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Experimental Study of Biodegradation of Ethanol and Toluene Vapors

Experimental Study of Biodegradation of Ethanol and Toluene Vapors

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Because the feed media are sterile, C x0 = 0. When the system is at steady state<br />

(dC x /dt = 0), then:<br />

μ = D<br />

(5-61)<br />

In a continuous stirred tank bioreactor (CSTR), cells are removed at a rate equal<br />

to their growth rate, <strong>and</strong> the growth rate <strong>of</strong> cells is equal to the dilution rate during<br />

steady state operations. This phenomenon allows us to manipulate growth rate as an<br />

independent parameter. Since growth rate is limited by at least one substrate in the<br />

CSTR, a simple description <strong>of</strong> its performance can be made by substituting the Monod<br />

equation for µ in Equation (5-61):<br />

μ C<br />

m e<br />

μ D<br />

(5-62)<br />

=<br />

=<br />

K<br />

s<br />

+ C<br />

e<br />

If D is set at a value greater than μ , the culture cannot reproduce quickly enough to<br />

m<br />

maintain itself <strong>and</strong> is washed out. That is, when<br />

dX<br />

μ < D , = ( μ − D)<br />

Cx<br />

< 0 , then<br />

dt<br />

biomass would be washed out. Moreover, when the dissolved oxygen (DO) is higher<br />

than the critical value (DO><br />

C cr<br />

), the growth rate is independent <strong>of</strong> the DO value.<br />

When the DO is lower than<br />

C cr<br />

, the growth approaches a first-order rate dependence on<br />

the dissolved-oxygen concentration (Shuler <strong>and</strong> Kargi, 2002). The oxygen limitation<br />

results in μ < D , thus biomass will also be washed out, <strong>and</strong> the operation will no longer<br />

be steady state.<br />

Using Equation (5-62) at steady state, when other nutrients are in excess, the<br />

ethanol concentration can be described as a function <strong>of</strong> the dilution rate for<br />

D < μ <strong>and</strong><br />

m<br />

C<br />

O<br />

> C<br />

2 cr<br />

:<br />

130

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