Light intensity distribution in multi-lamp photocatalytic reactors
dc.contributor.author | Boyjoo, Yash | |
dc.contributor.author | Ang, Ha Ming | |
dc.contributor.author | Pareek, Vishnu | |
dc.date.accessioned | 2017-01-30T10:43:34Z | |
dc.date.available | 2017-01-30T10:43:34Z | |
dc.date.created | 2013-09-23T20:01:15Z | |
dc.date.issued | 2013 | |
dc.identifier.citation | Boyjoo, Yash and Ang, Ha Ming and Pareek, Vishnu. 2013. Light intensity distribution in multi-lamp photocatalytic reactors. Chemical Engineering Science. 93: pp. 11-21. | |
dc.identifier.uri | http://hdl.handle.net/20.500.11937/5048 | |
dc.identifier.doi | 10.1016/j.ces.2012.12.045 | |
dc.description.abstract |
A computational fluid dynamics approach has been used to investigate the effect of lamp separation (Xlamp) on the radiation intensity distribution in a multiple-lamp photocatalytic reactor. The optical parameters (absorption and scattering coefficients) of Aeroxide® P25 titanium dioxide (TiO2) were determined by performing experiments using a single lamp system. Since the optical properties are wavelength dependent, the range of wavelength from the UV lamp was divided into 4 bands, and optical properties in each of the bands were determined by matching the experimental observations with simulated values. Simulations were then carried on multiple-lamp (2 and 4 lamps) photoreactors as a function of lamp separation and catalyst loadings. In case of 2-lamp system, the maximum local volumetric rate of energy absorption (<LVREA>) occurred at Xlamp=40mm, and it was independent of the catalyst loading. With 4 lamps however, optimum Xlamp was dependent on the catalyst loading. At low loads (up to Wcat=0.06gL-1), the optimum Xlamp was 80mm but as the catalyst concentration increased, the value of the optimum lamp separation decreased considerably, with 30mm for Wcat=0.07gL-1 and decreasing further as the concentration further increased. Because of the high absorption coefficient of the catalyst, the wall emissivity had a negligible effect on the <LVREA> for both configurations, even when the lamps were close to the wall. Finally, in both cases, the optimum lamp separation was independent of the lamp emissive power. | |
dc.publisher | Pergamon | |
dc.subject | Photochemistry | |
dc.subject | Computation | |
dc.subject | Reaction engineering | |
dc.subject | Photoreactor | |
dc.subject | Light intensity distribution | |
dc.subject | Mathematical modelling | |
dc.title | Light intensity distribution in multi-lamp photocatalytic reactors | |
dc.type | Journal Article | |
dcterms.source.volume | 93 | |
dcterms.source.startPage | 11 | |
dcterms.source.endPage | 21 | |
dcterms.source.issn | 0009-2509 | |
dcterms.source.title | Chemical Engineering Science | |
curtin.department | ||
curtin.accessStatus | Fulltext not available |