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<small>VCH, P. 0. Box 101161, D-6940 Weinheim (Federal Republic of Germany) Switzerland: VCH, P. 0. Box, CH-4020 Base1 (Switzerland) </small>
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<small>ISBN 3-527-28314-5 (VCH, Weinheim) </small> <b><small>ISBN 1-56081-154-4 (VCH, New York) </small></b>
</div><span class="text_page_counter">Trang 3</span><div class="page_container" data-page="3"><small>This book was carefully produced. Nevertheless, authors, editors and publisher do not warrant the information con- tained therein to be free of errors. Readers are advised to keep in mind that statements, data, illustrations, procedural details or other items may inadvertently be inaccurate. </small>
<small>Published jointly by </small>
<small>VCH Verlagsgesellschaft mbH, Weinheim (Federal Republic of Germany) </small>
<b><small>VCH Publishers Inc., New York, NY (USA) </small></b>
<small>Editorial Director: Dr. Hans-Joachim Kraus Editorial Manager: Christa Maria Schultz Production Director: Maximilian Montkowski Production Manager: Peter J. Biel </small>
<small>Library of Congress Card No.: 91-16462 British Library Cataloguing-in-Publication Data: Biotechnology Second Edition </small>
<small>Biotechnology: Vol 4. Measuring, modelling and control. </small>
<small>Vol. Ed. Schiigerl, K. 620.8 </small>
<small>ISBN 3-527-28314-5 </small>
<small>Die Deutsche Bibliothek </small>
<b><small>Biotechnology </small></b><small>: a multi volume comprehensive treatise / ed. by H.-J. Rehm and G. Reed. In cooperation with </small><b><small>A. </small></b><small>Piihler and P. Stadler. </small>
<small>NE: Rehm, Hans J . [Hrsg.] 2., completely rev. ed. </small>
<small>Vol. 4. Measuring, modelling, and control / </small><b><small>ed. by K. Schiigerl. </small></b>
<small>- 1991 </small>
<small>ISBN 3-527-28314-5 (Weinheim) ISBN 1-56081-154-4 (New York) NE: Schiigerl, Karl [Hrsg.] </small>
<i>0 </i><small>VCH Verlagsgesellschaft mbH, D-6940 Weinheim (Federal Republic of Germany), 1991 Printed on acid-free and low-chlorine paper. </small>
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<small>Composition and Printing: Zechnersche Buchdruckerei, D-6720 Speyer, Bookbinding: Klambt-Druck GmbH, D-6720 Speyer Printed in the Federal Republic of Germany </small>
</div><span class="text_page_counter">Trang 5</span><div class="page_container" data-page="5">In recognition of the enormous advances in biotechnology in recent years, we are pleased to present this Second Edition of “Biotech- nology” relatively soon after the introduction of the First Edition of this multi-volume com- prehensive treatise. Since this series was ex- tremely well accepted by the scientific commu- nity, we have maintained the overall goal of creating a number of volumes, each devoted to a certain topic, which provide scientists in academia, industry, and public institutions with a well-balanced and comprehensive over- view of this growing field. We have fully re- vised the Second Edition and expanded it from ten to twelve volumes in order to take all re- cent developments into account.
These twelve volumes are organized into three sections. The first four volumes consider the fundamentals of biotechnology from bio- logical, biochemical, molecular biological, and chemical engineering perspectives. The next four volumes are devoted to products of indus- trial relevance. Special attention is given here to products derived from genetically engi- neered microorganisms and mammalian cells. The last four volumes are dedicated to the de- scription of special topics.
The new “Biotechnology” is a reference work, a comprehensive description of the state-of-the-art, and a guide to the original literature. It is specifically directed to micro- biologists, biochemists, molecular biologists, bioengineers, chemical engineers, and food and pharmaceutical chemists working in indus- try, at universities or at public institutions.
A carefully selected and distinguished Scien- tific Advisory Board stands behind the series. Its members come from key institutions repre- senting scientific input from about twenty countries.
The present volume, fourth in the series, re- flects the enormous impact of computer tech- nology on biotechnology, especially in the areas of measurement and control. It describes monitoring of the biotechnological process with sophisticated analytical techniques, use of the resulting data by means of mathematical models, and computer-aided closed loop con- trol for improvement of the productivity of biotechnological processes. While Volume 4
<b>can be used independently, Volume 3 “Bio- </b>
processing” is recommended as a companion volume.
The volume editors and the authors of the individual chapters have been chosen for their recognized expertise and their contributions to the various fields of biotechnology. Their will- ingness to impart this knowledge to their col- leagues forms the basis of “Biotechnology” and is gratefully acknowledged. Moreover, this work could not have been brought to fru- ition without the foresight and the constant and diligent support of the publisher. We are grateful to VCH for publishing “Biotechnolo- gy” with their customary excellence. Special thanks are due Dr. Hans-Joachim Kraus and Christa Schultz, without whose constant ef- forts the series could not be published. Finally, the editors wish to thank the members of the Scientific Advisory Board for their encourage- ment, their helpful suggestions, and their con-
</div><span class="text_page_counter">Trang 6</span><div class="page_container" data-page="6">August Kirchenstein Institute of Microbiology Latvian Academy of Sciences
Biochemical Engineering Research Centre Indian Institute of Technology
Weizmann Microbial Chemistry Laboratory Department of Chemistry
Manchester, UK
Department of Chemical Engineering
Massachusetts Institute of Technology Alimentaire Cambridge, MA, USA
Department of Applied Microbiology The Hebrew University
Departement de Genie Biochimique et Institut National des Sciences Appliquees
Institut fur Biotechnologie
Eidgenossische Technische Hochschule Scientific Development Group Oss. The Netherlands
</div><span class="text_page_counter">Trang 7</span><div class="page_container" data-page="7">Department of Plant Sciences University of Western Ontario London, Ontario, Canada
Chair of Fermentation Chemistry and Industrial Microbiology Lepetit Research Center Gerenzano, Italy
Institute of Molecular and Cell Biology National University of Singapore
Laboratory of Microbial Ecology Rij ksuniversiteit Gent
Gent, Belgium
Institut fur Biochemie
</div><span class="text_page_counter">Trang 8</span><div class="page_container" data-page="8">1 Common Instruments for Process <sup>12 </sup> Analysis and Control 5
6 Determination of Cell Concentration and Characterization of Cells 179
Process Models: Optimization of Yeast Production <small>- </small><b>A </b>Case Study
16 Control of Bioreactor Systems 509
<i><b>S. Shioya, K.-I. Suga </b></i>
19 Expert Systems for Biotechnology 625
<i><b>A . Halme, N. Karim </b></i>
9 Cell Models 267
<i>K. -H. Bellgardt </i>
</div><span class="text_page_counter">Trang 9</span><div class="page_container" data-page="9">E G & G
Idaho National Engineering Laboratory Idaho Falls, ID 83415, USA
Automation Technology Laboratory Helsinki University of Technology Electrical Engineering Building Otakaari 5A
SF-02150 ESPOO, Finland
<i><b>Chapter 19 </b></i>
Biological Reaction Engineering Group Chemical Engineering Department
Eidgenossische Technische Hochschule (ETH) Universitatsstrane 6
CH-8092 Zurich, Switzerland
<i><b>Chapter 2 </b></i>
Institut fur Technische Chemie
D-3000 Hannover 1, FRG
<i><b>Chapters 9 and 12 </b></i>
Department of Agricultural and
Fort Collins, CO 80523, USA
<i><b>Chapter 19 </b></i>
Biological Reaction Engineering Group Chemical Engineering Department
Eidgenossische Technische Hochschule (ETH)
</div><span class="text_page_counter">Trang 10</span><div class="page_container" data-page="10">Pohang Institute of Technology Pohang, Korea
<i><b>Chapter 15 </b></i>
Biochemical Engineering Program University of California
Irvine, CA 92717, USA
<i>Chapter 16 </i>
Institut fur Technische Chemie
Department of Chemical Engineering Program of Biotechnology
Ben-Gurion University of the Negev Beer Sheva, Israel
<i>Chapter <b>I 1 </b></i>
Institut fur Biosystemtechnik
Bundesforschungsanstalt fur Landwirtschaft Bundesallee 50
D-3300 Braunschweig-Volkenrode, FRG
<i>Chapter 8 </i>
Department of Chemical Engineering Massachusetts Institute of Technology Cambridge, MA 02139, USA
<i>Chapter </i>7
Colorado State University Fort Collins, CO 80523, USA
<i>Chapter </i>6
Institut fur Bioverfahrenstechnik Universitat Stuttgart
Boblinger StraRe 72 D-7000 Stuttgart 1, FRG
<i>Chapter <b>I0 </b></i>
Department of Chemical Engineering University of California
Davis, CA 95616, USA
<i>Chapter <b>I5 </b></i>
Institut fur Technische Chemie Universitat Hannover
CallinstraRe 3
D-3000 Hannover 1, FRG
<i>Chapter 6 </i>
</div><span class="text_page_counter">Trang 11</span><div class="page_container" data-page="11">Institut fur Technische Chemie
Department of Fermentation Technology Faculty of Engineering
Osaka University, Suita Osaka 565, Japan
Department of Chemical Engineering Massachusetts Institute of Technology Cambridge, MA 02139, USA
<i><b>Chapter 7 </b></i>
Department of Fermentation Technology Faculty of Engineering
Osaka University, Suita Osaka 565, Japan
<b>Institut fur Biotechnologie 2 </b>
Institute for Automatic Control East China University
of Chemical Technology 130 Meilong Lu
Shanghai, People’s Republic of China
<i><b>Chapter 12 </b></i>
</div><span class="text_page_counter">Trang 12</span><div class="page_container" data-page="12">Hannover, Federal Republic of Germany
The fourth volume of the second edition of “Biotechnology” presents a survey on an in- creasingly important field of biotechnology: monitoring of the biotechnological process with sophisticated analysis techniques, use of the resulting data by means of mathematical models, and (computer-aided) closed loop con- trol for improvement of the productivity of biotechnological processes.
