981 |
The effect of aqueous NaCl solution on methane hydrate nucleation and growth Bai DS, Wu ZY, Lin CJ, Zhou D Fluid Phase Equilibria, 487, 76, 2019 |
982 |
Experimental and theoretical investigations on the adherent behaviors of high viscosity liquid: The effect of surface topography Wu CY, Zhu Q, Zheng T, Yang XN, Wang TZ, Hou B, He XD, Luo G, Li SB, Chen MJ Fluid Phase Equilibria, 486, 11, 2019 |
983 |
Computing solubility parameters of deep eutectic solvents from Molecular Dynamics simulations Salehi HS, Ramdin M, Moultos OA, Vlugt TJH Fluid Phase Equilibria, 497, 10, 2019 |
984 |
Pressure-viscosity relation of 2,2,4-trimethylhexane predicted using all-atom TEAM force field Gong Z, Sun H Fluid Phase Equilibria, 497, 64, 2019 |
985 |
Enhancement of the predictive power of molecular dynamics simulations for the determination of self-diffusion coefficient and viscosity demonstrated for propane Higgoda UA, Hellmann R, Koller TM, Froba AP Fluid Phase Equilibria, 496, 69, 2019 |
986 |
Mie 16-6 force field predicts viscosity with faster-than-exponential pressure dependence for 2,2,4-trimethylhexane Messerly RA, Anderson MC, Razavi SM, Elliott JR Fluid Phase Equilibria, 495, 76, 2019 |
987 |
Calculation of viscosities of branched alkanes from 0.1 to 1000 MPa by molecular dynamics methods using COMPASS force field Kondratyuk ND, Pisarev VV Fluid Phase Equilibria, 498, 151, 2019 |
988 |
Transport property prediction and inhomogeneity analysis of supercritical n-Dodecane by molecular dynamics simulation Chen C, Jiang X Fuel, 244, 48, 2019 |
989 |
Deep structure analysis on coal slags with increasing silicon content and correlation with melt viscosity Xuan WW, Wang HN, Xia DH Fuel, 242, 362, 2019 |
990 |
Comparative analysis of bark and woodchip biomass piles for enhancing predictability of self-heating Krigstin S, Helmeste C, Jia HZ, Johnson KE, Wetzel S, Volpe S, Faizal W, Ferrero F Fuel, 242, 699, 2019 |