545 - 545 |
Prefact to the special issue on mixing Kresta S, Tanguy PA |
546 - 557 |
Laminar mixing in eccentric stirred tank systems Alvarez MM, Arratia PE, Muzzio FJ |
558 - 565 |
Unconventional configuration studies to improve mixing times in stirred tanks Ascanio G, Brito-Bazan M, Brito-De La Fuente E, Carreau PJ, Tanguy PA |
566 - 579 |
Experimental analysis of hydrodynamics induced by a Moritz HAS impeller in laminar and turbulent regimes Escudie R, Line A, Kiener P |
580 - 590 |
Tracer dispersion in stirred tank reactors: Asymptotic properties and mixing characterization Giona M, Paglianti A, Cerbelli S, Pintus S, Adrover A |
591 - 600 |
Investigation of flow patterns in continuous-flow stirred vessels by laser Doppler velocimetry Mavros P, Xuereb C, Fort I, Bertrand J |
601 - 603 |
Power consumption in the turbulent regime for a coaxial mixer Tanguy PA, Thibault F |
604 - 613 |
Morphology development in kenics static mixers (application of the extended mapping method) Galaktionov OS, Anderson PD, Peters GWM, Meijer HEH |
614 - 621 |
The influence of viscosity ratio on mixing effectiveness in a two-fluid laminar motionless mixer Ventresca AL, Cao Q, Prasad AK |
622 - 631 |
Using a new interfacial area transport equation to predict interfacial area in co-current jet mixers Yarbro SL, Long RL |
632 - 637 |
On the applicability of the Grace curve in practical mixing operations Stegeman YW, van de Vosse FN, Meijer HEH |
638 - 652 |
Flow generated by an aerated Rushton impeller: Two-phase PIV experiments and numerical simulations Deen NG, Solberg T, Hjertager BH |
653 - 659 |
Operational characteristics of a new energy-saving impeller for gas-liquid mixing Vlaev SD, Mavros P, Seichter P, Mann R |
660 - 664 |
Simple model to evaluate loading/flooding transition in aerated vessels stirred by Rushton disc turbines Paglianti A |
665 - 673 |
Diagnosis of solid distribution in vessels stirred with multiple PBTs and comparison of two modelling approaches Montante G, Pinelli D, Magelli F |
674 - 681 |
Concept for scale-up of solids suspension in stirred tanks Kraume M, Zehner P |
682 - 687 |
Critical impeller speed for suspending solids in aerated agitation tanks Zhu YG, Wu J |
688 - 694 |
Measuring volumetric phase fractions in a gas-solid-liquid stirred tank reactor using an impedance probe Brunazzi E, Di Festa U, Galletti C, Merello C, Paglianti A, Pintus S |
695 - 709 |
CFD simulations of three-dimensional wall jets in a stirred tank Bhattacharya S, Kresta SM |
710 - 720 |
On the comparison between probability density function models for CFD applications Fissore D, Marchisio DL, Barresi AA |
721 - 726 |
CFD simulation of solids suspension in mixing vessels Kee NCS, Tan RBH |
727 - 733 |
Pressure drop and mass transfer study in static mixers with gas continuous phase Couvert A, Peculier MF, Laplanche A |
734 - 740 |
Flocculation monitoring: Focused beam reflectance measurement as a measurement tool Blanco A, Fuente E, Negro C, Tijero J |
741 - 752 |
An aqueous phase equilibrium calculation algorithm Makkuni A, Phoenix AV, Rohani S |
753 - 763 |
Determination of the optimum conditions for zinc extraction from ore containing sphalerite by HCl solutions Ata ON, Yesilyurt M, Colak S, Bese AV |
764 - 768 |
The effect of adding phosphate on the size of extremely fine needle-like lepidocrocite particles prepared by oxidizing an aqueous suspension of ferrous hydroxide Mihara N, Kawasaki H, Kumazawa H, Choi WS, Kwak JS, Choi HK |
769 - 773 |
Effect of technological factors on electrochemical hydrogenation of lignin Zhang HN, Zhang XY, Xie DM, Liu DH, Li ZH |
774 - 779 |
Dynamic process modelling using a PCA-based output integrated recurrent neural network Qian Y, Cheng HN, Li XX, Jiang YB |
780 - 781 |
Mona Lisa's gaze and smile - Myth or reality? Tamir A |