The bottleneck in biotechnological process control is the on-line measurement of con- trolled process variables. Except for tempera- ture, impeller speed (for stirred tank reactors), aeration rate (for aerobic microorganisms),
<i><b>pH, po,, which are usually controlled process </b></i>
variables, and the composition of the outlet gas <i>(0, </i>and <i><b>C 0 2 content), which sometimes is </b></i>
a controlled process variable (respiration quo- tient,
However, manufacturers have recently made great efforts to improve process analysis and control. In several laboratories, on-line systems for the analysis of the chemical me- dium composition are used to gain more infor- mation about the process and to control the concentrations of key components. Further- more, mathematical models have been devel- oped in order to describe the production proc-
ess and to effect process optimization and con- trol. Therefore, the Series Editors decided to add to <i><b>Biotechnology a separate volume with </b></i>
the title “Measuring, Modelling, and Con- trol”, and they asked the Volume Editor to or-
Cell growth and product formation/sub- strate conversion is at the focus of attention, and here the measuring and control techniques are well-developed and generally applicable.
“Modelling, design, and control” of down- stream processes are also considered because of the great importance of downstream proc- essing. However, because of their broad scope, they are too heterogeneous and not yet suffi- ciently developed for treatment in the same way as processes for growth and product for-
</div><span class="text_page_counter">Trang 13</span><div class="page_container" data-page="13"><i><b><small>0 </small></b></i>instruments for gas analysis, and
<i><b><small>0 </small></b></i>biosensors.
The last group of instruments is still being de- veloped.
Only instruments that are (or can be) used for process control are considered in detail. However, modern off-line techniques (e.g., NMR) are also taken into account.
The measuring techniques are subdivided into four groups:
<i><b><small>0 </small></b></i>physical techniques for the characteriza- tion of fluid dynamics,
<i><b><small>0 </small></b></i>chemical methods for the analysis of broth composition,
<i><b><small>0 </small></b></i>physical methods for the determination of cell concentration, and
<i><b><small>0 </small></b></i>physical/biochemical methods for the characterization of the biological state of the cells.
Most of these are on-line techniques; others can only be carried out in a quasi on-line mode. All of them are used to characterize the reactor/medium/cell system.
There are interesting new developments in the characterization of such systems by mod- ern mathematical methods, with optimization of sampling to gain maximal possible informa- tion. These new techniques are also included in
<i><b><small>0 </small></b></i>aerobic wastewater treatment,
<i><b><small>0 </small></b></i>anaerobic wastewater treatment, and
<i><b><small>0 </small></b></i>models for recombinant microorgan- isms.
Models for animal and plant tissue cultures have not yet been included because no reliable kinetic data are available for mathematical modelling of these cultures.
Modern control techniques are increasingly applied to closed loop control of bioreactor systems. Therefore, different types of closed loop control techniques, including computer- aided control, are considered in detail.
Instrumental control is much more reliable than control by a human operator. Further- more, long-range (many weeks or months) runs are only possible in the laboratories of re- search institutes and universities if automated equipment is used. Thus, automation of bio- reactors is also taken into account.
<b>Chapter 18 on modelling, design, and con- </b>
trol of downstream processing covers only the most important downstream processes. Devel- opment in this field is still limited, so this chapter is not as extensive as the potential im- portance of downstream processing would warrant.
Expert systems are being developed in dif- ferent aspects of technology, medicine, and the natural sciences. Their use in biotechnolo- gy is desirable, since they would permit the identification of equipment failures and their eventual elimination. Furthermore, by means of expert systems, large amounts of informa- tion from on-line and off-line measurements as well as from the literature and from heuris- tic knowledge can be used with high efficiency.
The reviews consider only the most impor- tant techniques and omit some detail because of limited space. Further information can be gained through the reference notations.
It is hoped that information given in this volume will help students, engineers, and scientists at universities, members of research institutes, and those in industry to increase their knowledge of this important and fast- growing field.
<b>Hannover, March 1991 K. </b>Schiigerl
</div><span class="text_page_counter">Trang 14</span><div class="page_container" data-page="14">2.2 Dissolved Oxygen Partial Pressure, <i>po, <b>7 </b></i>
2.3 Redox Potential, <i>Eh, and Dissolved C 0 2 Partial Pressure, pcO2 9 </i>
4.4 Dissolved COz Partial Pressure, <i>pCo2 </i>
3 Instruments for Determination of Physical System Properties 10
</div><span class="text_page_counter">Trang 16</span><div class="page_container" data-page="16">6 <i>I <b>Common Instruments f o r Process Analysis and Control </b></i>
Biological processes are influenced by sev- eral control variables: temperature, pH, dis-
<i><b>solved oxygen partial pressure p o 2 , as well as </b></i>
by state variables such as redox potential, Eh,
<i><b>and dissolved C 0 2 partial pressure, pco2, </b></i>
which have a direct influence on cell metabo- lism (FORAGE et al., 1985).
Other control variables (power input, aera- tion rate) and state variables (liquid viscosity) have an indirect effect on cell growth and product formation. They influence gas disper- sion (bubble size, gas holdup, and specific in- terfacial area) and the transport processes in the broth. The broth volume can be deter- mined by means of the liquid level and the holdup. In continuous cultivation, the residence time of the broth or its dilution rate, which equals the specific growth rate of the cells, is determined by the liquid throughput and broth volume.
With highly foaming broth the cells are sometimes enriched in the foam by flotation. The diminution of the cell concentration in the broth reduces cell growth and product forma- tion rates. Foam may be carried out of the reactor by the air flow and then may clog the gas analysis instruments and cause infection of the broth. Therefore, the foam detector be- longs to the standard equipment of bioreac- tors. First, the use of these instruments for process analysis, optimization, and control is considered.
Cells have an optimum temperature and p H for growth and frequently another optimum for product formation. Several authors have considered the calculation of the optimum temperature and p H profiles for product for- mation.
FAN and WAN (1963) used the discrete maximum principle to calculate the optimum temperature and p H profiles for a continuous multistage enzymatic reactor to maximize product concentration.
BOURDARD and FOULARD (1 973) consid- ered the optimization of yeast production in a batch process by means of optimum tempera- ture and p H profiles using the continuous maximum principle.
SPITZER (1976) used a grid search method with subsequent steepest descent to maximize biomass productivity in a continuously oper- ated bioreactor by optimizing pH and sub- strate profiles.
RAI and CONSTANTINIDES (1973) and CON-
<small>STANTINIDES </small>and RAI (1974) investigated the
<i>production of gluconic acid with Pseudomo- </i>
<i>nus ovalis and of penicillin G by Penicillium </i>
<i>chrysogenum in batch operation and used the </i>
continuous maximum principle to maximize the productivity by means of optimal tempera- ture and pH profiles.
CONSTANTINIDES et al. (1970) and KING et al. (1974) studied the production of penicillin
<i>G by P. chrysogenum in batch operation and </i>
used the continuous maximum principle and/ or a specific optimal control to evaluate the optimum temperature profile for achieving maximum productivity. ANDREYEVA and BIRYUKOV (1973) also investigated the batch production of penicillin G and used the contin- uous maximum principle to find the optimum p H profile for maximum productivity.
</div><span class="text_page_counter">Trang 17</span><div class="page_container" data-page="17">BLANCH and ROGERS (1972) maximized profit in gramicidin S production by <i><b>Bacillus brevis by evaluating the optimum temperature </b></i>
and pH as well as the number of stages using the discrete maximum principle.
Erythromycin biosynthesis in batch opera- tion was maximized by CHERUY and DURAND (1979) by evaluating optimal temperature and pH profiles.
On the other hand, the pH variation can be used to control the production process. PAN et al. (1972) reported on penicillin production where carbohydrate and nitrogen source feed rates were controlled by measurement of the pH. The nitrogen source was metabolized to basic cations and the carbohydrate source to CO, and organic acids. The balance of the two ingredients provided a basis for the pH con- trol.
ANDREYEVA and BIRYUKOV (1973) pro- posed a model for this pH effect and its use for calculating optimal fermentation condi- tions. CONSTANTINIDES (1979) reviewed these publications. SAN and STEPHANOPOULOS (1984) also proposed a relationship between the total rate of biomass growth and ammonia addition to the reactor for pH control.
ROSEN and SCHOGERL (1984) used the con- sumption of sodium hydroxide solution at a constant pH to calculate the cell mass produc- tion rate of <i><b>Chaetomium cellulolyticum and to </b></i>
control the substrate feed by means of a mi- croprocessor in a fed-batch biomass produc- tion process. SHIOYA (1988) developed an ad- vanced pH control system for the measure- ment of biological reaction rates.
In many microbial or cell culture systems the pH varies during growth. Acid or base must be added to the broth to keep the pH at the optimal value. In some enzymatic hydro- lytic reactions acid or base must also be used to keep the pH constant by neutralizing the produced acid or base. From the amount of acid or base required for keeping the pH con- stant, the growth rate or enzyme reaction rate can be calculated.
