5633 - 5645 |
Gas-liquid interfacial mass transfer in trickle-bed reactors: state-of-the-art correlations Iliuta I, Larachi F, Grandjean BPA, Wild G |
5647 - 5666 |
Particle-bed model for multicomponent adsorption-based separations: application to pressure swing adsorption Serbezov A, Sotirchos SV |
5667 - 5675 |
Drop coalescence in turbulent dispersions Liu SP, Li DM |
5677 - 5709 |
Feedback control of nonlinear differential difference equation systems Antoniades C, Christofides PD |
5711 - 5715 |
An alternative to the concept of the interval of quiescence (IQ) in the Monte Carlo simulation of population balances Song M, Qiu XJ |
5717 - 5722 |
Highly porous sphere moving through centerline of circular tube filled with Newtonian fluid Wu RM, Lee DJ |
5723 - 5735 |
Characterisation of gas-liquid two-phase flow inside capillaries Laborie S, Cabassud C, Durand-Bourlier L, Laine JM |
5737 - 5754 |
Particle and bubble movements around tubes immersed in fluidized beds - a numerical study Rong DG, Mikami T, Horio M |
5755 - 5760 |
A method for the measurement of gas concentration distribution in the adsorptive bed Wang ZX, Mo FZ, Shi YQ, Zhou M, Yu GC |
5761 - 5775 |
Experimental investigation of Taylor bubble acceleration mechanism in slug flow Tudose ET, Kawaji M |
5777 - 5786 |
Pressure gradient, liquid hold-up and mass transfer in a graphite fibre bed with cocurrent upward gas-liquid flow Hodgson I, Oloman C |
5787 - 5790 |
Effect of adsorbent shape on adsorption dynamics in a batch adsorber Wang ZL |