6.1 Mixing Equipment. Fig. 6.1 A standard tank with a working volume of 100 M 3 and used for penicillin production
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1 Chapter 6 Mixing Mixing, a physical process which aims at reducing non-uniformities in fluids by eliminating gradients of concentration, temperature, and other properties, is happening within every bioreactor. It is so important that, in a very large extend, decides the performance of a bioreactor. When mixing is beneficial to bioprocesses, for example, the contact of substrate and other nutrients to cells during cell culture, we should try to improve the mixing performance of a bioreactor through all kinds of means. Otherwise, we should avoid its negative effects. 1
2 6.1 Mixing Equipment Fig. 6.1 A standard tank with a working volume of 100 M 3 and used for penicillin production 2
3 Fig. 6.2 Typical configuration of a stirred tank 3
4 Fig. 6.3 Baffle arrangements 4
5 Fig. 6.4 Impeller designs 5
6 Impeller type Fig. 6.5 Viscosity ranges for different impellers 6 Viscosity (centipoise) Anchors propellers Flat-blade turbines paddles Gate anchors Helical screws Helical ribbons 1
7 6.2 Flow Patterns Developed in Agitated Tanks Fig. 6.6 Circular flow in a unbaffled stirred tank 7
8 6.2.1 Radial-flow impeller Fig. 6.7 Flow pattern produced by a radial-flow impeller in a baffled tank 8
9 6.2.2 Axial-flow impeller Fig. 6.8 Pitched-blade turbine 9
10 Fig 6.9 Flow pattern produced by an axial-flow impeller in a baffled tank 10
11 6.3 Mechanism of Mixing As illustrated before, large liquid-circulation loops developed in stirred vessels make mixing performance poor. For mixing to be effective, fluid circulated by the impeller must sweep the entire vessel in a reasonable time. In addition, the velocity of fluid leaving the impeller must be sufficient to carry material into the most remote parts of the tank. Turbulence must also be developed in the fluid; mixing is certain to be poor unless flow in the tank is turbulent. All these factors are important in mixing, which can be described as a combination of three physical processes: distribution, dispersion and diffusion. 11
12 Fig 6.10 Flow pattern developed by a radial-flow impeller 12
13 The process whereby materials are transported to all regions of the vessel by bulk circulation currents is called distribution. Distribution is an important process in mixing, but can be relatively slow. In large tank, the size of the circulation paths is also large and the time taken to traverse them is long; this, together with the regularity of liquid pumping at the impeller, inhibits rapid mixing. Accordingly, distribution is often the slowest step in the mixing process. However, if the rotational speed of the impeller is sufficiently high, superimposed on the distribution process is turbulence. Turbulence flow occurs when fluid no longer travels along streamlines but moves erratically in the form of cross-currents. 13
14 The kinetic energy of turbulent fluid is directed into regions of rotational flow called eddies; masses of eddies of various size coexist during turbulent flow. Large eddies are continuously formed by action of the stirrer; these break down into small eddies which produce even smaller eddies. Eddies, like spinning tops, posses kinetic energy. When the eddies become so small that they can no longer sustain rotational motion, their kinetic energy is dissipated as heat. The process of breaking up bulk flow into smaller and smaller eddies is called dispersion; dispersion facilitates rapid transfer of material throughout the vessel. The degree of homogeneity as a result of dispersion is limited by the size of the smallest eddies which may be formed in a particular fluid. 14
15 This size is given approximately as the Kolmogorov scale of mixing, or scale of turbulence, λ. λ = ( 3 ν ) 1/4 p m (6.1) Within eddies there is little mixing because rotating flow occurs in streamlines. Therefore, to achieve mixing on a scale smaller than the Kolmogorov scale, we must rely on diffusion. Molecular diffusion is generally regarded as a slow process, however, over small distances it can be accomplished quite rapidly. Within eddies of 30~100 μm diameter, homogeneity is achieved in about 1 s for low-viscosity fluids. Consequently, if power input to a stirred vessel produces eddies of this dimension, mixing on a molecular scale is accomplished virtually simultaneously.. 15
16 6.4 Assessing Mixing Effectiveness Mixing time is a useful parameter for assessing mixing efficiency and is applied to characterize bulk flow in fermenters. The mixing time t m is the time required to achieve a given degree of homogeneity starting from the completely segregated state. It can be measured by injecting a tracer into the vessel and following its concentration at a fixed point in the tank. Tracers in common use include acids, bases and concentrated salt solutions; corresponding detectors are ph probes and conductivity cells. Mixing time can also be determined by measuring the temperature response after addition of a small quantity of heated liquid. 16
