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43.3. Plasmid hstabiiity Kinetics in Conb'nuous Culture<br />

4.3.3.1. Mathematid Analysis<br />

Assummg that the ceils are m balanced growth, according to Imanaka and Aiba (1981).<br />

the change in plasmid-bearing ce& in the continuous culture system can be descnbed <strong>by</strong>:<br />

The anaiyticai solution <strong>of</strong> Eq. (4.1) is as follows:<br />

..Y+ = x,' exp(p+ - pp* - D)t = x0+ exp(-kft) (43)<br />

where k = -( p' - pp* - D) . a m-order decay rate constant, which is aiways positive<br />

because p* S D. Eq. (4.2) shows that the decay <strong>of</strong> phmici-bearing c& foiiows fmt-<br />

order kinetics and the concentration <strong>of</strong> plamid-bearing cells decreases with culture time<br />

during continuous culture. Since the total cefl concentration X, is observed constant<br />

during the culture process (See Figwe 4.17). the fiaction <strong>of</strong> plasmid-besring cells<br />

( F = X+ / X, ) &O foîiows an exponential decay pattern:<br />

F = F, exp(-k!t) (4.3)<br />

Similarly. the change in plasruid-ke œUs in the culture system can be descnbed as<br />

follows:<br />

Eq. (4.2) and (4.4) can be solved analytically to give:<br />

X- = X,- expC(p- - D )~J + [pp+~o' G][exp[((p- - Dut - eq(-k,t)] (43

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