If ApH(k+ 1) and ApH(k) are the differ- ences of pH from the set point at times <i>k + </i>1 and <i>k, F(k ) </i>is the feeding rate of acid or base for pH control, and <i><b>R(k) is acid or base pro- </b></i>
duction or consumption rate, then Eq. (1) can be used to calculate <i><b>R(k): </b></i>
<b>A pH(k </b>
where <i><b>a is a coefficient corresponding to the </b></i>
pH deviation caused by adding a unit amount of acid or base to the broth, and <i>b </i>is a coeffi- cient that corresponds to the pH deviation caused by the formation of a unit amount of cell mass or product.
If the pH is kept constant, i.e., A pH(k
be evaluated from
This principle was applied to
<i><b><small>0 </small></b></i>baker’s yeast production using a distur- bance predictive controller to determine the growth rate of the yeast,
<i><b><small>0 </small></b></i>determination of the reaction rate of N- acetyltyrosine ethyl ester (ATEE) with <i><b>a- </b></i>
chymotripsin to give ethanol and N-ace- tyltyrosine (AT) in a pH stat using a re- peated feedforwardlfeedback controller (repeated P F system),
<i><b><small>0 </small></b></i>determination of the overall production rate of (lactic) acid in hybridoma culture by an on-off controller.
The excretion of enzymes can sometimes be controlled by the pH value. For instance, LEE-
<small>LASART </small>and BONALY (1988) reported on con- trolling the excretion of acid phosphatase by
<i><b>Rhodotorula glutinis by means of the pH of </b></i>
the medium. The enzyme was excreted only in the pH range <b>4.5 </b>to <i><b>6.5. </b></i>
Several microorganisms produce different
<i><b>metabolites depending on the pH. Thus, As- </b></i>
<i><b>pergillus niger produces citric acid in the pH </b></i>
range from 2.5 to 3.5, whereas gluconic acid is produced at a higher pH and oxalic acid in the neutral pH range (SCHLEGEL, 1974).
Dissolved oxygen pressure or concentration is a state variable widely used to calculate the biomass concentration by 0,-balancing and to
</div><span class="text_page_counter">Trang 18</span><div class="page_container" data-page="18">8 <i>I Common Instruments <b>for </b>Process Analysis <small>and </small>Control </i>
control the growth or production process of aerobic microorganisms.
Furthermore, Po,-electrodes are used as re- search. tools for determining oxygen transfer rates (OTR) in pioreactors, biofilms, pellets, and cells immobilized in beads.
The use of oxygen balancing for real-time estimation of the biomass concentration was recommended first by HOSPODKA (1966). ZA-
<small>BRISKIE </small> and HUMPHREY (1978) worked out this technique of observation in detail. Using the relationship between oxygen uptake rate (OUR), the yield coefficient of the cell growth with regard to the oxygen consumption, Yx/02, the maintenance coefficient with regard to the oxygen consumption, moZ/X, and the
where
The growth rate may be approximated using Eqs. (3) and (4):
With this method the biomass concentration of <i>Saccharomyces cerevisiae was estimated. </i>
Several other authors used this technique in combination with the respiration coefficient, RQ, to estimate the biomass (e.g., COONEY et al., 1977; WANG et al., 1977; PERINGER and BLACHERE, 1979; TAKAMATSU et al., 1981). SQUIRES (1972) reported that po2 was used to control the sugar addition to the broth of
<i>Penicillium chrysogenum during penicillin pro- </i>
duction. The sugar feed was increased at a high po2 value; at a low po2 it was reduced. Since a close relationship exists between oxy-
gen and substrate uptake rates, this control of the substrate feed is very popular.
Under steady-state conditions, the oxygen uptake rate, OUR, and the oxygen transfer rate, OTR, are identical. Knowing the driving force for the oxygen transfer, <i>(0, </i>
be calculated: 0 TR
<i>KLa </i><small>= </small>
<i>(02 </i>
where <i>0, and 03 are the concentrations of the </i>
dissolved oxygen in the bulk and at the inter- face (in equilibrium with the gas phase). By measuring the oxygen balance during cell culti- vation, the volumetric mass transfer coeffi- cient can be calculated in real time.
<i>In cell-free systems, KLa can be determined </i>
by non-stationary or stationary measurements. The non-stationary method is based on the re-
By measuring the variation of the dissolved oxygen concentration in the bulk as a function of time, and calculating the dissolved oxygen concentration at the interface from the oxygen concentration in the gas phase, <i>KLa can be </i>
evaluated from Eq. (7). However, the interre- lationships between sorption rate and driving force are in practice more complex. Several re- lationships have been recommended for this calculation.
<b>A </b>good review of these methods is given in a ‘Report of a Working Party on Mixing’ of the European Federation of Chemical Engineering (LINEK and VACEK, 1986) and in the review article of LINEK et al. (1987).
Several papers consider the mass transfer of dissolved oxygen into biofilms, pellets, and cells immobilized in beads. The dissolved oxygen concentration profiles are determined by means of micro-oxygen electrodes (BUN-
<small>GAY </small>and HAROLD, 197 1 ; CHEN and BUNGAY, 1981; BUNGAY and CHEN, 1981; BUNGAY et al., 1969, 1983; WITTLER et al., 1986).
</div><span class="text_page_counter">Trang 19</span><div class="page_container" data-page="19">The combination of Eqs. (10) and (11) gives
The oxidation and reduction of a compound is controlled by the redox potential of its envi- ronment.
The oxidation-reduction potential of a pair of reversible, oxidizable-reducible compounds is related to the equilibrium between the oxi- dized (ox) and reduced forms (red) and the number of electrons involved in the reaction
<b>(ne-) (KJAERGAARD, 1977; KJAERGAARD </b>
and <b>JOERGENSEN, 1979; </b>THOMPSON <b>and GER- <small>SON, </small>in KJAERGAARD, 1977): </b>
The redox potential of this reaction is given by the Nernst equation:
R T activity of ox
<i><b>E h = E o </b></i>
n F activity of red
where <i><b>Eh </b></i>is the redox potential referred to the normal hydrogen electrode,
<i><b>Eo </b></i>is the standard potential of the sys- tem at 25 "C, when all activities of any reactants are at unity,
R the gas constant,
T the absolute temperature,
n the number of electrons involved in the reaction,
<i>F the Faraday constant. </i>
<b>(9) </b>
<b>JOERGENSEN (1941) introduced a concept ana- </b>
logous to the pH, namely the rH, which is de- fined as
<b>where aH2 </b>is the activity of hydrogen in the hy- drogen-hydrogen ion redox system according to Nernst. For hydrogen
This rH value may vary from rH <small>= </small>0, corre- sponding to a solution in which pH2 <small>= </small><b>1 bar </b>
and pH <small>= </small>0, to rH >42, corresponding to a so- lution with po, <small>= </small>l bar and pH <small>= </small>0. The rH val- ue is a function of the pH value. Therefore, for the measurement of the redox potential, both rH and pH values are needed.
The redox potential is used in practice for microaerobic cultivations, i.e., at very low dis- solved oxygen concentrations, which cannot be measured by standard oxygen electrodes. <b>An </b>
example is the production of exoenzymes by Bacillus amyloliquefaciens in continuous cul- ture at 0.5% oxygen saturation by means of
<b>redox-potential control (MEMMERT and WAN- <small>DREY, </small>1987). </b>
In small stirred tank reactors, the dissolved
COz concentration in the broth can be calcu- lated from the gas composition by assuming an equilibrium between the phases. In tower reac- tors and large commercial units, no equili- brium distribution <b>of COz exists between the </b>
phases; therefore, the direct measurement of
<i><b>pco2 can be useful. </b></i>
The driving force, (Pco2-pEo2), can be evaluated from the calculated pEo, at the in- terface and the measuredpco2 in the bulk. The
<b>CO, production rate, CPR, can be determined </b>
from the evolved gas stream and the gas com- position.
The volumetric mass transfer coefficient of the C 0 2 desorption is given by
CPR (KLa)co2 <small>= </small>
(Pco2-PEo2)
CPR can also be used for the calculation of the cell mass concentration and the specific growth rate, <small>,u. </small> The instantaneous specific growth rate of Penicillium chrysogenum was
<b>calculated by Mou and COONEY (1983) by </b>
measuring the CPR during the growth phase.
<i><b>By monitoring the O2 and/or COz concen- </b></i>
trations in the outlet gas and its flow rate, O2
<b>and/or CO, balances can be calculated and </b>
used for state estimation of biochemical reac-
</div><span class="text_page_counter">Trang 20</span><div class="page_container" data-page="20">10 <i>I <b>Common Instruments for Process Analysis and Control </b></i>
tors (e.g., STEPHANOPOULOS and SAN, 1982). However, because this state estimation method is based on measurements of the gas composi- tion, it will be discussed in Chapter <b>2. </b>
Temperature is the most important control variable for most biotechnological processes, including sterilization as well as cell growth and product formation. In general, a precision
<b>of f0.5 "C is necessary in the temperature </b>
range from +20 to
According to DIN 43 760 (German Stand- ard) the resistance of these instruments is guar- anteed with the following precision: 1OOf 0.1 ohm at 0 "C, which corresponds to an error of k 0.26 "C. Therefore, these resistance ther- mometers can be used without calibration. However, the resistances of all electrical con- nections must be controlled. These instruments are steam-sterilizable at 121 "C. Thermometers with short response times for fluid dynamical measurements are described in Chapter 4.
