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Appl Environ Microbiol, March 1998, p. 1040-1044, Vol. 64, No. 3
0099-2240/98/$04.00+0
Copyright © 1998, American Society for Microbiology. All rights reserved.
A Fermentor System for Regulating Oxygen at Low Concentrations
in Cultures of Saccharomyces cerevisiae
Patricia V.
Burke,
Kurt E.
Kwast,
Frank
Everts,§ and
Robert O.
Poyton*
Department of Molecular, Cellular, and
Developmental Biology, University of Colorado, Boulder, Colorado
80309-0347
Received 30 July 1997/Accepted 22 October 1997
 |
ABSTRACT |
The growth of yeast cells to high densities at low, but constant,
oxygen concentrations is difficult because the cells themselves respire
oxygen; hence, as cell mass increases, so does oxygen consumption. To
circumvent this problem, we have designed a system consisting of a
computer-controlled gas flow train that adjusts oxygen
concentration in the gas flow to match cellular demand. It does
this by using a proportional-integral-differential algorithm in
conjunction with a three-way valve to mix two gases, adjusting their
proportions to maintain the desired oxygen concentration. By modeling
yeast cell yields at intermediate to low oxygen concentrations, we have
found that cellular respiration declines with oxygen concentration, most likely because of a decrease in the expression of genes for respiratory proteins. These lowered rates of oxygen consumption, together with the gas flow system described here, allow the growth of
yeast cells to high densities at low oxygen concentrations. This system
can also be used to grow cells at any desired oxygen concentration and
for regulated shifts between oxygen concentrations.
 |
INTRODUCTION |
Oxygen is an important environmental
signal for most organisms (2). It determines whether energy
generation occurs primarily through oxidative phosphorylation or
glycolysis. The former is more efficient but also generates reactive
oxygen species, which can damage cells. Consequently, cells require
enzymes for the appropriate mode of energy metabolism and for
protection from reactive oxygen species. In the yeast
Saccharomyces cerevisiae, the expression of a large number
of proteins is affected by oxygen tension (15). Most of
these proteins function in respiration, in other processes that use
oxygen (e.g., the synthesis of sterols, heme, or unsaturated fatty
acids), or in the oxidative stress response. Some of these proteins are
expressed optimally in air, some are expressed optimally under
anaerobic conditions, and some are expressed optimally at intermediate
microaerophilic oxygen tensions (2, 12, 15). The effects of
oxygen on the expression of many of these proteins are exerted through
transcription of their genes. Those genes that are expressed optimally
in air have been designated aerobic genes; those genes that are
expressed optimally under microaerophilic or anaerobic conditions have
been designated hypoxic genes.
Most genetic studies of oxygen-regulated gene expression in yeast have
been done with cells grown either aerobically or anaerobically, or with
mutant strains deficient in heme biosynthesis. These studies have
implicated heme and a few transcription factors in the expression of
aerobic and hypoxic genes but have not revealed how yeast cells actually sense oxygen. Recently, we began to address this question by
examining the effects of oxygen concentration on the expression of
several genes that encode proteins of the terminal portion of the
respiratory chain (3). In these studies, oxygen
concentration was varied by sparging fermentor cultures with gases of
different fixed oxygen concentrations. Cells were grown until oxygen
demand exceeded supply, as indicated by a decrease in the
dissolved-oxygen (DO) concentration in the culture. They were then
harvested for RNA isolation and assessment of gene expression by
Northern blot analysis. The dose-response curves obtained from these
studies revealed that expression of these genes switches on or off at very low oxygen thresholds (0.5 or 1 µM O2). Although the
fermentor system used for these studies performed adequately, cell
yields from cultures grown at or near these oxygen thresholds
were very low (3). Unfortunately, these low yields preempted
biochemical studies aimed at elucidating the molecular basis for either
oxygen sensing or oxygen thresholds in these cells.
Biochemical studies generally require substantial amounts of cellular
material. Because of this, very little biochemistry has been done with
yeast cells grown at the low oxygen concentrations (i.e., 0.5 to 1 µM
O2) that serve as thresholds for the above-mentioned genes.