17 Let us assume a small pulse of tracer is added to fluid in a stirred tank already containing tracer material at concentration C i. When flow in the system is circulation, the tracer concentration measured at some fixed point in the tank will follow a pattern similar to that shown in Figure Before mixing is complete, a relatively high concentration will be detected every time the bulk flow brings tracer to the measurement point. The peaks in concentration will be separated by a period approximately equal to the average time taken for fluid to traverse one bulk circulation loop. In stirred tank this period is called the circulation time t c. After several circulations the desired degree of homogeneity is reached. 17
18 C t c Tracer concentration C f 0.1(C - C ) f i C i Time t m t Fig Concentration response after tracer is injected into a stirred tank 18
19 Definition of the mixing time t m depends on the degree of homogeneity required. Usually, mixing time is defined as the time after which the concentration of tracer differs from the finial concentration C f by less than 10% of the total concentration difference (C f C i ). At t m the tracer concentration is relatively steady and the fluid composition approaches uniformity. For a single-phase liquid in a stirred tank with several baffles and small impeller, there is an approximate relationship between mixing time and circulation time t m = 4t c (6.2) 19
20 We can predict that mixing time in stirred tanks will depend on variables such as the size of the tank and impeller, fluid properties such as viscosity, and stirred speed. The relationship between mixing time and several of these variables has been determined experimentally for different impellers; results for a Rushton turbine in a baffled tank are shown in Fig The dimensionless number N i t m is plotted as a function of the impeller Reynolds number (Re) i. t m is the mixing time based on a 10% deviation from final conditions, and N i is rotational speed of the stirrer. N i t m represents the number of stirrer rotations required to homogenize the liquid. 20
21 Fig 6.12 Variation of mixing time with Reynolds number for a six-blade Rushton turbine in a baffled tank 21
22 At low Reynolds number, N i t m increases significantly with decrease of (Re) i. However, as Reynolds number is increased above about , N i t m approaches a constant value which persists at high (Re) i. For Rushton turbines, this constant value can be estimated using the following relationship. N i t m = (Re) i = 1. 54V 3 D i 2 N i D i ρ μ (6.3) (6.4) 22
23 Example 6.1 Estimation of mixing time A fermentation broth with viscosity 10 2 Pa s and density 1000 kg m 3 is agitated in a 2.7 m 3 baffled tank using a Rushton turbine with diameter 0.5 m and stirred speed 1 s 1. Estimate the mixing time. Solution: From Eq.(6.4): (Re) i = (Re) i > , therefore N i t m is constant and can be calculated from Eq.(6.3): N i t m = 33.3 Therefore: t m = 33.3/1 = 33.3 s 23
24 6.5 Power Requirements for Mixing Usually, electrical power is used to drive impellers in stirred tanks. For a given stirred speed, the power required depends on the resistance offered by the fluid to rotation of the impeller. Average power consumption per unit volume for industrial bioreactors ranges from 10 kw m 3 for small vessels to 1~2 kw m 3 for large vessels. Friction in the stirrer motor gearbox and seals reduces the energy transmitted to the fluid; therefore, the electrical power consumed by stirrer motors is always greater than the mixing power by an amount depending on the efficiency of the drive. Energy costs for operation of stirrers in bioreactors are an important consideration in process economics. 24
25 6.5.1 Ungassed Newtonian Fluids Mixing power for non-aerated fluids depends on the stirrer speed, the impeller diameter and geometry, and properties of the fluid such as density and viscosity. The relationship between these variables is usually expressed in terms of dimensionless numbers such as the impeller Reynolds number (Re) i and the power number N p. N p is defined as: and N p = P 3 ρn i D i 5 (6.5) P = N p ρn i 3 D i 5 (6.6) 25
26 Fig Correlation between power number and Reynolds number for Rushton turbine, paddle and marine propeller without sparging 26
27 Fig 6.14 Correlation between power number and Reynolds number for anchor and helical-ribbon impeller without sparging 27
28 Laminar region: The laminar regime corresponds to (Re) i < 10 for many impellers; for stirrers with very small wall-clearance such as the anchor and helical-ribbon mixer, laminar flow persists until (Re) i = 100 or greater. In the laminar regime: or N p 1/(Re) i P = k 1 μn i2 D i 3 (6.7) Turbulent regime: Power number is independent of Reynolds number in turbulent flow. Therefore: P = N p ρn i3 D i 5 (6.8) 28