The absolute pressure is measured with re- spect to zero pressure. Gauge pressure is meas- ured with respect to that of the atmosphere. The SI unit of the pressure is Newton per square meter (N/m2) called Pascal (Pa). (1 bar=0.1 M P a = 10' N/m2; 1 mbar <small>= </small>100
P a <small>= </small>100 N/m2.) Bar and millibar deviate with
less than 2% from the technical and physical atmosphere.
Pressure measurements are necessary for the control of the sterilization and the state of the outlet gas filter as well as for the evaluation of the holdup and the partial pressures of the ga- seous components in the gas and liquid phases. Membrane pressure gauges are commonly used in biotechnology, because they are particularly suited to aseptic operations. Numerous pres- sure gauges are used in the chemical industry (HIRTE, 1980; ANDREW and MILLER, 1979). In biotechnology, the commonly employed pressure gauges are based on strain and/or capacitance measurements. The capacitance pressure gauges can measure very small pres- sure differences; therefore, they are used for liquid level measurements. For the construction of the different pressure meters, see HIRTE (1980) and ANDREW and MILLER (1979).
Measurement of the liquid volume is impor- tant for filling bioreactors with nutrient solu- tions, for continuous and for fed-batch culti- vations. It can be performed (OEDEKOVEN, 1980; ELFERS, 1964; ANDREW and RHEA, 1970) as follows:
<i><b><small>0 </small></b></i>by measuring the hydrostatic pressure difference between the bottom of the reactor, <small>P b , </small>and the head space, <small>P h , </small>by means of pressure gauges. The pressure difference is proportional to the weight of the liquid in the reactor:
where <i>h is the liquid height above the </i>
<i><b><small>p </small></b></i>the density of the broth, and
<i>g </i>the acceleration of gravity,
<i><b><small>0 </small></b></i>by measuring the total weight of the bottom,
reactor by load cells. The accuracy of the volume measurement is +0.2% for large reactors and
The measurement of the volume of an aer- ated broth is accomplished with a level con-
</div><span class="text_page_counter">Trang 21</span><div class="page_container" data-page="21">troller. The common liquid level meters are based on the variation of the capacitance C of the sensor with the composition of the dielec- tricum. For plate condensers, the capacitance is given by
<i><b>A </b></i>
C= <i><small>E O E , </small></i> <small>- </small>
<i>d </i>
<i><b>where A is the area of the plates, </b></i>
<i>d </i> the distance between the plates,
<i>E o the absolute dielectric constant </i>of vacuum, and
<i>E, the relative dielectric constant of the </i>
aerated broth between the plates.
<i>The value of E, of the broth and of the air dif- </i>
fer by a factor of about 80. In the case of non- aerated broth the capacitance of the condens- er, C, is given by
where Co is the capacity of the condenser with air,
<b>AC the capacity difference due to </b>
broth per unit height, and
<i>h </i> the height of the liquid in the ca- pacitor.
The capacity of the condenser with aerated broth is given by
where <i><b><small>E </small></b></i>is the gas holdup in the aerated broth. Analogous relationships hold true for cylindri- cal condensers (OEDEKOVEN, <b>1980). </b>
The accuracy of the level control amounts to
liquid level. In the case of large reactors, the level variation can be extremely large. There- fore, only the level of the broth can be meas- ured in the reactor, not that of the aerated broth, which is measured outside of the reac- tor, e.g., in a non-aerated section. Also in the case of foam formation, the measurement of the aerated broth level by capacitance instru- ments becomes difficult. Under these condi- tions floating bodies can be used as level con- trollers.
Since cultivation broths have adequate elec- trical conductivity, the liquid level can also be measured by inexpensive electrical conductivi- ty probes. Their application is restricted to aqueous broths. In the presence of a second (organic) liquid phase, their application cannot be recommended.
For other level control instruments, see, e.g., OEDEKOVEN <b>(1980), ELFERS (1964), AN- </b>
<small>DREW </small><b>and RHEA (1970). </b>
Gas and liquid flow rates are important con- trol variables for biotechnological processes; they must be known for reactor operation and for component balancing. In this chapter, only instruments for liquid throughput measure- ment are taken into account. Instruments for gas throughput measurements are considered
<b>in Chapter 2. Special techniques for measure- </b>
ments of local liquid velocities are treated in
<b>Chapter 4. </b>
Of the large number of available instru- ments ( S C H R ~ D E R , <b>1980; ANDREW et al., 1979; ERICSON, 1979) only three types are im- </b>
portant in biotechnological practice:
<small>- </small>differential pressure flowmeters, and
<small>- </small>magnetic-inductive flowmeters.
The floating body flowmeter or rotameter consists of a conical tube and a floating body with the upper diameter <i><b>D,, mass M,, and den- </b></i>
sity <i><b><small>ps </small></b></i>(Fig. 1). In the upstreaming fluid, the lifting force, which is produced by the differ- ential pressure across the slot between the tube wall and the floating body, is balanced by the weight of the floating body minus its buoyan- cy. The position of the float is a function of the flow rate and the density of the fluid, <i><b><small>p . </small></b></i>
<b>The volumetric throughput q v is given by </b>
The flow coefficient <i><b>a </b></i>is a function of the Rey-
<b>nolds number and the diameter ratio Dk/D,, </b>
<i><b>where Dk is the diameter of the tube at the up- </b></i>
per edge of the floating body.
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Calibration of <i><b>q v </b></i>is necessary because of the nonlinear relationship between the position of the floating body and the throughput. It can be carried out with water or air and recalcu- lated for the nutrient medium with known den- sity by means of the <i>a-Ru diagram, where </i>
the Ruppel number
depends only on the instrument constants and fluid properties, but not on the throughput.
The accuracy of rotameters is between <small>k </small>1 and k 3 % depending on the ratio <i><b>qv/qV,max </b></i>
( S C H R ~ D E R , 1980).
Differential pressure flowmeters consist of a tube with a restriction (usually an orifice plate). The pressures <i><b>p 1 and p z upstream and </b></i>
downstream of the orifice are measured. The
<i><b><small>p </small></b></i> the density of the fluid,
<i>D the tube diameter, </i>
<i>q </i> the dynamic viscosity of the fluid, and
<i><b>w </b></i> the mean flow rate of the fluid.
the orifice-to-tube diameter ratio <i>d / D for </i>
smooth tubes.
In practice, standardized orifices are used for which the flow coefficients are given in diagrams. The accuracy of calibrated orifice
<b>flowmeters is f0.5'70 of qv,max. </b>
According to the induction law of Faraday, an electrically conductive liquid passing a mag- netic field induces a voltage between two elec- trodes positioned perpendicular to the direc- tion of the flow. The voltage is proportional to the flow velocity:
where
<i>B the magnetic induction, D the tube diameter, and </i>
<i><b>The volumetric throughput q v is given by </b></i>
(SCHRODER, 1980):
<i>rcD </i>
<i>4 B B </i>
Cultivation broths are electrically conductive, because they contain nutrient salts. Therefore, magnetic-inductive flowmeters can be em- ployed for the measurement of nutrient me- dium throughputs. For the description of these instruments, see S C H R ~ D E R (1980).
Magnetic-inductive flowmeters are fairly ex- pensive. However, they have important advan- tages:
<small>- </small>the voltage <i><b>U is proportional to qv, </b></i>
<small>- </small>they are independent of the density and viscosity of the fluid as well as of the velocity profile of the fluidin tubes,
<small>- </small>they d o not produce a pressure drop,
<small>- </small>they do not have moving parts,
<small>- </small>they can be steam-sterilized.
Their accuracy is <small>k </small>1% at <b>qv,max, </b>and <small>k </small>1.5% at <b>0.5 qv.max. </b>
The flow coefficient <i>a is usually given as a </i>
function of the orifice Reynolds number and
</div><span class="text_page_counter">Trang 23</span><div class="page_container" data-page="23"><i>In an agitated reactor, the power input, P, </i>
can be calculated by Eq. (23) by measuring the torque on the shaft, <i>MN, and the speed of ro- </i>
tation,
The torque is measured by torsion dynamome- ters or strain gauges and the impeller speed by an electronic tachometer. In large-scale reac- tors, the consumed electrical energy, as meas- ured by the wattmeter, yields useful data on power input, if the mechanical losses in gear, seals, etc., are taken into account.
In small laboratory reactors, the mechanical losses are considerable in comparison with the power input into the broth. Therefore, power input measurements are inaccurate and are not recommended.
<i>In bubble columns, P can be calculated by </i>
where <i>MG </i> is the gas mass flow,
<i>R </i> the gas constant,
T the absolute temperature,
<b>pin </b> the gas pressure at the column
However, since the second and third terms to- gether make up only 0.2% of the overall pow- er input, the power input due to the gas expan- sion dominates:
<b><small>P i n </small></b>
<b><small>Pout </small></b>
In the power inputs, Eqs. (24) and <i><b>(25), </b></i>the en- ergy losses due to mechanical energy (e.g., due to gas compression) are not considered.
The viscosity of the broth influences the op- eration of bioreactors considerably. At a high viscosity, a high specific power input is neces- sary to increase the intensity of transfer proc- esses: oxygen transfer (into the broth of aero- bic microorganisms) and mixing. Since at high specific power input the energy dissipation rate in the reactor is high, improvement of heat transfer is also important to keep the tempera- ture constant.