Indeed, such studies would require the growth of yeast cells to high
density at low, but constant, limiting oxygen tensions. This is
difficult because cells themselves consume oxygen; hence, as cell mass
increases, so does oxygen consumption. The system described here was
designed to circumvent this problem. It is a computer-controlled
feedback system for gas flow that allows oxygen concentration in the
gas entering the fermentor to increase with cellular demand. It does
this by mixing two gases, adjusting their proportions to maintain a
desired fixed oxygen concentration.
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MATERIALS AND METHODS |
Strains and media.
Yeast strain JM43 (MAT
leu2-3,112 his4-580 trp1-289 ura3-52) (6) was used for
all of the studies described here. Cells were grown in a semisynthetic
medium, SSG (containing, per liter, 3 g of Bacto yeast extract, 10 g of galactose, 0.8 g of NH4SO4, 1 g
of KH2PO4, 0.5 g of NaCl, 0.7 g of
MgSO4 · 7H2O, 5 µg of
FeCl2, and 0.4 g of CaCl2), supplemented
with amino acids and uracil at 40 µg/ml, 0.1% (vol/vol) Tween 80, 20 µg of ergosterol per ml, and 350 ppm of Dow Corning FG-10 Silicone
antifoam.
Growth conditions.
Precultures were grown aerobically in a
shaker (200 rpm) at 28°C to mid-logarithmic phase. The resulting
cultures were inoculated into a New Brunswick BioFloIIc fermentor, with
a working volume of 3.5 liters, and grown to early or mid-log phase
before harvesting. Temperature, pH, and agitation were maintained at
28°C, 5.0, and 300 rpm, respectively. Oxygen concentration in the
fermentor was either regulated or unregulated. In the latter case,
gases of fixed oxygen concentration were used and cultures were
harvested when the oxygen tension dropped below 80% of the initial
value. When oxygen concentration was regulated, oxygen was monitored with an oxygen sensor as described below. For both types of
experiments, cultures were inoculated with enough cells to allow 5 to 7 doublings in cell mass before harvesting. At the time of harvest, cells were quick-chilled through several feet of coiled copper tubing immersed in a salted ice bath, collected by centrifugation, and washed.
Measurement and control of DO.
A block diagram of the gas
flow train and control system is shown in Fig.
1. Either nitrogen or a process gas (gas
1) enters the flow train on the left while air or a second process gas
(gas 2) enters on the right. Gas flow in both the right and left arms is set with Cole Palmer 150-mm rotameters (model no. L-03294-26), selected by a solenoid control valve, and monitored with a mass flow
meter. Two in-line filters (2 and 0.2 µm) protect the mass flow meter
and ensure sterility in the fermentor vessel. To reduce time delays,
which can cause stability problems with regulation by the
proportional-integral-differential (PID) algorithm, the length of
tubing between the fermentor vessel and the solenoid valve was made as
short as possible. The gases used for the experiments described here
are oxygen-free nitrogen (Matheson), which contains less than 0.5 ppm
of oxygen; filtered house air; and process gases, which are mixtures of
Certified Standard gases made up in oxygen-free nitrogen. The process
gases are attached to the gas flow train through two semiautomatic
changeover manifolds (model no. 5201; Matheson).

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FIG. 1.
Gas flow train and control system. A solenoid control
valve allows either gas 1 or gas 2 to enter the fermentor, where oxygen
tension is monitored with a polarographic DO sensor; the signal is
amplified at the transmitter and sent to a microcomputer with a DAP.
The solenoid valve is under computer control and may be programmed for
a constant duty cycle, to maintain a particular oxygen concentration,
or to shift oxygen concentrations. Gas 1 is usually either the
low-oxygen gas or nitrogen, while gas 2 is usually either the
high-oxygen gas or air. Gas flow is adjusted with the rotameters and
monitored by the mass flow meter. Atm, atmosphere.