29 Table 6.1 Constants in Eq.(6.7) and (6.8) Impeller type k 1, (Re) i = 1 N p, (Re) i = 10 5 Rushton turbine 70 5~6 Paddle 35 2 Marine propeller Anchor Helical ribbon
30 N p for turbines is significantly higher than for most other impellers, indicating that turbines transmit more power to the fluid than other designs. Power required for turbulent flow is independent of the viscosity of the fluid but proportional to fluid density. The turbulent regime is fully developed at (Re) i > 10 3 or 10 4 for most small impellers in baffled vessels. Transition regime: Between laminar and turbulent flow lies the transition regime. Both density and viscosity affect power requirements in this regime. There is usually a gradual transition from laminar to fully-developed turbulent flow in stirred tanks; the flow pattern and Reynolds-number range for transition depend on system geometry. 30
31 Eqs.(6.7) and (6.8) express the strong dependence of power consumption on stirrer diameter and, to a lesser extent, stirrer speed. Small changes in impeller size have a large effect on power requirements, as would be expected from dependency on impeller diameter raised to the third or fifth power. In the turbulent regime, a 10% increase in impeller diameter increases the power required by more than 60%; a 10% increase in stirrer speed rasies the power required by over 30%. 31
32 Example 6.2 Calculation of power requirements A fermentation broth with viscosity 10 2 Pa s and density 1000 kg m 3 is agitated in a 50 m 3 baffled tank using a marine propeller 1.3 m in diameter. The tank geometry is as specified in Figure Calculate the power required for a stirred speed of 4 s 1. Solution: From Eq.(6.4): (Re) i = = From Figure 6.13, flow at this (Re) i is fully turbulent and N p = 0.35 Therefore: P = = kgm 2 s 3 = 83 kw 32
33 6.5.2 Ungassed Non-Newtonian Fluids Impeller Reynolds number based on the apparent viscosity μ a : (Re) i = N i D i μ a 2 For stirred tanks, an approximate relation for pseudoplastic fluids is often used: Substituting Eq.(6.11) into (6.10) gives: ρ (6.9) For power-law fluids: 2 N i D i ρ (Re) i = n K γ r 1 (6.10) γ = kn (6.11) i (Re) i = N 2 n i K k 2 i n-1 D ρ (6.12) 33
34 N P P = ρn 3 5 i D i 50 Newtonian Non-Newtonian (Re) i = ρn i D i μ 2 or ρn i D i μ a 2 Fig Correlation between power number and Renolds number for a Rushton turbine in unaerated fluids 34
35 6.5.3 Gassed Fluids All of the changes in hydrodynamic behavior duo to gassing are not completely understood. Power consumption is strongly controlled by gas-cavities formation; because this process is discontinuous and appears somewhat randomly, reduction in power consumption is typically non-uniform. The random nature of gas dispersion in agitated tanks means that it is difficult to obtain an accurate prediction of power requirements. However, an expression for the ratio of gassed to ungassed power as a function of operating conditions has been obtained. 35
36 p P g 0 = Fg 0.10( N V i ) i N D ( gw V i 4 i 2 / 3 ) 0.20 (6.13) Fig Gas cavities formed behind the blades of a 7.6 cm nine-blade fat-disc turbine in water sparged with air 36
37 6.6 Scale-up of Mixing Systems Design of industrial-scale bioprocess is usually based on the performance of small-scale prototypes. Determining optimum operating conditions at production scale is expensive and timeconsuming; accordingly, it is always better to know whether a particular process will work properly before it is constructed in full size. Ideally, scale-up should be carried out so that conditions in the large vessels are as close as possible to those producing good results in the small vessels. As mixing is an important function of bioreactors, it would seem desirable to keep the mixing time constant on scale-up. Unfortunately, as explained below, the relationship between mixing time and power consumption makes 37
38 this rarely possible in practice. As the volume of mixing vessels is increased, so too are the lengths of the flow paths for bulk circulation. To keep the mixing time constant, the velocity of fluid in the tank must be increased in proportion to the size. As a rough guide, under turbulent conditions the power per unit volume is proportional to the fluid velocity squared: P/V v 2 (6.14) Suppose a cylindrical 1 m 3 pilot-scale stirred tank is scaled up to 100 m 3. If the tanks are geometrically similar, the length of the flow path in the large tank is about 4.5 times that in the small one. Therefore, to keep the same mixing time, fluid velocity in the large tank must be approximately 4.5 times faster. From Eq.(6.14) this would entail a or 20-fold increase in power 38
