| 1 |
Prediction of thermodynamic properties of pure ionic liquids through extended SAFT-BACK equation of state
Maghari A, ZiaMajidi F
Fluid Phase Equilibria, 356, 109, 2013 |
| 2 |
Prediction of sound velocity and heat capacities of n-alkanes from the modified SAFT-BACK equation of state
Maghari A, Sadeghi MS
Fluid Phase Equilibria, 252(1-2), 152, 2007 |
| 3 |
The BACK equation of state for hydrogen and related compounds
Boublik T
Fluid Phase Equilibria, 240(1), 96, 2006 |
| 4 |
A mixing rule for the quadrupolar contribution to the Helmholtz energy
Weingerl U, Fischer J
Fluid Phase Equilibria, 171(1-2), 59, 2000 |
| 5 |
The use of statistical associating fluid theory to improve the BACK equation of state I. Pure fluids
Zhang ZY, Yang JC, Li YG
Fluid Phase Equilibria, 172(2), 111, 2000 |
| 6 |
Data driven temperature dependence of EOS parameters
Deak A, Kemeny S, Farkas I
Fluid Phase Equilibria, 140(1-2), 97, 1997 |
| 7 |
A Hybrid Equation of State for Stockmayer Pure Fluids and Mixtures
Kriebel C, Muller A, Winkelmann J, Fischer J
Fluid Phase Equilibria, 119(1-2), 67, 1996 |
| 8 |
Simulation Studies on Mixtures of Dipolar with Nonpolar Linear-Molecules .2. A Mixing Rule for the Dipolar Contribution to the Helmholtz Energy
Muller A, Winkelmann J, Fischer J
Fluid Phase Equilibria, 120(1-2), 107, 1996 |
| 9 |
A Cubic Perturbed Hard-Chain Equation of State
Lin HM, Chen JT, Lee MJ
Fluid Phase Equilibria, 126(1), 29, 1996 |
| 10 |
Polarizable Dipolar 2-Center Lennard-Jones Fluids - Computer-Simulations and Equation of State
Kriebel C, Winkelmann J
Journal of Chemical Physics, 105(20), 9316, 1996 |