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|
Oxygen-free nitrogen and air are used to calibrate the DO sensor (12 mm; Ingold, Wilmington, Mass.). For anaerobic experiments, nitrogen is
passed through an Oxyclear oxygen absorber (LabClear, Oakland, Calif.)
in order to reduce its residual oxygen level to below 50 ppb. At the
end of each experiment, the zero calibration of the DO sensor is
checked with a chemical zeroing gel (Ingold).
Oxygen concentration in the fermentor is monitored with the DO sensor.
The signal from this electrode is amplified with an Ingold 4300 transmitter, and a scaled, 4- to 20-mA signal is sent to the MicroStar
Data Acquisition Processor (DAP) model 1200/2. Analog data from the
mass flow meter (type 0258C 0 to 5 V; MSK) and the BioFloIIc
fermentor (0 to 1 V) are also sent to the DAP, where they are
digitized, averaged where appropriate, and sent on to a microcomputer
(model 333P; Dell) for display and logging to disk. The DAP contains an
80186 microprocessor with firmware for data processing and control,
including the PID algorithm, and digital output lines that are used to
control the solenoid control valve (model no. 8320B174Q; ASCO). The
solenoid control valve operates at 120 V and is optically isolated from
its 0 to 5 V control signal with an SSR OPTO22 120D25 relay. It is
switched to gas 1 or gas 2, depending on the signal from the DAP. When oxygen concentration is regulated, the valve is switched to gas 1 for
some fraction (0 to 100%) of the 1-s duty cycle and to gas 2 for the
remainder of the 1-s duty cycle. The DAP is controlled by scripts
(instruction sets) sent to it by the microcomputer. Source code is
available upon request.
The oxygen concentration (in µM) in the fermentor vessel was
calculated from the measured DO level and based on oxygen solubility in
the growth medium at 28°C, the ambient barometric pressure, and the
pressure in the fermentor vessel (i.e., differential pressure) by using
the following formula: O2 = [(bi
bo)/(bs
bo) × f] × cO2. The value bi is the
measured output (in bits) from the dissolved oxygen sensor at time i,
bo is the measured output in the absence of oxygen,
bs is the measured output in air-saturated growth medium, f
is the amplification factor (0 to 1) of the oxygen meter, and
cO2 is the concentration of
O2 (in µM) in air-saturated medium at the measured
pressure (i.e., ambient plus differential pressure). The osmotic
pressure of the supplemented SSG growth medium used here was 184 mosM.
The differential pressure in the fermentor vessel at the 4-liters/min
sparge rate used for these experiments was extremely low (less than
0.4% of an atmosphere) and therefore had little effect on the value of
cO2. The value for bo
was obtained for each experiment by equilibration of the oxygen sensor
in either O2-free nitrogen or zeroing gel. The lowest value
obtained from these treatments was used in all cases. The value for DO
concentration in air-saturated growth medium in our laboratory in
Boulder, Colo., was typically between 195 and 197 µM.
RNA isolation and hybridization.
Total RNA was isolated from
washed cells essentially as described (7). RNA samples were
separated on 0.22 M formaldehyde-agarose gels in a
morpholinepropanesulfonic acid (MOPS)-formaldehyde buffer (0.02 M MOPS,
0.04 M Na acetate, 0.008 M EDTA, 0.22 M formaldehyde) and transferred
to Nytran or Nytran Plus membranes (Schleicher and Schuell).
Approximately 30 µg of total RNA was loaded per lane; loading was
adjusted to give equal signals for hybridization to the ACT1
gene. DNA probes were prepared by random-primer labeling of
double-stranded DNA fragments with [
-32P]dCTP (Dupont
NEN). Probes were a 500-bp PstI fragment for
COX5a, a 370-bp AccI-BglII fragment
for COX5b, and a 520-bp StyI fragment for
ACT1. Hybridization and stringency washes were performed as described previously (13). Signal intensity was quantitated with an AMBIS radioanalytic imaging system. For quantitation of transcripts, signals were normalized to that for ACT1 mRNA.
