Call number: LD2668 .T4 1960 C37

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There is a considerable volume of work available in literature which suggests that the performance of axial-flow hollow fibre membrane modules is limited by poorly distributed flow through the shell-side. This study was commissioned to examine the distribution of shell-side flow and its effect on mass transfer and to compare the performance measured by the axial-flow configuration to that obtained by a commonly used alternative known as the helically-wound module design. Laminar flow and mass transfer models have been developed to examine performance through axial-flow hollow fibre modules. These models also consider deviations from laminar flow in the form of turbulence and hydrodynamically undeveloped flow. Modelling analysis on four fibre bundle cross-sections quantify the extent to which channelling limits flow and mass transfer performance. Experimental flow and mass transfer work with locally fabricated hollow fibre modules demonstrated some inconsistencies with axial laminar flow modelling. Pressure drop and mass transfer results exceeded predictions from modelling. This thesis has hypothesised that fibres in axial-flow hollow fibre modules are not aligned as straight and parallel rods (as assumed in modelling) but interweave. Fibre interweaving results in flows between ducts. Such flows create mixing between ducts which results in more intimate contact between the flow and membrane surface, the consequence being higher pressure drop and higher mass transfer. The implication from this work was that axial flow and mass transfer modelling was limited in its use for characterisation of shell-side performance. The experience with helically-wound hollow fibre membrane modules (also fabricated locally) was that, by deliberately inducing flow between ducts, it was possible to considerably improve mass transfer performance. It was found that, whilst helically-wound modules could not be packed as tightly as axial-flow modules and required more sophisticated fabrication techniques, the benefit in their use arose from a substantial improvement in the level of shell-side mass transfer.

The effect of unsteady thermocapillary convection on the mass transfer rate of a solute between two immiscible liquids within a rectangular microscale channel with differentially heated sidewalls was numerically investigated. A computational fluid dynamic code in Fortran77 was developed using the finite volume method with Marker and Cell (MAC) technique to solve the governing equations. The discrete surface tracking technique was used to capture the location of the moving liquid-liquid interface. The code produced results consistent with those reported in published literature. The effect of the temperature gradients, the aspect ratio, the viscosity of liquid, and the deformation of the interface on the mass transfer rate of a solute were studied. The mass transfer rate increases with increasing temperature gradient. The improvement of the mass transfer rate by the thermocapillary convection was found to be a function of the Peclet number (Pe). At small Pe, the improvement of the mass transfer rate increases with increasing Pe. At high Pe, increasing the Pe has no significant effect on increasing the mass transfer rate. Increasing the aspect ratio of the cavity up to 1 increases the mass transfer rate. When the aspect ratio is higher than 1, the vortex moves only near the interface, resulting in decreasing the mass transfer rate. By increasing the viscosity of the liquid in top phase, the maximum tangential velocity at the interface decreases. As a result, the improvement of the mass transfer rate decreases. The deformation of the interface has no significant effect on the improvement of the mass transfer rate. By placing the heating source at the middle of the cavity, two steady vortices can be induced in a cavity. As a result, the mass transfer rate is slightly enhanced than that in the system with one vortex. By reversing the direction of the temperature gradient, the mass transfer rate decreases due to the decrease in the velocity of bulk fluid. The thermocapillary convection also promotes the overall reaction process when the top wall of the cavity is served as a catalyst. / Graduation date: 2005

Polycyclic aromatic hydrocarbons (PAH) have been identified as a serious environmental problem. In past research it has been proven that naphthalene, the simplest PAH, could be biodegraded using roller bioreactors and Pseudomonas putida. In this previous work it became apparent that the mass transfer rate of the hydrophobic naphthalene was the rate limiting factor in biodegradation, as the bacteria could degrade the naphthalene as fast as it entered solution. The challenge for the present research was to find a simple, inexpensive method for increasing the mass transfer rates within the framework of the previously successful reactor. <p>After some deliberation, the addition of inert particles (glass beads) was determined to be the preferred option to increase mass transfer. The inert particles visibly increased the turbulence in the reactor and significant increases in both mass transfer and bioremediation rates were achieved. The augmentation of mass transfer rates was found to be dependent on the type, size and relative loading of the particles. Two types of inert particles were investigated to increase mass transfer rates, spherical glass beads and Raschig rings. Glass beads were found to be far superior to Raschig rings for the intended purpose. Three sizes of spherical glass beads were then compared experimentally (1, 3, and 5mm). It was discovered that the 3mm beads were vastly superior to 1mm beads and 5 mm beads were slightly superior to 3mm beads. Different bead loadings (volume of particles / total working volume) were then explored with 10%, 25% and 50% bead loading investigated. Although slight increases in mass transfer were observed at higher bead loadings, the reduction in working volume for biodegradation meant that 50% was accepted as the optimum loading parameter. <p>The optimum conditions for maximum mass transfer occurred using 5 mm spherical glass beads at 50% loading. The increase in mass transfer and biodegradation rates compared to a traditional roller bioreactor were found to be 10 fold and 11 fold, respectively. The optimum mass transfer conditions were then applied to 2-methylnaphthalene with increases in mass transfer and biodegradation equal to 6 fold and 8 fold, respectively. The candidate bacteria used in this study was found incapable of degrading 1,5 dimethylnaphthalene although the mass transfer results demonstrate promise for the developed technology. To determine the effects of scale on the process, two larger reactors were finally studied. They were eight times and twenty-one times the size of the initial bioreactor. The process was shown to speed up at larger scale which shows great promise for future applications. The maximum degradation rate achieved in the larger reactor was 148 mgL-1h-1. This compares very well with the best result found in literature, 119 mgL-1h-1, which was achieved in a much more complex system. Clearly, the bead mill bioreactor designed during the present work is a simple concept that shows superior performance for the bioremediation of PAHs.