High viscosity can be caused by high sub- strate concentration (e.g., starch), high prod- uct concentration (e.g., xanthan), high cell concentration (e.g., penicillin), high solid con- tent (e.g., peanut flour), or by their combina- tion. The most general description of the rheo- logical properties of fluids is given by the rela- tionship between the velocity gradient dv/dx and the stress, <i><b><small>T, </small></b></i>the so-called flow equation: dv
<small>- = </small>
<i><b>dx </b></i>
as long as viscoelastic behavior is not present or very slight. This flow equation can be calcu- lated from the experimentally measured shear diagrams (shear rate versus shearing stress). It should be noted, however, that such a calcula- tion is not always possible. In contrast to the shear diagram, the flow equation is indepen- dent of the experimental conditions (e.g., the type of viscosimeter) used for the determina- tion of the viscosity.
There are many methods available to esti- mate the rheological behavior of fluids, but there are only a few that furnish true fluidity values. These include the capillary, the falling sphere, the Couette, the Searle, and the tor- sional pendulum methods. Until now, the eval- uation of the flow equation from the shear diagram has only been possible for the capil- lary, Couette, and Searle methods (MUSCHEL-
<small>KNAUTZ </small>and HECKENBACH, 1980).
The capillary viscosimeter cannot be em- ployed for cultivation broths because of ad-
</div><span class="text_page_counter">Trang 24</span><div class="page_container" data-page="24"><small>14 </small> <i><b><small>1 </small></b><small>Common Instruments </small><b>for </b><small>Process Analysis and Control </small></i>
<b>verse wall effects in the capillary. As for the </b>
falling sphere and torsional pendulum viscosi- meters, the flow equation cannot be calculated from the shear diagram (only partial solutions are known).
The Couette and Searle viscosimeters can only be used if the following conditions are fulfilled: the annular slit between inner and outer cylinders must be large enough to reduce the wall effects, and measurements must be made using different cylinder lengths to elimi- nate the end effects. In a Searle viscosimeter, the speed of rotation is limited by the occur- rence of Taylor instabilities.
By measuring the torque <i>MN </i>on the shaft of different types of stirrers at differing stirrer speeds, <i>N </i>is suited for the evaluation of the power input but not for the viscosity. These techniques, which are commonly used accord- ing to the literature, are not suitable for the evaluation of the shear diagram and the abso- lute viscosity.
Only the coaxial cylinder viscosimeters, Couette with rotation outer cylinder and Searle with rotation inner cylinder, are consid- ered here, since they are the most popular
where <i><small>w </small></i> is the angular speed,
Mi the torque exerted on the inner cy- linder, and
<i>L the length of the inner cylinder. </i>
From Eqs. (27) and (28) it follows that
<small>ti </small>and <i><small>t, </small></i>are the shear stresses at the in- ner and outer cylinders.
The relationship between the angular velocity
<i><b>of the rotating cylinder SZ and </b><small>t </small></i>is experimen- tally determined to obtain the shear diagram. The relationship dv/dx=f(z) (flow equation) can be calculated from Eq. (30). For this eval- uation, see MUSCHELKNAUTZ and HECKEN-
<small>BACH </small> (1980) and DINSDALE and MOORE
where <i><b>q </b></i>is the dynamical viscosity.
In practice, relative viscosities are frequent- ly determined. The shear stress is measured for different shear rates with fluids of known (oils) and unknown (broth) viscosities, and the relative viscosity of the broth can be calculated from the ratio of their shear stresses at the same shear velocity, if the broth has Newton- ian behavior.
On-line determination of the broth viscosity is sometimes useful for controlling a process. The on-line techniques only yield relative vis- cosities. The viscosity of the <i>Aspergillus niger </i>
broth was measured on-line by means of a tube viscosimeter by BLAKEBROUGH et al. (1978). PERLEY et al. (1979) used an on-line capillary technique for the measurement of the viscosity <i>of the Hansenula polymorpha broth. </i>
LANGER and WERNER (1981) and NEUHAUS et al. (1983) developed an on-line slot-type vis- cosimeter and measured the viscosity of the
<i>Penicillium chrysogenum broth. KEMBLOWSKI </i>
et al. (1985) used an on-line impeller type vis- cosimeter to determine the viscosity of the
<i><b>A ureobasidium pullulans broth. </b></i>
Integration of Eq. (29) with <b><small>s2 = </small></b><i>R?/Ri </i><small>= </small>tilta
cially a combination of different surfactants with proteins, may cause stable foams in aer- ated bioreactors. Foam control is necessary to
</div><span class="text_page_counter">Trang 25</span><div class="page_container" data-page="25">avoid the loss of broth, the clogging of the gas analyzers, and infections caused by foam carry-out.
Foam can be suppressed by antifoam agents (BEROVIC and CIMERMAN, 1979; SIE and SCHOGERL, 1983; SCHUGERL, 1986; PRINS and <small>VAN'T </small>RIET, 1987; VIESTURS et al., 1982) or destroyed with mechanical foam breakers (VIESTURS et al., 1982). Foam can be detected by an electrical conductivity probe, capaci- tance probe, heat conductivity probe, or light scattering probe (HALL et al., 1973; VIESTURS et al., 1982). Antifoam and mechanical foam breakers are frequently combined, if the foam is very stable.
The presence of an antifoam agent in the broth may influence cell growth and product formation as well as downstream processing. Mechanical foam breaking may exert stress and selection pressure on the cells.
The dissociation constant K, of the purest water is very low (10-'5.74 at 25 "C). The con- centration of water can be considered as con- stant because of the low K, value. Thus, only the ion product K, is taken into account: [ H + ] <small>* </small>[OH-] =K,= 1.008. at 25 "C (32a) Forming the logarithm of Eq. (32a)
log [H
-log [ H + ] = p H -log [OH-] <i><b>=POH </b></i>
-log K, <small>= </small>PK, and pH fpoH <small>= </small>pK,
At [H
The pH can be measured with a galvanic cell
<i><b>(chain). The potential E of the cell is given by </b></i>
the Nernst equation:
<i>R T F </i>
where <i>Eo is the standard potential and F the Faraday constant. </i>
In this definition the thermodynamic activities of the ions were replaced by their concentra- tions since the activities cannot be measured. The absolute potential cannot be measured either, only the potential difference
Silver-silver chloride electrodes are used in the galvanic chain for sterilizable electrodes. Fig. 2 shows the schematic assembly of a pH electrode (INGOLD I). In this figure <i>E l is the </i>
potential on the outer surface of the glass membrane, which depends on the pH value of
<i><b>the sample solution. E2 is the asymmetry (bias) </b></i>
potential, i.e., the potential of the glass mem- brane with the same solutions on both sides.
<i><b>E3 is the potential on the inner surface of the </b></i>
glass membrane, which is a function of the pH
<i><b>value of the internal buffer solution. E4 is the </b></i>
potential of the internal Ag/AgCl lead-out electrode, dependent on the KCl concentration in the internal buffer solution. <i><b>E5 is the poten- </b></i>
tial of the reference AgCl/Ag electrode, which
<small>reference </small>
<b><small>elect rulyt </small></b>
<small>internal buffer solution </small>
<b><small>Fig. 2. </small></b><small>Schematic assembly of </small>a <small>pH-electrode (Dr. </small>
<b><small>W. </small></b><small>Ingold </small><b><small>AG, Brochure </small></b>I, <small>with permission). For details see text. </small>
are obtained.
</div><span class="text_page_counter">Trang 26</span><div class="page_container" data-page="26"><b>16 </b> <i><small>I </small>Common Instruments f o r Process Analysis and Control </i>
depends on the KC1 concentration in the refer-
<i><b>ence buffer solution, E6 is the diaphragm or </b></i>
diffusion potential.
<i><b>Since El </b></i>is the potential which we want to measure, the individual potentials <i><b>E2-E6 </b></i>
should be kept constant. These are included in the standard potential
In modern pH electrodes,
<small>- </small>10.4k3.8 mV at pH 7.02 and 20 "C). The potential difference between the indica- tor and reference electrodes <i>U is also given by </i>
the Nernst equation:
<small>- </small>
<i>2.3R T </i>
<i>F </i>
where the Nernst potential UN <small>= - - </small>
59.2 mV at 25 "C. However, in real pH elec- trodes, the Nernst potential is not attained, but only approached to 97.5% (in the case of new electrodes). Furthermore, <i>UN is reduced with </i>
increasing age of the electrode. The aging causes sluggish response, increasing electrical resistance, <b>a smaller slope, and zero point </b>
drift. During steam sterilization, a pressure difference builds up on both sides of the glass membrane. Therefore, a counter pressure is imposed to avoid the destruction of the elec- trode. Frequent steam sterilization has a con- siderable aging effect. Therefore, pH elec- trodes must be recalibrated frequently with buffer solutions.
<i><b>During in situ steam sterilization a consider- </b></i>
able, irreversible signal drift of the pH electro- des occurs. Therefore, it is advisable to meas- ure the pH value of the broth in the reactor after each steam sterilization by an indepen- dent method and correct the reading of the pH meter.
Since the potential <i>U depends on the tem- </i>
perature, pH-meters have a temperature com- pensation, which is usually calculated by the relationship
<i><b>UN( T ) </b></i><small>= </small>UN(25 "C) (1
where ~ ~ = 3 . 2 1 f O . 5 3 . 1 0 - ~ / " C ,
<i>t </i><small>= </small><i>T </i><small>- </small>standard temperature (25 "C).