Miscellaneous.
Statistical analysis, modeling, and data
plots were done with MATHCAD (MathSoft, Cambridge, Mass.). Cell density
was monitored by measuring turbidity with a Klett meter fitted with a
no. 54 green filter.
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RESULTS |
Computer control at intermediate and low oxygen tensions.
In
order to grow cells to high densities at low, but constant, oxygen
concentrations, we developed a computer-controlled gas flow system
(Fig. 1) that mixes two gases, adjusting their proportions to maintain
the desired oxygen concentration. This allows oxygen concentration in
the gas flow to increase with cellular demand (i.e., cell mass). With
this computer-controlled system, two process gases may be mixed to give
any desired oxygen concentration in the feed gas.
In the simplest case, program control of the solenoid valve (Fig. 1) is
set for a constant duty cycle, which may employ one process gas or the
other, or any combination of the two. As an example, we compared cell
growth obtained with a fixed duty cycle, mixing air and nitrogen to
give ~100 µM O2 in the saturated culture media, with
cell growth in which the duty cycle was regulated to maintain the
oxygen concentration at 100 µM. In the culture with a fixed duty
cycle, a decline in oxygen concentration was apparent at 6 h and
this concentration dropped to 80% of its initial value at 16 h,
at which time the experiment was terminated. In the culture with the
regulated duty cycle, the duty cycle began to change by 6 h to
accommodate increased cellular demand for oxygen. This culture was
terminated at the same time point (i.e., 16 h) as the unregulated
culture, so that mRNA levels could be compared. The cell growth rates
in both cultures were equivalent. Moreover, the cell yields at the time
of harvest in both cultures were comparable (Table
1). However, the regulated experiment could have continued for several more hours because the air fraction of
the process gas had only increased from 50 to 65% of the maximum for
the duty cycle at the time of harvest. Hence, the regulated culture
could have produced more cell mass.
We also compared the growth rates of regulated and unregulated cultures
at 1 µM O2, which is two orders of magnitude below the
oxygen concentration used for the experiment described above. For this
experiment, two different feed gas mixtures were used
one containing
0.1% oxygen, the other 1.0% oxygen
to keep the oxygen concentration
near 1 µM. In the unregulated culture, cells were maintained in
exponential growth until the oxygen concentration dropped to 80% of
its initial value, at which time they were harvested. The regulated
culture was grown for 16 h and then harvested. Although the
signal-to-noise ratio was higher at these lower oxygen concentrations, the gas flow train successfully maintained its initial oxygen concentration in the regulated culture to within 10% of its initial set point. As in the first experiment, the growth rates in both cultures were equivalent (Table 1), but, unlike in the first experiment, oxygen became limiting (i.e., declined to 80% of its initial concentration) at very low cell densities in the unregulated culture. This resulted in an extremely low cell yield (0.08 g [wet
weight] per liter) (Table 1). In contrast, the yield from the
regulated culture was significantly higher because this culture could
be grown for a longer period of time before oxygen concentration declined. In this experiment, cells were harvested at 16 h so that
mRNA levels could be compared to those in the experiment described
above. The cell yield was 1.4 g (wet weight) per liter, the same
yield obtained after 16 h in the regulated culture grown at 100 µM O2 (Table 1). Higher yields than this are possible because, as in the culture grown at 100 µM O2, the
fraction of the duty cycle for the higher-oxygen gas was still low
(i.e., in the range of 20 to 40%) at the time of cell harvest.
To illustrate the usefulness of the regulated system for growing cells
to high densities at low oxygen concentrations, we did the experiment
whose results are shown in Fig. 2. Here,
we used two feed gas mixtures (0.05 and 0.5% oxygen) to keep the oxygen concentration at 0.44 µM and allowed cells to grow to
stationary phase. The oxygen concentration was invariant for the first
5 h, after which the culture began to consume appreciable amounts of oxygen and the solenoid control valve began to regulate the oxygen
concentration. For the duration of the experiment, the oxygen
concentration was maintained at 0.44 ± 0.1 µM (mean ± standard deviation). The cell yield in this experiment was 7.04 g
(wet weight) per liter. It is nearly two orders of magnitude higher than yields that could be obtained in unregulated cultures grown at
this oxygen concentration.