39 per unit volume. So, if the power input to the 1 m 3 pilot-scale vessel is P, the power required for the same mixing time in the 100 m 3 tank is about 2000 P. This represents an extremely large increase in power, much greater than is economically or technically feasible with most equipment used for stirring. Because the criterion of constant mixing time can hardly ever be applied for scale-up, it is inevitable that mixing time increase with scale. If instead of mixing time, P/V is kept constant during scaleup, mixing time can be expressed to increase in proportion to vessel diameter raised to the power Reduced productivity and performance often accompany scale-up of bioreactors as a result of lower mixing efficiency and subsequent alteration of the physical environment. One way of improving the design procedure is to use scale-down methods. 39
40 The general idea behind scale-down is that small-scale experiments to determine operating parameters are carried out under conditions that can actually be realized, physical and economically, at production scale. For example, if we decide that power input to a large-scale vessel cannot exceed a certain limit, we can calculate the corresponding mixing time and use an appropriate power input to a small-scale bioreactor to stimulate mixing conditions in the large-scale system. With this approach, as long as the flow regime is the same in the small- and large-scale fermenters, there is a better chance that results achieved in the small-scale unit will be reproducible in the larger system. 40
41 6.7 Improving Mixing in Fermenters Sometimes, it is impossible to reduce mixing time by simply raising the power input. So, while increasing the stirrer speed is an obvious way of improving fluid circulation, other techniques may be required. Mixing can be improved by changing the configuration of bioreactors. Baffles should be installed; this is routine for stirrer fermenters and produces greater turbulence. For efficient mixing the impeller should be mounted below the geometric center of the vessel. In standard designs the impeller is located about one impeller diameter, or one-third the tank diameter, above the bottom of the tank. 41
42 Mixing is facilitated when circulation currents below the impeller are smaller than those above; fluid particles leaving the impeller at the same time instant then take different periods of time to return and exchange material. Rate of distribution throughout the vessel is increased when upper and lower circulation loops are asynchronous. Another device for improving mixing is multiple impellers, although this requires an increase in power input. Typical bioreactors used for aerobic culture are tall cylindrical vessels with liquid depths significantly greater than the tank diameter. This design produces a higher hydrostatic pressure at the bottom of the vessel, and gives rising air bubbles a longer contact time with liquid. Effective mixing in tall fermenters requires more than one impeller. 42
43 Fig Multiple impellers in a tall fermenter 43
44 In ungassed systems with spacing between impellers of at least one impeller diameter, the power dissipated by multiple impellers is approximated by the following relationship: P n = np s (6.15) Additional mixing problems can appear in fermenters when material is fed into system during operation. If bulk distribution is slow, fermenters operated continuously or in fed-batch mode may develop highly localized concentrations of substrate or other added material near the feed point. 44
45 This has been observed particularly in large-scale processes for production of SCP (single-cell-protein) from methanol. Because high levels of methanol are toxic to cell growth, biomass yields decrease significantly when mixing of feed material into the broth is slow. Also observed was that during animal cell culture when alkali such as NaOH was used to control ph, high local ph value seriously affected the growth of the cells, although experiment was carried out within a small fermenter. Problems like this can be alleviated by using multiple injection points to aid distribution of added material. It is much less expensive to do this than to increase the fluid velocity and power input (grad). 45
46 6.8 Effect of Rheological Properties on Mixing For effective mixing there must be turbulent conditions in the mixing vessel. Intensity of turbulence is represented by the impeller s Reynolds number. As discussed before for a baffled tank with turbine impeller, once (Re) i falls below criteria turbulence is damped and mixing time increases significantly. (Re) i decreases in direct proportion to increase in viscosity. Accordingly, non-turbulent conditions and poor mixing are likely to occur during agitation of highly viscous fluids. Increasing the impeller speed is an obvious solution, but this requires considerable increase in power consumption and therefore may not be feasible. 46
47 Most non-newtonian fluids in bioprocessing are pseudoplastic. Because the apparent viscosity of these fluids depends on the shear rate, the rheological behavior of many culture broths depends on shear conditions in the fermenters. Pseoduplastic fluids are shear thinning, i.e. their apparent viscosity decreases with increasing shear. Accordingly, in stirred vessels, pseudoplastic fluids have relatively low apparent viscosity in the high-shear zone near the impeller, and relatively high apparent viscosity when the fluid is away from the impeller. As a result, flow patterns similar to that illustrated below can develop. 47
