1193 - 1197 |
Origin of pressure fluctuations in fluidized beds Puncochar M, Drahos J |
1199 - 1210 |
The second law optimal state of a diabatic binary tray distillation column Rosjorde A, Kjelstrup S |
1211 - 1217 |
Preferential oxidation of carbon monoxide in hydrogen-rich gas over platinum-cobalt-alumina aerogel catalysts Kwak C, Park TJ, Suh DJ |
1219 - 1236 |
A method for time and spatially resolved measurement of convective heat transfer coefficient (h) in complex flows Vitrac O, Trystram G |
1237 - 1249 |
Simulation of imbalance reduction between two reactors in an ethylene dichloride cracker Park Y, Choi BS, Yi J |
1251 - 1265 |
On the origin of heterogeneous structure in dense gas-solid flows Li H, Kuipers JAM |
1267 - 1276 |
Discrete element study of particle circulation in a 3-D spouted bed Takeuchi S, Wang XS, Rhodes MJ |
1277 - 1293 |
Modelling of polyacrylamide gel dosimeters with spatially non-uniform radiation dose distributions Fuxman AM, McAuley KB, Schreiner LJ |
1295 - 1301 |
Modeling the controlled release of drug embedded in a plate-like polymer matrix Lin SH, Hsu JP, Tseng S |
1303 - 1312 |
An improved integral non-linear model for the contact of particles in distinct element simulations Di Renzo A, Di Maio FP |
1313 - 1321 |
Is subcooling the right driving force for testing low-dosage hydrate inhibitors? Arjmandi M, Tohidi B, Danesh A, Todd AC |
1323 - 1336 |
Hopf bifurcation and solution multiplicity in a model for destabilized Bridgman crystal growth Sonda P, Yeckel A, Daoutidis P, Derby JJ |
1337 - 1347 |
Chiral separation of beta-blocker drug (nadolol) by five-zone simulated moving bed chromatography Wang X, Ching CB |
1349 - 1362 |
Synthesis of mass exchange network for batch processes - Part II: Minimum units target and batch network design Foo CY, Manan ZA, Yunus RM, Aziz RA |
1363 - 1370 |
Validation of radiotracer technology in dynamic scaling experiments in porous media Stamatakis E, Haugan A, Dugstad O, Muller J, Chatzichristos C, Bjornstad T, Palyvos I |
1371 - 1381 |
Experimental validation of a simple model for gas-liquid slug flow in horizontal pipes Orell A |
1383 - 1387 |
Particle size effect of CH4 hydrate for self-preservation Takeya S, Uchida T, Nagao J, Ohmura R, Shimada W, Kamata Y, Ebinuma T, Narita H |
1389 - 1399 |
Mass transfer investigations in electrodeionization processes using the microcolumn technique Monzie I, Muhr L, Lapicque F, Grevillot G |
1401 - 1409 |
Characteristics of non-uniform reaction blocks for chemical heat pump Lee CH, Park SH, Choi SH, Kim YS, Kim SH |
1411 - 1427 |
Effect of adsorption of organic solvents on the band profiles in reversed-phase non-linear chromatography Poplewska I, Antos D |
1429 - 1440 |
A population balance approach to describing bulk attrition Ouchiyama N, Rough SL, Bridgwater J |
1441 - 1448 |
Analysis of the milling rate of pharmaceutical powders using the Distinct Element Method (DEM) Kwan CC, Mio H, Chen YQ, Ding YL, Saito F, Papadopoulos DG, Bentham AC, Ghadiri M |
1449 - 1464 |
A novel algorithm for solving population balance equations: the parallel parent and daughter classes. Derivation, analysis and testing Bove S, Solberg T, Hjertager BH |
1465 - 1475 |
Effect of liquid properties on the performance of bubble column reactors with fine pore spargers Mouza AA, Dalakoglou GK, Paras SV |
1477 - 1489 |
Modeling simultaneous biological clogging and physical plugging in trickle-bed bioreactors for wastewater treatment Iliuta I, Larachi F |
1491 - 1495 |
Numerical evidence for a "highway in state space" for reactors with minimum entropy production Johannessen E, Kjelstrup S |