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FIG. 2.
Cell growth at low oxygen concentration. Yeast cells
were grown in the fermentor at an oxygen concentration of 0.44 µM by
using feed gas mixtures of 0.05 and 0.5% oxygen. Cell growth was
monitored by taking 5-ml samples and assaying culture density
turbidometrically with a Klett colorimeter equipped with a green (no.
54) filter. The difference in turbidity between the culture and the
uninoculated growth medium is expressed as a difference in Klett units
( Klett) (upper trace) and is plotted on the left ordinate. The
concentration of oxygen in the culture medium (lower trace) is plotted
in 5-min-interval increments on the right ordinate. The oxygen
concentration in the culture throughout the entire experiment was
0.44 ± 0.1 µM (mean ± standard deviation). The cells were
harvested and weighed after cessation of growth.
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Modeling cell growth and oxygen consumption.
Cell yields can
be estimated from the oxygen balance equation:
|
(1)
|
where KLa is the gas-liquid mass transfer coefficient,
[O2]sat is the oxygen concentration supplied
by the feed gas, [O2] is the oxygen concentration in the
fermentor, Qm is the specific respiration rate,
and m(t) is the cell mass in grams at time
t. Under our experimental conditions, kLa is 40 h
1, Qm is 100 µM
h
1g
1 at moderate to high oxygen
concentrations (i.e., 100 to 200 µM O2 [air]) and 30 µM h
1g
1 at low oxygen concentrations
(i.e., 1 µM O2), and m(t) increases exponentially with doubling times of 2.6 to 3.0 h, depending on the experiment.
Under steady-state conditions, where oxygen concentration is constant,
we can calculate the maximal cell mass yield (in grams), mass yield as
a function of time, and the variation in the duty cycle necessary to
maintain a constant oxygen concentration from equation 1. Maximal cell
mass yield, Mmax, calculated from the limiting condition,
when the feed gas is entirely the second, higher-oxygen, gas, is given
by:
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(2)
|
where [gas 2] is the concentration of oxygen in the second,
higher-oxygen, gas. With one feed gas (i.e., unregulated conditions in
which oxygen tension decreases as cell mass increases), equation 1 becomes:
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(3)
|
where b is [ln(2)/mass doubling time] and t is time
(in hours). From equation 3 it is possible to calculate oxygen
concentration in the fermentor as a function of time.
When d[O2]/dt in equation 1 is set
equal to zero, the equation can be used to model cell growth and
respiration under steady-state conditions. In contrast, equation 3 can
be used to model cell growth and respiration under conditions where
oxygen tension decreases with time. Given the cell growth rate, cell
yield, and oxygen concentration in the fermentor, we have used these
equations to calculate the specific respiration rate as 100 µM
O2/h/g for cultures grown in 100 or 200 µM O2
and as 30 µM O2/h/g for cultures grown at 1 µM
O2. This reduction in specific respiration rate at reduced oxygen concentrations has been observed previously (8a, 10) and is significant because it leads to a lack of proportionality between cell yield and oxygen concentration; this, in turn, leads to an
increase in cell yield in low-oxygen cultures. By using the appropriate
specific respiration rate (above), the cell yields from regulated
cultures can be calculated to be considerably higher than the cell
yields from unregulated cultures. For example, if growth were allowed
to continue until the feed gas is entirely the high-oxygen gas, cell
yields from regulated cultures would be 7- and 30-fold higher than from
unregulated cultures grown in 100 µM and 1 µM O2,
respectively.
Gene expression with the regulated system.
The utility of this
fermentor system for studies of oxygen-regulated gene expression is
illustrated by the experiment whose results are shown in Fig.