48 Stagnant zones Fig Mixing pattern for pseudoplastic in a stirred tank 48
49 The effects of local fluid thinning in pseudoplastic fluids can be countered by modifying the geometry of the system or impeller design. Stirrers of large diameter are recommended. For turbine impellers, instead of the usual tank-to-impeller diameter ratio of 3:1 used with low viscosity fluids, this ratio is reduced to between 1.6 ~ 2.0. Different impeller designs which sweep the entire volume of the vessel are also recommended. The most common types used for viscous mixing are helical impellers and gate- and paddle-anchors mounted with small clearance between the impeller and tank wall. Mixing with these stirrers is accomplished at low speed without highvelocity streams. Helical agitators have been successfully used to reduce shear damage and improve mixing in viscous cell suspensions. 49
50 Alternative impeller designs such as the helical ribbon and anchor improve mixing in viscous fluids; however their application in fermentaters is only possible when oxygen demand in culture is relatively low. Although large-diameter impellers operating at relatively slow speed give superior bulk mixing, high-shear systems with small, high-speed impellers are preferable for breaking up gas bubbles and promoting oxygen transfer to the liquid. in design of fermenters for viscous cultures, a compromise is usually required between mixing effectiveness and adequate mass transfer (undergrad). 50
51 6.9 Role of Shear in Stirred Tank Mixing in bioreactors must provide the shear conditions necessary to disperse bubbles, droplets and cell flocs. Dispersion of gas bubbles by agitation involves a balance between opposing forces. Shear forces in turbulent eddies stretch and distort the bubbles and break them into small sizes; at the same time, surface tension at the gas-liquid interface tends to restore the bubbles to their spherical shape. In the case of solid material such as cell flocs or aggregates, shear forces in turbulent flow are resisted by the mechanical strength of the particles. While bubbles break-up is required in fermenters to facilitate 51
52 oxygen transfer, disruption of cell is undesirable. Different cell types display different levels of shear sensitivity; insect, mammalian, and plant cells are known to be particularly sensitive to mechanical forces. Bioreacters used for culture for those cells must limit the intensity of shear while still providing adequate mixing and mass transfer. At the present time, the effects of shear on cells are not well understood. Cell disruption is an obvious outcome of high shear forces; however more subtle changes such as retardation of growth and product synthesis, denaturation of extracellular proteins, change in morphology, and thinning of the cell wall, may also occur. Because there is significant spatial variation in shear 52
53 intensity in stirred vessels, the precise shear conditions experienced by cells are poorly defined. There have been many publications addressing the problem of shear damage, especially in insect- and mammalian-cell cultures. Several mechanisms have been considered in terms of their contribution to cell damage: Interaction between cells and turbulent eddies; Collision between cells, collision of cells with the impeller, and collision of cells with stationary surfaces in the vessel; Generation of shear forces in the boundary layers and wakes near solid objects in the reactor, especially the impeller; 53
54 Generation of shear forces as bubbles rise through liquid; and Bursting of bubbles at the liquid surface. In general, when gas bubbles are not present in the liquid, interactions between cells and turbulent eddies are considered most likely to damage cells. However, if the vessel is sparged with air, shear damage can occur at much lower impeller speeds due to shear effects associated with bubbles. 54
55 6.9.1 Interaction Between Cells and Eddies Hydrodynamic effects have been studied mainly with animal cells because shear damage is a significant problem in large-scale culture. Many animal cells used in bioprocessing are anchoragedependent; this means that the cells must be attached to a solid surface for survial. In bioreactors, the surface area required for cell attachment is provided very effectively by microcarrier beads, which range in diameter from 80 ~ 200 μm. Cells cover the surface of the beads which are then suspended in nutrient medium. 55
56 Fig Chinese hamster ovary (CHO) cells attached to microcarriers 56
