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understanding <strong>of</strong> the nature <strong>of</strong> the immobiüÿed recombinant yeast through experiments<br />

and modelling.<br />

6.2. Continuous Culture in XmmobiIizeà-Ceil Bioreactor<br />

62.1. Modd Development<br />

An idealised modei is w d<br />

to characten.ize the Unmobiliwl cell system as jiiustrated in<br />

Figure 6.1. As shown in Figure 6.1, the i-d bi<strong>of</strong>ilm has a unifonn density <strong>of</strong> œUs<br />

attached to the support and a locally d o m thickness with negiigible interna1 and<br />

extemal mas W e r mistance. 'Ihese assurnptions may be justified for the present<br />

immobïiized-ceU-film airM <strong>bioreactor</strong> because <strong>of</strong> the thin bi<strong>of</strong>ilm (les than 2.0 mm ) and<br />

suong hydmdynamic Nculation and mixing in the <strong>bioreactor</strong>. It is ako assumed that no<br />

growth merence between the plasrnid-bea~g and plasmid-frez cells ex&&, which was<br />

confimied for the present ncombinant yeast in previous <strong>studies</strong>. Under these<br />

assumptions, an identicai specific growth rate for both the bi<strong>of</strong>ïim and suspended plasmid-<br />

bearing and plamid-Eree ceh in the immobilized-ceiî-fîim biore-r may be justified. The<br />

specific growth rate <strong>of</strong> the immobilized ceil system at a fïxed dilution rate is denoted as<br />

in the immobïiized-cetl-fi airlift <strong>bioreactor</strong>, ceils grow on the cloth film and are<br />

continuously detached into the medium due to hydrodynamic forces. It is unlüUely that<br />

additional free space wiU be avaiiable for re-entiy <strong>of</strong> the released œk onto the Wy-<br />

covend cloth surface again (Ghose, 1988). huming a constant vaiue <strong>of</strong> plasmid los

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