3. Here, the effects of oxygen
concentration on the expression of ACT1, COX5a,
and COX5b are shown. ACT1 encodes actin,
COX5a encodes the aerobic isoform (Va) of cytochrome
c oxidase subunit V, and COX5b encodes the
hypoxic isoform (Vb) of cytochrome c oxidase subunit V. The
ACT1 gene, whose expression is not oxygen sensitive, was
used as a control. COX5a is optimally expressed in air (200 µM O2), while COX5b is optimally expressed under anaerobic conditions. The results shown in Fig. 3 allow us to
determine the oxygen thresholds for expression of these two genes. The
mRNA level from COX5a declines precipitously at oxygen
concentrations of 0.5 µM or below. This agrees with the 0.5 µM
O2 threshold we determined previously for unregulated
cultures (3). In contrast, the mRNA level from
COX5b increases at oxygen concentrations of 0.2 µM or
below, indicating that the threshold for switching on this gene is
between 0.5 and 0.2 µM O2. Previous attempts to define
this threshold in unregulated cultures have been unsuccessful
(3) because of low cell yields. The high cell yields
produced in the regulated cultures now make possible studies aimed at
determining the biochemical bases for these low oxygen thresholds for
gene expression.

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FIG. 3.
Effects of oxygen on the expression of COX5a
and COX5b. Northern blot of total RNA isolated from cells
grown in 200 µM O2 (air) (lane 1), 50 µM O2
(lane 2), 5 µM O2 (lane 3), 0.5 µM O2 (lane
4), 0.2 µM O2 (lane 5), and oxygen-free N2
(lane 6). The RNA was hybridized with probes specific for
COX5a, COX5b, and ACT1, as described
in Materials and Methods. The ACT1 gene was probed as a
control for RNA load. The levels of COX5a and
COX5b mRNAs, normalized to the ACT1 mRNA, are
presented as decimal percentages relative to their levels in air (for
COX5a) or nitrogen (for COX5b).
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System stability and regulation.
A PID-algorithm-regulated
system may be hard to tune for stability in the face of rapid shifts or
transients and tight regulation at set points. Because tightly
regulated systems may not be stable to large transients, we have
designed the control program to approach the desired oxygen tension by
operating at the theoretical duty cycle for that oxygen tension until
one of two criteria is met: either the error signal becomes less than a
specified value, or the time allowed to reach the set point is
exceeded. Once one of the above criteria is met, the program changes
from the programmed, theoretical duty cycle to PID control of the duty
cycle. This is a modified type of PID control inasmuch as the error
signal increases or decreases the duty cycle of the solenoid valve,
which will change the proportion of oxygen in the gas flow.
Figure 4A shows the response of the
system to transient introduction of a gas of higher oxygen
concentration. The system was equilibrated with 0.1% oxygen, and
regulation was started with the second gas (1% oxygen) fully on.
Within 5 min, the DAP script for PID control reversed the rise in
oxygen tension, and within 10 min it returned it to the control value.
Figure 4B shows oscillations at low oxygen concentration when the set
point is just above the actual oxygen concentration for gas 1 (Fig. 1);
this oscillation is reduced after the culture begins to consume oxygen.
Such oscillations are common with simple PID control (4,
14); further adjustment of the three parameters for low oxygen
concentrations might improve the regulation. Alternatively, a predictor
model (14) or a feed-forward model (11) could be
used at low oxygen concentrations.

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FIG. 4.
System responses. (A) Response time of the modified PID
controller. The system was equilibrated with gas 1 prior to initiation
of computer control; regulation was started with gas 2 fully on. (B)
Oscillations in oxygen tension when the set point is just above the
actual oxygen concentration for gas 1. Initially, there is little
oxygen consumption because the density of the cell culture is low.
Later, as the culture begins to consume more oxygen, the size of the
oscillation in oxygen concentration is reduced.
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Other uses.