57 There are many benefits associated with the use of microcarriers; however, a disadvantage is that cells attached to microcarriers cannot easily change position or rotate in response to shear forces in the fluid. This, coulped with the lack of a protective cell wall, make animal cells on microcarriers especially susceptible to shear damage. Interactions between microcarriers and eddies in turbulent flow have the potential to cause mechanical damage to cells. The intensity of shear associated with these interactions is dependent on the relative sizes of the eddies and microcarriers. If the particles are small relative to the eddies, they tend to be captured or entrained in the eddies as shown below. 57
58 (a) (b) Eddy streamlines Microcarrier paths Microcarrier Microcarrier Eddy streamlines High shear zone Fig Eddy-microcarrier interactions 58
59 As fluid motion within eddies is laminar, if the density of the microcarriers is about the same as the suspending fluid, there is little relative motion of the particles. Accordingly, the velocity difference between the fluid streamlines and the microcarriers is small, except for brief periods of acceleration when the bead enters a new eddy. On average, therefore, if the particles are smaller than the eddies, the shear effects of eddy-cell interactions are minimal. If the stirred speed is increased and the average eddy size reduced, interactions between eddies and microcarriers can occur in two possible ways. A single eddy that cannot fully engulf the particle will act on part of its surface and cause the particle to rotate in the fluid; 59
60 this will result in a relatively small level of shear at the surface of the bead. However, much higher shear stress result when several eddies with opposing rotation interact with the particle simultaneously. It has been found experimentally that detrimental effects start to occur when the Kolmogorov scale for eddy size drops below 2/3 ~ 1/2 the diameter of the microcarrier beads. Excessive agitation leads to formation of eddies with size small enough and of sufficient energy to cause damage to the cells. These findings for cell on microcarroers apply also to freely suspended cells; however, because cells are smaller than microcarriers, eddy size causing shear damage are also small. 60
61 Example 6.3 Operating conditions for turbulent shear damage Microcarrier beads 120 μm in diameter are used to culture recombinant CHO cells for hormone production. It is proposed to use a 6-cm turbine impeller to mix the culture in a 3.5 liter stirred tank. Air and carbon dioxide are supplied by flow through the bioreactor headspace. The microcarrier suspension has a density of approximately 1010 kg m 3 and a viscosity of Pa s. Estimate the maximum allowable stirrer speed which avoids turbulent shear damage of the cells. 61
62 Solution: Damage due to eddies is avoided if the Kolmogorov scale remains greater than 2/3 ~ 1/2 the diameter of the beads. Let us determine the stirrer speed required to create eddies with size λ = 2/3 120 = 80 μm = m. The stirrer power producing eddies of this dimension can be calculated: p m = ν λ 3 4 = ( ( ) 4 ) 3 = m 2 s -3 where ν = μ ρ = = m s 62
63 Fluid mass in the impeller zone is roughly equal to ρd i3 where ρ is fluid density and D i is impeller diameter. Therefore, the stirrer power P is equal to p m multiplied by ρd i3 : P = ( ) 3 = kg m 2 s 3 = W N p is about 5 for a turbine impeller operating in the turbulent regime, depending on the geometry of the tank. The stirrer speed corresponding to these conditions can be calculated: N i 3 = P ' N p ρd i 5 = ( ) 5 = 2.89 s -3 63
64 N i = 1.42 s 1 = 85.5 rpm Flow is just turbulent with (Re) i = This analysis indicates that shear damage from turbulent eddies is not expected until the stirrer speed exceeds about 85 rpm. If the culture were sparged with gas, it is possible that shear damage would happen due to other mechanisms, e.g. bursting bubbles. If the viscosity of the liquid is increased, the size of the smallest eddies also increases. Increasing the fluid viscosity should, therefore, reduce shear damage in bioreactors. This effect has been demonstrated by addition of thickening agents to animal-cell growth medium; moderate increase in viscosity have been shown to significantly reduce turbulent cell death. 64
65 6.9.2 Bubble Shear When liquid containing shear-sensitive cells is sparged with air, other damaging mechanisms come into play. From experiments conducted so far, these appear to be associated primarily with bubbles bursting at the surface of the liquid, breakage of the thin bubble film and rapid flow from the bubble rim back into the liquid generate high shear forces capable of damaging certain types of cell. 65
66 Summary After the study of this chapter, you should be: familiar with equipment used for mixing in stirred tanks; able to describe the mechanisms of mixing and their effect on mixing time; able to understand the effects of scale-up on mixing; able to know how liquid properties, gas sparging, impeller size and stirrer speed affect power consumption in stirred vessels; and able to understand how cells can be damaged by shear in stirred fermenters. 66
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