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Emission of microorganisms from biofilters
Authors:S P P Ottengraf  J H G Konings
Institution:(1) University of Technology, Eindhoven;(2) DSM Research, Geleen, The Netherlands
Abstract:Experiments are reported on the discharge of microbial germs by biofilter systems used for the treatment of waste gases containing volatile organic compounds. The systems investigated concern six full-scale filter installations located in the Netherlands in several branches of industry, as well as a laboratory-scale installation used for modelling the discharge process. It is concluded that the number of microbial germs (mainly bacteria and to a much smaller extent moulds) in the outlet gas of the different full scale biofilters varies between 103 and 104 m–3, a number which is only slightly higher than the number encountered in open air and of the same order of magnitude encountered in indoor air. It is furthermore concluded that the concentration of microorganisms of a highly contaminated inlet gas is considerably reduced by the filtration process. On the basis of the experiments performed in the laboratory-scale filter bed, it is shown that the effect of the gas velocity on the discharge process results from two distinctive mechanisms: capture and emission. A theoretical model is presented describing the rate processes of both mechanisms. The model presented and the experimentally determined data agree rather well.List of Symbols a s m–1 specific area of the packing material - C m–3 microbial gas phase concentration - C e , C i m–3 microbial concentration in the exit and inlet gas resp. - CFU colony-forming-units - d c , d m m diameter of collecting and captured particle resp. - D m diameter of the filter bed - E single particle target efficiency - H m bed height - k c s–1 first order capture rate constant per unit of bedvolume - k e m–3 emission rate constant per unit of bedvolume - n number of observations - r c , r e m–3 s–1 capture and emission rate per unit of bed-volume - Re = 
$$\frac{\varepsilon }{{(1 - \varepsilon )}}\frac{{\varrho  u{\text{ }}d_c }}{\mu }$$
Reynolds number - S t = 
$$\frac{{\varrho _m  u{\text{ }}dm^2 }}{{9\mu {\text{ }}d_c }}$$
Stokes number - u m s–1 superficial gas velocity - u m m s–1 superficial gas velocity at which C e = C i Greek Symbols epsiv void fraction of the filter bed - rhov kg m–3 density of the gas phase - rhov m kg m–3 density of captured particle - mgr Pa s dynamic gas phase viscosity - eegr = 
$$1 - \frac{{C_e }}{{C_i }}$$
filter bed efficiency
Keywords:
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