 |
Solubility of disperse yellow 54 in supercritical carbon dioxide with or without cosolvent Tsai CC, Lin HM, Lee MJ |
295 - 299 |
The ternary system H2O-Fe(NO3)(3)-Co(NO3)(2) isotherms 0 and 15 degrees C El Goundali B, Kaddami M |
300 - 315 |
Modelling of calcium sulphate solubility in concentrated multi-component Azimi G, Papangelakis VG, Dutrizac JE |
316 - 325 |
Volume translation in equations of state as a means of accurate property estimation Frey K, Augustine C, Ciccolini RP, Paap S, Modell M, Tester J |
326 - 334 |
Prediction of gas condensate properties by Esmaeilzadeh-Roshanfekr equation of state Bonyadi A, Esmaeilzadeh F |
335 - 342 |
Apparent molar volume, isentropic compressibility and conductivity of di-sodium hydrogen phosphate in water and in aqueous solutions of 1-propanol Sadeghi R, Khoshnavazi R, Parhizkar H |
343 - 353 |
A proposal for the estimation of binary mixture activity coefficients from surface tension measurements throughout the entire concentration range Broco P, Pineiro A, Amigo A, Gracia-Fadrique J |
354 - 358 |
Binary interaction parameter k(ij) for calculating the second cross-virial coefficients of mixtures Meng L, Duan YY, Wang XD |
359 - 359 |
Effect of temperature on the surface tension of diluted aqueous solutions of 1,2-hexanediol, 1,5-hexanediol, 1,6-hexanediol and 2,5-hexanediol (vol 258, pg 67, 2007) Romero CM, Paez MS, Miranda JA, Hernandez DJ, Oviedo LE |