For more information on pH electrodes, their use, storage, aging, etc., see INGOLD I, PE-
<small>TERSEN </small> (1 980), MELZNER and JAENICKE (1980), and MCCULLOUGH and ANDREW (1979).
The dissolved oxygen concentration is also measured by electrochemical methods. Two types of electrodes are in use:
<small>- </small>polarographic electrodes
<small>- </small>galvanic electrodes.
In polarographic or amperometric elec- trodes the dissolved oxygen is reduced at the surface of the noble metal cathode in a neutral potassium chloride solution, provided it reaches 0.6-0.8V negative with respect to a suitable reference electrode (calomel or Ag/ AgC1). The current-voltage diagram is called the polarogram of the electrode (Fig. 3).
<small>1 </small>
<b><small>Negative bias voltage </small></b> <small>Oxygen </small>
<i><b><small>Fig. 3. Polarogram and calibration curve for a po,- </small></b></i>
<b><small>electrode (LEE and TSAO, 1979). </small></b>
At the plateau of the polarogram, the reac- tion rate of oxygen at the cathode is limited by the diffusion of oxygen to the cathode. Above this voltage the water is electrolyzed into oxy- gen and hydrogen. In the plateau region (0.6-
0.8 V), the current is proportional to the par- tial pressure of the dissolved oxygen (Fig. 3).
In this probe, the cathode, the anode, and the electrolyte are separated from the measur-
</div><span class="text_page_counter">Trang 27</span><div class="page_container" data-page="27">ing liquid by a membrane which is permeable to gaseous oxygen. In the electrolyte, the fol- lowing reactions occur: Since hydroxyl ions are constantly being sub- stituted for the chloride ions as reaction pro- ceeds, KCl or NaCl must be used as an electro- lyte. When the electrolyte becomes depleted of C1-, it has to be replenished.
The dissolved oxygen concentration is meas- ured by the galvanic electrode which does not require an external voltage source for the re- duction of oxygen at the cathode. Using a basic metal such as zinc or lead as anode and a nobler metal such as silver or gold as cathode, the voltage is generated by the electric pair and is sufficient for a spontaneous reduction of oxygen at the cathode surface. The reaction of the silver-lead galvanic electrode is given by:
During the reduction of oxygen, the anode sur- face is gradually oxidized. Therefore, occa- sional replacement of the anode is necessary.
The polarographic or amperometric elec- trode is in greater demand in biotechnological practice than the galvanic electrode. Fig. 4 shows a schematic view of a steam-sterilizable polarographic or amperometric oxygen elec- trode.
<b>A constant voltage (ca. 650 mV) is applied </b>
<b>between cathode (Pt) and anode (AgIAgCl). A </b>
regular control of this voltage is necessary in order to avoid incorrect measurements. The <small>Gas permeable mernbr 'ane </small>
<small>Sterilizable </small>po,-electrode (Dr. <small>W. Ingold </small>
<b><small>AG, </small></b>Brochure <b><small>11, </small></b>with permission).
control is carried out by measuring the polaro- gram and adjusting the bias voltage to main- tain a voltage-independent current in the pla- teau region of the polarogram.
The current <i><b>ip,02 </b></i>is proportional to <i>po2 </i>only in the plateau region:
where <i>K </i>is a constant,
<i><b>A the surface area of the cathode, </b></i>
<i>P </i>the membrane permeability,
<i>d </i>the membrane thickness.
The response time is proportional to <i>d 2 / P . </i>
<i><b>Therefore, thin membranes with high gas 02- </b></i>
permeability are used. Two membranes are used for the <i>p o , </i>electrodes for sterile opera- tion. The inner membrane consists of a 25 pm teflon foil, the outer one of a 150 wm silicone membrane reinforced by thin steel mesh. This type of electrode was developed by the Instru-
</div><span class="text_page_counter">Trang 28</span><div class="page_container" data-page="28">18 <i><small>1 </small><b>Common Instruments for Process <small>AnalyJ :is and </small>Control </b></i>
mentation Laboratory Inc., Lexington, Mass., USA, and also produced by Dr. W. Ingold AG, Urdorf, Switzerland (INGOLD 11). This type of electrode has a fairly long response time (45 to 90 s to attain 98% of the final sig- nal).
During steam sterilization, the membrane thickness and shape change irreversibly. An improved construction of BAUERMEISTER (1981) enables the electrodes to endure many (ca. 20) sterilizations without any change in the membranes.
The temperature of the calibrations and measurements must be controlled closely <small>(k </small>0.1 "C) because of the temperature sensitivi-
ty of the signal (temperature coefficient 3%/ "C). Since the electrode measures the partial pressure of oxygen, the signal is independent of the 02-solubility in the broth. The calibra- tion should be performed in the reactor under the same fluid dynamic conditions (stirrer speed) as those that prevail during cultivation to avoid errors due to differences in diffusion resistance at the surface of the membrane.
The calibration is carried out with nitrogen- and air-saturated broth by setting these values at 0 and 100%. The partial pressure of oxygen is expressed as follows:
<i><b>p o 2 = </b></i><b>[PB-p(HzO)] x 0.2095 </b> (37) where pB is the temperature-corrected
(barometric) pressure in the react or,
p(H20) the vapor pressure of the broth at the temperature of the calibration,
0.2095 the fraction of oxygen in at- mospheric air.
The sources of error in the measurement of
<i><b>po2 </b></i>are numerous: errors in reading of temper- ature and pressure, drift due to membrane fouling, change in membrane shape, variation of bias voltage and electrical resistance as well as capture of bubbles, etc. With sufficient ac- curacy of temperature and pressure measure- ments, and with bias voltage in the plateau re- gion, the precision of the measurements is on the average f <i><b>5 % . </b></i>Below <i><b>5 % </b></i>of the 02-satura- tion, the error increases with decreasing po,.
The dissolved oxygen concentration [O,] is calculated by the relationship:
and <i><b><small>CY </small></b></i>is the Bunsen coefficient.
Bunsen coefficients <i><b><small>CY </small></b></i>of oxygen for some simple aqueous solutions and a few cultivation broths have been given by SCHUMPE (1985). For more details, see MELZNER and JAENICKE (1980), INGOLD 11, LEE and TSAO (1979), FRITZE (1980), BUEHLER and INGOLD (1976), and SCHINDLER and SCHINDLER (1983).
The definition of the redox potential is given by Eq. (9). To determine E , the potential be- tween the redox electrode and a standard refer- ence electrode is measured. The universal ref- erence reaction is the oxidation of hydrogen: H 2 - + 2 H + + 2 e -
(39) The standard potential Eo(H+/H2) is by defi- nition equal to zero at all temperatures. The universal reference electrode is known as the Standard Hydrogen Electrode (SHE), which consists of a platinum-coated platinum foil that is immersed in a solution containing 1 mol L - ' H + , and over which flows hydrogen gas at a pressure of 1 bar. The reference electrodes (Hg/calomel/sat. KC1, or Ag/AgCl/KCl) used in practice are referred to the SHE:
where Eh is the redox potential against the
</div><span class="text_page_counter">Trang 29</span><div class="page_container" data-page="29">The sterilizable redox meter consists of a Pt electrode and an Ag/AgCl reference electrode. The electrodes are calibrated with redox buf- fers in the range of <b>Eh </b><small>= </small>
Redox potentials occur in a range of
mV. A simple pH meter with a mV scale is an adequate measuring instrument. The redox po- tential depends on the po, and pH in the broth. However, since both are measured in bioreactors, these effects can be taken into ac- count. In aerobic cultivations the po, and re- dox meters give nearly the same information at a constant pH value. In microaerobic and anaerobic cultivations the redox potential gives additional information about the state of the broth components. However, because of the complex composition of the broth this infor- mation is only qualitative.
For more information on the redox poten- tial, see MELZNER and JAENICKE (1980), KJAERGAARD (1977), KJAERGAARD and JOERGENSEN (1979), INGOLD 111, and FRITZE (1980a, b).
<i><b>The presence of dissolved C 0 2 in the broth </b></i>
influences cell growth and product formation (Ho et al., 1987). Therefore, thepco2 can be an important variable. The pco, can be meas- ured in-line using thepcoz meter of Dr. <b>W. In- </b>
gold <b>AG (INGOLD IV). The instrument con- </b>
sists of a pH meter and a hydrogen carbonate solution, which is separated from the broth by a gas-permeable membrane. Fig. <i><b>5 </b></i>illustrates the main features of the electrode.
