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celi fraction decreases monotonicaiiy with generation number (n) according to the<br />

foilowing equation:<br />

where a = pCc/p+. From Eq. (23) it is obvious that in batch systern with any a > 1.0 and p<br />

> O, H, = O. The Imanaka and Aiaa (1981) model is mtructnred, but elegantly simple.<br />

in principle, any recombinant organisrn satisfying the underlying assmnptions shouid<br />

confonn to the model. Unfortunately, the p and a usuaiiy Vary du~g the culture penod,<br />

and the assumed exponential growth is not exactly followed.<br />

Pioneering deveiopments in stmctured modehg <strong>of</strong> mDred combinant culture<br />

came h m Bailey's and Shuier's groups working with recombinant E. coli (Lee and<br />

BaiIey, 1984; Seo and Baüey, 1985; Ataai and Shuler, 1986; Kim and Shuler, 1990a; Kim<br />

and Shuler. 1990b). The plasmid stability and the expression <strong>of</strong> a cloned-gene product has<br />

ken descnbed <strong>by</strong> a mathematid mode1 based upon the molecular mechanisn <strong>of</strong> plasmid<br />

replication, partition and transcription. These <strong>studies</strong> laid the fondation for mer<br />

mathematicai modehg and pointed the way for futm experimental work. Later, at a<br />

singieîeIl level, using population balance models, Hjortso and Bailey mathematicaily<br />

descnbed the plasmid stability in yeast S. cerevisiae with selection pressure (Hjortso and<br />

Bailey, 1984a) and without selection pressure (Hjortso and Bailey, 1984b). Two<br />

assumptions were examined for plasmid partitioning: (i) random and independent<br />

distribution <strong>of</strong> plasmids between the mother and the daughter tells at partition; and (ii) a<br />

greaar or eqrial probability <strong>of</strong> a plasmid residing in the mother ceii after division than in

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