2674 - 2674 |
A tribute to John M. Prausnitz Cummings P, O'Connell J, Harold MP |
2675 - 2688 |
John M. Prausnitz: Bridging abstractions and realities O'Connell JP |
2689 - 2701 |
Renewable fuels from biomass: Technical hurdles and economic assessment of biological routes Klein-Marcuschamer D, Blanch HW |
2702 - 2710 |
Population balance modeling of a microalgal culture in photobioreactors: Comparison between experiments and simulations Bertucco A, Sforza E, Fiorenzato V, Strumendo M |
2711 - 2731 |
Molecular thermodynamics of LNA:LNA base pairs and the hyperstabilizing effect of 5'-proximal LNA:DNA base pairs Fakhfakh K, Marais O, Cheng XBJ, Castaneda JR, Hughesman CB, Haynes C |
2732 - 2738 |
Lidocaine-ibuprofen ionic liquid for dermal anesthesia Park HJ, Prausnitz MR |
2739 - 2748 |
Environmental aspects of metals removal from waters and gold recovery Salminen J, Blomberg P, Makinen J, Rasanen L |
2749 - 2756 |
Effects of cell construction parameters on the performance of lithium/sulfur cells Song MK, Zhang YG, Cairns EJ |
2757 - 2762 |
Predicting multicomponent adsorption: 50 years of the ideal adsorbed solution theory Walton KS, Sholl DS |
2763 - 2775 |
Biofuel purification in GME zeolitic-imidazolate frameworks: From ab initio calculations to molecular simulations Zhang K, Gupta KM, Chen YF, Jiang JW |
2776 - 2788 |
Thermodynamic model for the permeability of light gases in glassy polymers Minelli M, Sarti GC |
2789 - 2794 |
Pervaporation of organic compounds from aqueous mixtures using polydimethylsiloxane-containing block copolymer membranes Greer DR, Ozcam AE, Balsara NP |
2795 - 2809 |
Analysis of countercurrent membrane vapor extraction of a dilute aqueous biosolute Liu DE, Cerretani C, Tellez R, Scheer AP, Sciamanna S, Bryan PF, Radke CJ, Prausnitz JM |
2810 - 2823 |
Separation of conglomerate forming enantiomers using a novel continuous preferential crystallization process Vetter T, Burcham CL, Doherty MF |
2824 - 2831 |
Understanding cubic equations of state: A search for the hidden clues of their success Wilczek-Vera G, Vera JH |
2832 - 2840 |
An experimental investigation on the influence of phenol on the solubility of CO2 in aqueous solutions of NaOH Jodecke M, Xia JZ, Kamps APS, Maurer G |
2841 - 2853 |
Liquid li structure and dynamics: A comparison between OFDFT and second nearest-neighbor embedded-atom method Chen M, Vella JR, Panagiotopoulos AZ, Debenedetti PG, Stillinger FH, Carter EA |
2854 - 2860 |
Modeling the permittivity of electrolyte solutions Mollerup JM, Breil MP |
2861 - 2870 |
Thermodynamic mechanism of free heme action on sickle cell hemoglobin polymerization Aich A, Pan WC, Vekilov PG |
2871 - 2880 |
Thermodynamics of protein aqueous solutions: From the structure factor to the osmotic pressure Franco LFM, de Oliveira CLP, Pessoa PD |
2881 - 2890 |
A low-disturbance nonequilibrium molecular dynamics algorithm applied to the determination of thermal conductivities Furtado FA, Abreu CRA, Tavares FW |
2891 - 2912 |
Developing intermolecular-potential models for use with the SAFT-VR Mie equation of state Dufal S, Lafitte T, Galindo A, Jackson G, Haslam AJ |
2913 - 2925 |
Dew-point measurements for water in compressed carbon dioxide Meyer CW, Harvey AH |
2926 - 2932 |
On the simultaneous description of h-bonding and dipolar interactions with point charges in force field models Langenbach K, Engin C, Reiser S, Horsch M, Hasse H |
2933 - 2950 |
An electrolyte CPA equation of state for mixed solvent electrolytes Maribo-Mogensen B, Thomsen K, Kontogeorgis GM |
2951 - 2957 |
High-throughput and comprehensive prediction of H-2 adsorption in metal-organic frameworks under various conditions Liu Y, Zhao SL, Liu HL, Hu Y |
2958 - 2967 |
Modeling permporometry of mesoporous membranes using dynamic mean field theory Rathi A, Edison JR, Ford DM, Monson PA |
2968 - 2976 |
Liquid-liquid phase split in ionic liquid plus toluene mixtures induced by CO2 Canales RI, Brennecke JF |
2977 - 2984 |
Binary and ternary mixtures of liquid crystals with CO2 de Groen M, Vlugt TJH, de Loos TW |
2985 - 2992 |
Application of the functional renormalization group method to classical free energy models Lue L |
2993 - 2999 |
Water and methane in shale rocks: Flow pattern effects on fluid transport and pore structure Ho TA, Striolo A |
3000 - 3011 |
Solvent effects on esterification equilibria Riechert O, Husham M, Sadowski G, Zeiner T |
3012 - 3021 |
Classical density functional theory for methane adsorption in metal-organic framework materials Fu J, Tian Y, Wu JZ |
3022 - 3028 |
Microstructure of room temperature ionic liquids at stepped graphite electrodes Feng G, Li S, Zhao W, Cummings PT |
3029 - 3037 |
Molecular-based virial coefficients of CO2-H2O mixtures Schultz AJ, Kofke DA, Harvey AH |
3038 - 3052 |
High pressure measurements and molecular modeling of the water content of acid gas containing mixtures Fouad WA, Yarrison M, Song KY, Cox KR, Chapman WG |
3053 - 3072 |
Predicting the thermodynamic properties and dielectric behavior of electrolyte solutions using the SAFT-VR plus DE equation of state Das G, Hlushak S, dos Ramos MC, McCabe C |
3073 - 3080 |
Incorporating critical divergence of isochoric heat capacity into the soft-SAFT equation of state Llovell F, Vega LF, Anisimov MA, Sengers JV |
3081 - 3093 |
An improved algorithm for the three-fluid-phase VLLE flash calculation Hinojosa-Gomez H, Solares-Ramirez J, Bazua-Rueda ER |
3094 - 3103 |
A crossover-UNIQUAC model for critical and noncritical LLE calculations Parvaneh K, Haghbakhsh R, Shariati A, Peters CJ |
3104 - 3115 |
Thermodynamics of Flat Thin Liquid Films Myint PC, Firoozabadi A |
3116 - 3137 |
Viscosity and Density of Isobutane Measured in Wide Ranges of Temperature and Pressure Including the Near-Critical Region Herrmann S, Hassel E, Vogel E |
3138 - 3143 |
Diffusion in Fluids Between Knudsen and Fickian Limits: Departure from Classical Behavior Aranovich GL, Donohue MD |