The dissolved <i>Cot </i>diffuses through the membrane into the hydrogen carbonate solu- tion. The equilibrium of the reaction
CO,+H,O
Measu
<b><small>Fig. 5. </small></b><small>Sterilizable pco,-electrode (Dr. </small><b><small>W. Ingold AG, Brochure IV, with permission). </small></b>
<small>Construction of a C0,-sensor: (1) 20 mL syringe, </small><b><small>(2) </small></b>
<b><small>high-temperature coaxial cable, (3) cable screw con- </small></b>
<small>nection, (4) adjustment nut, </small><i><b><small>( 5 ) </small></b></i><small>locking plug, (6) supply </small>duct, <b><small>(7) welding socket, </small></b>(8) <small>bore hole con- ductor, </small>(9) <small>draw tube, (10) pH-electrode, (11) refer- </small>
<b><small>ence electrode, (12) C0,-electrode, </small></b><small>(13) membrane body, (14) calibration buffer, </small><b><small>(15) </small></b><small>glass membrane, (16) reinforced silicon membrane. </small>
<i><b>is determined by the dissociation constant K </b></i>
<i><b>where H is the Henry coefficient. </b></i>
Since the hydrogen carbonate concentration in the electrolyte is high, it can be assumed to be constant. Thus, Eq. (41) can be simplified to
The potential of the inner pH electrode is a function of [H'I:
</div><span class="text_page_counter">Trang 30</span><div class="page_container" data-page="30">20 <i><small>I </small>Common Instruments f o r Process <small>Analysis and </small>Control R T </i>
<i>F </i>
<i><b>E </b></i><small>= </small><i>Eo </i>
<i>where 2.3 R T/F=59.16 mV at 25 "C, </i>
<i>E is the measured potential, and Eo is the standard potential. </i>
From relationships (43) and (44)
The response time is fairly long (one to sev- eral minutes) and is influenced by the thickness of the membrane and by the electrolyte solu- tion as well as by the response time of the pH electrode.
The measuring range of the electrode is 1 to 1000 mbar COz. The deviation is f 2 % , if the electrode is calibrated with gas mixtures. If the inner pH electrode is calibrated by buffer solu- tions, the deviation is f 10%. To avoid errors due to the complex temperature dependence of the reading, the calibration should be carried out at broth temperature.
The electrode is sterilizable. The steriliza- tion is performed after the reduction of the pressure of the p H electrode on the stainless- steel reinforced plastic membrane. The p H electrode is calibrated by buffer solutions after sterilization. Then the electrode is filled with the electrolyte and put into the measuring posi- tion. Fig. <i><b>5 </b></i>shows the electrode during calibra- tion and measurement. For more information, see INGOLD IV.
According to FLY" (1982) the relevance, accuracy, and precision of the measured data and the reliability, accuracy, precision, resolu- tion, specificity, response, sensitivity, availa- bility, and costs of the sensors/instruments are important for their use in process control. All
data which influence the productivity and the yield of the process and the quality of the product are relevant. Accuracy of the meas- ured data is expressed as the difference be- tween the observed value of the variable and its true value, which is usually determined by calibration.
The precision of the data relates to the probability that repeated measurements of the same system will produce the same values. The distribution of the values around their mean is usually characterized by the variance and/or standard deviation, or, e.g., the 95% confi- dence interval.
The most important property of a sensor is its reliability, which is made up of factors such as failure rate, failure mode, ease of preventive maintenance, ease of breakdown maintenance, physical robustness, and its credibility in the mind of process operators (FLY", 1982). The latter plays a role only if the data are used by the operator and not by a n automated sys- tem.
Based on information from three chemical works, LEES (1976) published data on the re- liability of the instruments important in the fermentation industry (Tab. 1).
One can observe that at the time of investi- gation (1970-1975) the pH meter and the <i>0, </i>
and COz analyzers were the least reliable in- struments. During the last ten years, the relia- bility of these instruments has been improved considerably, provided an accurate flowmeter is used for the <i>0, </i>and CO, instruments.
<b>FLY" (1982) gave detailed results on the </b>
performance of the instruments in a 1 m 3 pilot plant bioreactor (Tab. <b>2). </b>
<i><b>One can see that the po2 measurement had </b></i>
the lowest accuracy, the <i><b>po2 </b></i>and air flow con- trol the lowest precision, and the volume meas- urement the lowest resolution. In the mean- time, the air-flow control should have attained a much higher accuracy and precision, pro- vided the right instrument is used (e.g., mass flowmeter). In recent years, the accuracy of the <i><b>po2 </b></i>measurement has not been improved markedly, it can, however, be achieved by fre- quent calibration. The accuracy and precision
<i><b>of the po2 control is much better if one uses </b></i>
three sensors and parameter-adaptive control.
</div><span class="text_page_counter">Trang 31</span><div class="page_container" data-page="31"><b><small>Tab. 1. Instrument Reliability </small></b>(LEES, <small>1976) </small>
<small>Notes: W , weekly; H, hourly; R, per run, which relates to the frequency with which the measuring instru- ments are recalibrated </small>
</div><span class="text_page_counter">Trang 32</span><div class="page_container" data-page="32"><i><b>22 </b><small>1 </small><b>Common Instruments f o r Process Analysis and Control </b></i>
In this chapter, only H +-selective electrodes are considered. However, using ion-selective membranes, in principle the concentration of an arbitrary ion can be determined by means of the Nernst equation:
The production of ion-selective carrier-mem- brane-electrodes is very easy. A standard pH- electrode is combined with an ion-selective membrane consisting of an ionophore in a polymer matrix.
The ionophore and the softener are usually dissolved in a PVC solution, put on the sur- face <i><b>of the pH-electrode, and dried. Fig. 6 </b></i>
shows several constructions of such elec- trodes.
Ion-selective membranes may be prepared by ionophore antibiotics (valinomycin, nonac- tin, etc.) (SCHINDLER and SCHINDLER, <small>1983) </small> and synthetic carriers (crown ethers and cryp- tates, cyclodextrins, cyclotriveratrylene, perhy- drotriphenylene, etc.) (ATWOOD et al., <small>1984; </small> V ~ G T L E , 1975, <small>1981). </small>Chiroselective transport molecules are particularly interesting for the more detailed analysis of broth components (LEHN, <small>1988). </small>
At present, reliability and selectivity of ion- selective membranes are not always satisfacto- ry. However, host-guest-complex chemistry is developing rapidly. Therefore, it is expected that some years from now reliable, ion-selec- tive electrodes will be available.
The combination <i>of pH, po,-, pco,-, </i> and NH: -selective transducers with biochemical receptors (enzymes, antibodies, lectins, etc.) is considered in Chapter 3 (Biosensors).
<b><small>Fig. </small></b><i><b>6 . </b></i><small>Different types of ion-selective carrier mem- brane electrodes with liquid- and solid-lead-offs (SCHINDLER and SCHINDLER, 1983, with permis- sion). </small>
<b><small>(a) </small></b><small>Glass membrane electrode. (1) ion-selective glass membrane, </small> <b><small>(2) non-specific glass shaft, (3) Ag/ </small></b>
<small>AgC1-lead-off electrode, </small><b>(4) </b><small>lead-off electrode (liq- uid), </small><i><b><small>( 5 ) </small></b></i><small>cable. </small>
<b><small>(b) </small></b><small>Liquid membrane electrode with ion-exchanger reservoir. </small><b><small>(1) porous membrane, (2) ion-exchanger </small></b>
<small>reservoir, (3) lead-off electrolyte (liquid), </small><b><small>(4) Ag/ </small></b>
<small>AgC1-lead-off electrode. </small>
<b><small>(c) </small></b> <small>PVC ion-exchanger membrane electrode. (1) PVC ion-exchanger membrane, </small><b><small>(2) PVC tube, (3) </small></b>
<small>lead-off electrolyte (liquid), </small><b>(4) </b><small>Ag/AgCl-lead-off electrode. </small>
<b><small>(d) Coated wire-electrode. (1) Pt-wire, (2) PVC ion- </small></b>
<small>exchanger membrane, (3) cable. </small>
<b><small>(e) </small></b><small>Disc electrode without </small><i><b><small>O2 </small></b></i><small>reaction barrier. (1) carrier-PVC-membrane, (2) Pt-wire, (3) acryl/glass mantle, (4) PTFE-insulated, silver-coated Cu-wire, </small>
<i><b><small>( 5 ) </small></b></i><small>PTFE or acryl glass. </small>
<b><small>(f) </small></b><small>Coated glass electrode. (1) carrier-PVC-mem- brane, </small><b><small>(2) ion-selective glass membrane, </small></b>(3) <small>acryl glass mantle, </small><b><small>(4) </small></b><small>Ag/AgCl-lead-off electrode, </small><i><b><small>( 5 ) </small></b></i><small>in- ner electrolyte or cement lead-off, e.g., Ag/AgCl/ </small>
<i><b><small>Harvard cement, (6) non-specific glass shaft, (7) </small></b></i>
<small>acryl glass or PTFE. </small>
<i><b><small>(9) Disc electrode with O2 reaction barrier. </small></b></i><small>(1) car- rier-PVC-membrane, </small><i><small>(2) </small></i><small>Ag/AgCl (melt), (3) Pt- wire, (4) acryl glass mantle, </small> <i><b><small>( 5 ) </small></b></i><small>PTFE-insulated, </small>
<i><b><small>silver-coated Cu-wire, (6) PTFE or acryl glass with </small></b></i>
<small>Ag/AgCl/Pt-solid contact. </small>
</div><span class="text_page_counter">Trang 33</span><div class="page_container" data-page="33"><small>M. (1983), Dissolved oxygen contours in </small><i><b>Pseudo- </b></i>
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<i><b>Process Industries </b></i><small>(ANDREW, </small>
