2307 - 2316 |
Characterization of spouted bed regimes using pressure fluctuation signals Piskova E, Morl L |
2317 - 2329 |
Effect of precursor loading on non-spherical TiO2 nanoparticle synthesis in a diffusion flame reactor Yu MZ, Lin JZ, Chan TL |
2330 - 2340 |
Mathematical modelling of temperature induced moisture migration in bulk powders Bronlund JE, Paterson T |
2341 - 2366 |
Dispersion mechanism of nano-particulate aggregates using a high pressure wet-type jet mill Seekkuarachchi IN, Tanaka K, Kumazawa H |
2367 - 2377 |
On a rapid method to characterize intercrystalline defects in zeolite membranes using pervaporation data Pera-Titus M, Llorens J, Cunill F |
2378 - 2390 |
Inferential closed-loop control of particle size distribution for styrene emulsion polymerization Abedini H, Shahrokhi M |
2391 - 2401 |
Numerical modeling of coupled phenomena in a mechanically stirred molten-glass bath heated by induction Jacoutot L, Fautrelle Y, Gagnoud A, Brun P, Lacombe J |
2402 - 2407 |
Spinodal decomposition of binary mixtures with composition-dependent heat conductivities Molin D, Mauri R |
2408 - 2419 |
Sequential experimental design for model discrimination - Taking into account the posterior covariance matrix of differences between model predictions Schwaab M, Monteiro JL, Pinto JC |
2420 - 2435 |
CFD simulation of flow pattern and plume dimensions in submerged condensation and reactive gas jets into a liquid bath Gulawani SS, Dahikar SK, Joshi JB, Shah MS, RamaPrasad CS, Shukla DS |
2436 - 2449 |
Flow field and residence time distribution simulation of a cross-flow gas-liquid wastewater treatment reactor using CFD Le Moullec Y, Potier O, Gentric C, Leclerc JP |
2450 - 2464 |
Granular pressure and particle velocity fluctuations prediction in liquid fluidized beds Gevrin F, Masbernat O, Simonin O |
2465 - 2476 |
Reactive bed materials for improved biomass gasification in a circulating fluidised bed reactor Pecho J, Schildhauer TJ, Sturzenegger A, Biollaz S, Wokaun A |
2477 - 2483 |
Response surface methodology for optimizing the induction conditions of recombinant interferon beta during high cell density culture Tabandeh F, Khodabandeh M, Yakhchali B, Habib-Ghomi H, Shariati P |
2484 - 2499 |
Mass transfer from ensembles of fluid spheres to a power-law liquid at moderate Reynolds and Peclet numbers Kishore N, Chhabra RR, Eswaran V |
2500 - 2507 |
Application of flow-focusing to the break-up of an emulsion jet for the production of matrix-structured microparticles He YH |
2508 - 2522 |
Using electrical resistance tomography and computational fluid dynamics modeling to study the formation of cavern in the mixing of pseudoplastic fluids possessing yield stress Pakzad L, Ein-Mozaffari F, Chan P |
2523 - 2535 |
Optimization of square microneedle arrays for increasing drug permeability in skin Ai-Qallaf B, Das DB |
2536 - 2547 |
A time-averaged model for gas-solids flow in a one-dimensional vertical channel Benyahia S |
2548 - 2558 |
Fluctuations in dense phase pneumatic conveying of pulverised coal measured using electrical capacitance tomography Azzopardi BJ, Jackson K, Robinson JP, Kaji R, Byars M, Hunt A |
2559 - 2575 |
Mass transfer across the falling film: Simulations and experiments Xu ZF, Khoo BC, Wijeysundera NE |
2576 - 2586 |
Pore-scale derivation of the Ergun equation to enhance its adaptability and generalization Du Plessis JP, Woudberg S |
2587 - 2594 |
Hydrophobic PVDF hollow fiber membranes with narrow pore size distribution and ultra-thin skin for the fresh water production through membrane distillation Wang KY, Chung TS, Gryta M |
2595 - 2600 |
Sugaring-out: A novel phase separation and extraction system Wang B, Ezejias T, Feng H, Blaschek H |