3415 - 3420 |
Bubble formation at submerged nozzles for small gas flow rate under low gravity Tsuge H, Terasaka K, Koshida W, Matsue H |
3421 - 3428 |
Supercritical extraction of clove bud essential oil : isolation and mathematical modeling Reverchon E, Marrone C |
3429 - 3440 |
A new mechanism for nuclei formation in suspension crystallizers : the role of interparticle forces Qian RY, Botsaris GD |
3441 - 3453 |
The split of horizontal annular flow at a T-junction Roberts PA, Azzopardi BJ, Hibberd S |
3455 - 3462 |
Analysis of autocatalytic reactions with Michaelis-Menten kinetics in an isothermal continuous stirred tank reactor Kumar J, Nath S |
3463 - 3469 |
Determination of the critical residence time for the stability of uniform down-flow in a packed-bed reactor Christoforatou EL, Balakotaiah V |
3471 - 3482 |
A new linear approximation formula for cyclic adsorption in a biporous adsorbent Kim DH |
3483 - 3492 |
Velocity profiles in a closed, unbaffled vessel : comparison between experimental LDV data and numerical CFD predictions Armenante PM, Luo CG, Chou CC, Fort I, Medek J |
3493 - 3498 |
A very effective new method to solve the population balance equation with particle-size growth Song M, Steiff A, Weinspach PM |
3499 - 3509 |
A model for prediction of transient response to the change of fuel feed rate to a circulating fluidized bed boiler furnace Park CK, Basu P |
3511 - 3520 |
Third-phase catalytic activity of halogen exchange reactions in phase transfer catalytic system Ido T, Yamamoto T, Jin G, Goto S |
3521 - 3526 |
Theoretical analysis of mass and heat transfer in monolith catalysts with triangular channels Groppi G, Tronconi E |
3527 - 3542 |
Internal mass transfer in sintered metallic pellets filled with supercritical fluid Stuber F, Julien S, Recasens F |
3543 - 3552 |
Entrance of straight and branched chain compounds from their bulk liquid phase into H-ZSM-5 zeolite Choudhary VR, Choudhary TV |
3553 - 3559 |
Supercritical desorption of bergamot peel oil from silica gel -Experiments and mathematical modelling Reverchon E, Iacuzio G |
3561 - 3578 |
Pattern formation in fixed-bed catalytic reactors - II Trinh S, Ramkrishna D |
3579 - 3588 |
Critical points with the Wong-Sandler mixing rule - II. Calculations with a modified Peng-Robinson equation of state Castier M, Sandler SI |
3589 - 3592 |
Experimental validation of a model allowing pressure gradient determination for non-Newtonian purely viscous fluid-flow through packed beds Sabiri NE, Comiti J |
3593 - 3597 |
Isobaric heat capacities of multicomponent gases between 323 and 423 K and at pressures up to 25 MPa : comparison with some equations of state Dordain L, Coxam JY, Quint R, Grolier JPE, Barreau A, Ingrain D |
3599 - 3603 |
Production of filamentous carbon and hydrogen by solarthermal catalytic cracking of methane Steinfeld A, Kirillov V, Kuvshinov G, Mogilnykh Y, Reller A |
3605 - 3612 |
Identification of the fragmentation mechanisms in wet-phase fine grinding in a stirred bead mill Varinot C, Hiltgun S, Pons MN, Dodds J |
3613 - 3616 |
Mass transport across clathrate hydrate films - a capillary permeation model Mori YH, Mochizuki T |
3617 - 3621 |
Heat transfer in dilute gas-particle suspensions Wang XS, Rhodes MJ, Gibbs BM, Geldart D |