| 4039 - 4040 |
The vanishing chemical engineer?
Van Swaaij W |
| 4041 - 4053 |
Large eddy simulations of the turbulent flow in a stirred reactor
Revstedt J, Fuchs L, Tragardh C |
| 4055 - 4072 |
Velocity control of hyperbolic partial differential equation systems with single characteristic variable
Gundepudi PK, Friedly JC |
| 4073 - 4084 |
Effect of NaOH concentration on a sequential phosphazene reaction by phase-transfer catalysis
Wu HS, Meng SS |
| 4085 - 4094 |
On the scale-up of external loop airlift reactors: Newtonian systems
Al-Masry WA, Abasaeed AE |
| 4095 - 4104 |
New fractionation process for citrus oil by pressure swing adsorption in supercritical carbon dioxide
Sato M, Goto M, Kodama A, Hirose T |
| 4105 - 4112 |
The effect of precursor in flame synthesis of SiO2
Briesen H, Fuhrmann A, Pratsinis SE |
| 4113 - 4127 |
Air entrapment and air bubble dispersion at two-dimensional plunging water jets
Brattberg T, Chanson H |
| 4129 - 4133 |
Hydrodynamic meniscus profiles in creeping flow
Sciffer SD, Evans GM, Lucas JA |
| 4135 - 4146 |
On the use of different parabolic concentration profiles for nonlinear adsorption and diffusion in a single particle
Botte GG, Zhang RY, Ritter JA |
| 4147 - 4149 |
Axial dispersion in rich, binary gas mixtures: model form and boundary conditions
Choong TSY, Paterson WR, Scott DM |
| 4151 - 4154 |
A reassesment of relationship between riser and downcomer gas holdups in airlift reactors
Contreras A, Chisti Y, Molina E |
| 4155 - 4158 |
Modification of Kozeny-Carman concept for calculating pressure drop in flow of viscoplastic fluids through fixed beds
Dolejs V, Siska B, Dolecek P |