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</div><span class="text_page_counter">Trang 36</span><div class="page_container" data-page="36">Zurich, Switzerland
1 Introduction 30
2 Mass Balancing for Gas Analysis 31 2.1 Basic Gas Balance Equations 31
2.2 Inert Gas Balance to Calculate Flow Rates 33
2.3 Steady-State Gas Balance to Determine the Biological Reaction Rate 33 2.4 Determination of CPR with Accumulation of CO, in the Liquid Phase 34 2.5 Determination of
Liquid Phases 35
2.6 Determination of
2.7 Determination of Oxygen Uptake Rates by a Dynamic Method 36 2.8 Loop Reactors with External Aeration to Determine OUR 36 2.9 Methods to Measure Low Oxygen Uptake Rates 37
2.10 Oxygen Transfer in Large-Scale Bioreactors 38 3.1 Systematics of Elemental Balancing 41
3.2 Elemental Balancing for Monitoring a Poly-P-Hydroxybutyric Acid (PHB) Producing Culture 42
4.1 Objectives of On-Line Gas Analysis and Requirements for Accuracy and Reliability 45 4.2 Definition of Measurement Requirements 45
4.3 Errors Caused by Simplification of Balancing 46
<b>3 Application of Gas Analysis Results to Elemental Balancing Methods 41 </b>
4 Error Analysis for Gas Balancing 44
4.3.1 Simplifications Concerning Pressure, Temperature, Humidity, and Gas Flow 4.3.2 Errors Caused by Steady-State Assumption 47
4.4 Erroneous Estimation of Reaction Rates Caused by Measurement Errors 49 4.4.1 Errors in the Measurement of Gas Flow 49
4.4.2 Statistical Error Propagation 49 4.4.3 Errors in Oxygen Gas Analysis 50
4.4.4 Instantaneous Error Analysis for the Elemental Balancing Example PHB 4.4.5 Dynamic Error Analysis for Reaction Rates 54
5.1 System without Removal of Condensable Volatiles 56 Rates 46
51
<i><b>5 </b></i> Sample Pretreatment and Multiplexing 56
</div><span class="text_page_counter">Trang 37</span><div class="page_container" data-page="37"><b>5.2 </b> Application of Paramagnetic and Infrared Analyzers to the Measurement of Oxygen
<b>and Carbon Dioxide 56 </b>
<b>5.3 Special Valve Manifolds for Mass Spectrometers 57 6.1 Positive Displacement Devices </b> 58
<b>6 . 2 Rotameters 59 </b>
<b>6.3 Thermal Mass Flow Monitors (MFM) </b> 59
<b>7 Instruments for Analysis of Gas Composition 60 7.1 Paramagnetic Oxygen Analyzers 60 </b>
</div><span class="text_page_counter">Trang 38</span><div class="page_container" data-page="38"><i>List of Symbols and Abbreviations 29 </i>
C concentration (kg m-3)
<i>CPR </i>carbon dioxide production rate (mol <b>s </b><small>- ') </small>
<i>CTR carbon dioxide transfer rate (mol </i><b>s </b><small>- ') </small> G gas flow rate (m3 s-')
<i>H </i> Henry coefficient (L bar mol-')
<i>K </i> equilibrium constant
<i>K L a mass transfer coefficient </i>(s-')
<i>L </i> liquid flow rate (m3 s - ' )
<i>M </i> total mass flow (kg <b><small>s - ' ) </small></b>
<i>n </i> number of moles
<i>OUR oxygen uptake rate (mol </i><b>s-') </b>
<i>OTR oxygen transfer rate (mol </i><b>s-') </b>
<i><b>p </b></i> pressure (bar)
PHB poly-P-hydroxybutyric acid
Q specific reaction rate (mol kg
<i><b>r </b></i> reaction rate (mol L
<i>R </i> <b>gas constant (=0.08314bar L mol-' K - I ) </b>
E electrode G gas phase
i index for component inert inert gas
L liquid phase re1 relative
0 input into the reactor 1 output from the reactor
biomass concentration (g L <b><small>- I ) </small></b>
gas phase molar fraction <small>( - ) </small>
</div><span class="text_page_counter">Trang 39</span><div class="page_container" data-page="39">It is evident from Chapter 1 of this volume of “Biotechnology” that on-line fermentation analysis is of increasing importance because precise control of environmental variables is necessary to optimize process yield and selec- tivity. Most biological products are not vola- tile and are either dissolved in the fermentation fluid, precipitated, or enclosed within the cell membrane boundary. These products are usually difficult or presently impossible to measure on-line in a process environment. This is also true for the biocatalyst itself (cell or enzyme).
In industrial processes each sensor causes risks of infection, whether located in the sterile region or connected to the process with a liq- uid sampling device. This risk does not exist if measurements are made in the effluent gas stream outside the sterile region.
On-line gas analysis is of general interest be- cause almost any biological process using liv- ing organisms involves consumption and pro- duction of gases and volatile compounds. Es- pecially oxygen consumption and carbon dioxide production occur in any aerobic fer- mentation process. Measurement of these reac- tion rates gives direct information about the culture activity. Oxygen consumption rate usually is directly proportional to the heat evo- lution of any aerobic process (COONEY et al., 1969).
Historically, one of the first instruments for gas analysis was the Orsat apparatus (HERON and WILSON, 1959). In this apparatus CO, and
<i><b>O2 are subsequently absorbed in sodium hy- </b></i>
droxide and pyrogallol solutions, and volume changes are detected. Inert gases are deter- mined by difference. CO, production was one of the first biological activities to be quantified in yeast alcohol production. Traditionally, the measurements were made using volumetric methods.
Under normal conditions, where the ideal gas law is valid, gas volume, pressure, and mo- lar amount are directly linked with each other. This makes barometric and volumetric meas- urements very useful. In microbiology the Warburg apparatus is still a very popular method of measuring gas reaction rates. Oxy-
gen and CO, production can be measured si- multaneously by first measuring pressure change and subsequently absorbing CO, in an alkaline solution, then making a final pressure measurement. Volumetric and barometric methods were also further developed to give on-line readings of gas composition (VANA,
1982).
Historically, the results of on-line gas analy- sis have almost exclusively been used to moni- tor fermentations. Since more reliable analyti- cal instruments and on-line data acquisition and computing hard- and software have been developed, it is now possible to use gas analy- sis data together with other measurements to quantitatively characterize fermentation kinet- ics. Cheap and reliable process computer sys- tems, together with increasingly powerful and easy to use software, have dramatically im- proved capabilities.
Gas analysis usually involves measurement of gas flow rates and gas composition. Setting up appropriate mass balances allows evalua- tion of actual production and consumption rates. Today, gas flow rates can be measured with mass flow meters which directly give an electric signal. This facilitates automatic data
<b>evaluation using computers. A whole series </b>of instruments to measure gas composition on- line has been developed. The instruments in- clude paramagnetic oxygen analyzers, infrared absorption photometers, gas chromatographs (GC), mass spectrometers (MS), flame ioniza- tion detectors (FID), amperometric and poten- tiometric sensors, and semiconductor devices. Generally speaking, excluding pH measure- ment, gas analysis is the most widespread and most reliable on-line analysis in industrial fer- mentation processes. It has been applied to the on-line analysis of bacterial, fungal, and high- er cell culture systems. Its potential in animal and plant cell culture has not yet been fully ex- ploited. This is clearly seen by the fact that in a recent review of on-line analysis of animal cell culture the possibility of oxygen uptake rate measurements has not even been mentioned (MERTEN et al., 1986).
</div><span class="text_page_counter">Trang 40</span><div class="page_container" data-page="40"><i><b>Mass Balancing for </b><small>Gas </small>Analysis </i> 31
<i><b>ficient; V, and VL </b></i><b>(L3), </b>gas and liquid volume;
<i><b>r </b></i><b>(MT-'L-3), </b>reaction rate.
The above equations have been written to apply to any component (oxygen, carbon dioxide, ethanol, etc.). They include accumu- lation, convective flow, inter-phase transfer, and reaction terms. Usually there is only one biological reaction term, but a special excep- tion is the case of COz dissociation to yield bi- carbonate. In a batch reactor the liquid flow terms are <i>L 1 =Lo </i><small>= </small><i>0. In </i>a fed-batch culture
<i>L o # L 1 , </i>and in a continuous culture <i>Lo= L,>O. </i>
Here <b>Ct, is the liquid phase concentration </b>
in equilibrium with CG,, and it is calculated by Henry's law
<i>C G I R T = C t , H </i> (3)
Balances which consider gas transfer and gas reaction rates are necessary to characterize the aeration efficiency and to follow biological activity. The same equations can be applied to any component. Well-mixed phases, whose concentrations can be assumed to be uniform, can be described simply, while situations with spatial variation require more complex mod- els. The following general gas balance equa- tions can be written for a well-mixed (tank geometry) system (Fig. 1):
<i>are: Ho, </i><small>= </small>856.9 <i>L bar/mol; Hco, </i><small>= </small>34.01
<i>L bar/mol; HN,= 1484 L bar/mol. The solu- </i>
bility of pure gases in water can also be ex- pressed in liters of gas per liter of water. At 30°C the values are:
dt
(1)
<i>-K,a(Ct, </i><b>--CLJ </b><small>VL </small>
<i>concentrations; G and <b>L (L3T-'), </b></i>gas and liq-
<i>uid flow rates; KLa </i><b>(T-l), </b>mass transfer coef-
It is often convenient to write gas balances in terms of partial pressures instead of concen- trations. Using the ideal gas law
<i>where R </i><small>= </small>0.08205 atm L/mol <b>K </b><small>= </small>0.08314
<b>(bar L/mol K) </b><small>= </small><b>8314 (Pa L/mol K) or its equi- </b>
valent for a flowing system,
<i>where N is moledtime and G is volume/time. </i>
Thus, useful expressions are:
<b><small>Fig. 1. </small></b>Gas transfer <small>in </small>a stirred tank reactor with <small>ni = </small>