Biomedical Engineering Reference
In-Depth Information
Exhaust gas
Mixer
Motor
Feed
Compartment 1
V 1
Compartment 2
V 2
Gas
Supply
Valve
Product
Pump
Separator
FIGURE 18.13 Schematic of compartment formation in a chemostat.
d
S 1
d
YF X = S m max S 1
1
t ¼ k LS aðS 2 S 1 Þþð1þa 1 ÞDðS 0 S 1 Þ
K S þS 1 X 1
(18.61)
where
a 1 is the volumetric ratio of the lower compartment to the top compartment, the volu-
metric mass transfer coefficients (k LX a and k LS a) are based on the top compartment and the
dilution rate (D) is based on the total reactor volume. In strongly mixed flow reactors
(high Reynolds number), the mass transfer coefficients are nearly the same for all species
(as molecular diffusion is negligible compared to flow-induced diffusion or dispersion),
either be (fine) solid particles (like microbes) or soluble molecules (like sugar substrates).
Mass balances in the lower compartment with Monod growth model lead to
m max S 2
K S þS 2 k d
d
X 2
d
t ¼ k LX a
a 1 ðX 1 X 2 Þþ
X 2
(18.62)
d
S 2
d
t ¼ k LS a
YF X = S m max S 2
1
a 1 ðS 1 S 2 Þ
K S þS 2 X 2
(18.63)
For steady-state operations, none of the concentrations would be changing with time.
Therefore, Eqns (18.60) through (18.63) are reduced to a set of algebraic equations as usual
for the continuous cultures.
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