This is a versatile system that was set up
initially for use at intermediate and low oxygen concentrations. It has
also been used to grow cells in atmospheric and even hyperbaric oxygen
(data not shown). In addition, it has been used to shift cells from one
oxygen concentration to another. The shift in oxygen concentration within the fermentor is typically 95% complete within 4 min; this allows changes in gene expression to be monitored after a rapid shift
in conditions.
 |
DISCUSSION |
Several strategies have been used to control DO concentration in
fermentor cultures of various microbes (4, 5, 8, 10, 11,
14). These vary in the type of control algorithm used and in the
parameters that are regulated. The easiest parameters to regulate are
agitation within the fermentor vessel and total gas flow into the
vessel. Consequently, the most commonly used controllers have relied on
varying the agitation rate or on varying both the agitation rate and
the rate of inlet gas flow. Both strategies regulate oxygen
concentration by altering the agitation or sparge rate, both of which
modify the gas-liquid mass transfer coefficient, kLa.
Alterations in the agitation or sparge rate concomitantly alter the
fluid flow and shear characteristics within the fermentor (9). Because DO probes may be sensitive to shear,
alterations in shear can exacerbate measurement problems at the low
oxygen levels that approach the limits of probe sensitivity. The
regulation of agitation and/or sparge rate is therefore not useful for
studies aimed at growing cells at very low oxygen concentrations. In
addition, yeast cells grown at low oxygen concentrations require added
unsaturated fatty acids (usually supplied as Tween 80) and ergosterol
(1). These supplements increase foaming in the medium, which
can be very difficult to suppress when the agitation or sparge rate
increases.
Our solution to the problem of growing yeast cells at low but constant
oxygen concentrations is to mix two gases at constant agitation and gas
flow levels. Because the DO probe may be sensitive to changes in fluid
flow, especially at the limits of probe sensitivity, we chose to
maintain constant agitation and gas flow. This minimizes variations in
gas-liquid transfer rates, foaming, and oxygen probe sensitivity
problems. The proportion of the two gases is adjusted to maintain
oxygen tension near the set point by using a PID-control algorithm.
Although this strategy is similar to that used by Chen et al.
(4), our system regulates at lower oxygen tensions and permits higher cell yields. Our system also allows one to start a
fermentation with a constant gas mixture before switching to PID
control; this avoids instabilities that are characteristic of many PID
systems responding to large changes in set point (4). Regulation with this system is good at intermediate oxygen
concentrations and satisfactory at low oxygen concentrations. Tighter
regulation at low oxygen concentrations might be achieved by using a
feed-forward algorithm similar to that used by Smith et al.
(11).
This regulated system for growing yeast cells has been used reliably to
grow cells at oxygen concentrations between 0.2 and 200 µM. Gene
expression in the oxygen-regulated cultures is comparable to that for
unregulated cultures. However, the regulated system supports higher
cell yields at very low oxygen tensions. Indeed, it increases cell
yield nearly two orders of magnitude, at oxygen concentrations below 1 µM, relative to those levels achievable in an unregulated system. The
gas flow system described here is also useful for programmed shifts
between different oxygen concentrations and is sufficiently versatile
to allow a wide range of gas mixtures to be used, in conjunction with
appropriate probes.
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ACKNOWLEDGMENTS |
This work was supported by GM 30228 (R.O.P.) from the National
Institutes of Health and grant 4557 from the Tobacco Research Council.
 |
FOOTNOTES |
*
Corresponding author. Mailing address: Department of
Molecular, Cellular, and Developmental Biology, University of Colorado, Campus Box 347, Boulder, CO 80309-0347. Phone: (303) 492-3823. Fax:
(303) 492-7744. E-mail: poyton{at}spot.Colorado.EDU.
Present address: Department of Physics, Whitman College, Walla
Walla, WA 99362.
Present address: Department of Molecular and Integrative
Physiology, University of Illinois at Urbana-Champaign, Urbana, IL 61801.
§
Present address: Lucent Technologies, Denver, CO.
 |
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Appl Environ Microbiol, March 1998, p. 1040-1044, Vol. 64, No. 3
0099-2240/98/$04.00+0
Copyright © 1998, American Society for Microbiology. All rights reserved.
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