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Mass Transfer
Mass transfer occurs in mixtures containing local
concentration variation
Mass is transferred from one location to another
under the influence of a concentration difference or
concentration gradient in the system
For example, in bioprocessing, the supply of oxygen
in bioreactors for aerobic culture
Concentration of oxygen at the surface of air bubbles
is high compared with the rest of the fluid, therefore
this concentration difference promotes oxygen
transfer from bubbles into the medium
Molecular Diffusion
Molecular diffusion is the movement of component
molecules in a mixture under the influence of a
concentration difference in the system
It occurs in the direction required to destroy the
concentration difference
If the gradient is maintained by constantly supplying
material to the region of high concentration and
removing it from region of low concentration,
diffusion will be continue
Diffusion Theory (cont’d)
In the previous figure, concentration CA varies from
CA1 to CA2 is a function of distance y
Molecules A will diffuse away from the region of high
concentration until eventually the whole system
acquires uniform composition
Diffusion Theory (cont’d)
According to Fick’s Law of diffusion, which states
that mass flux is proportional to the concentration
gradient:
dy
dCD
a
NJ A
ABA
A
where:
JA = mass flux of component A
NA = rate of mass transfer of component A
a = is are across which mass transfer occurs
DAB = binary diffusion coefficient or diffusion of component A
CA – concentration of component A
y = distance
DCA/dy = concentration gradient
Role of Diffusion in Bioprocessing Fluid mixing is carried out in most industrial processes where mass
transfer takes place
Areas of bioprocessing in which diffusion plays major role aredescribe below:
Scale of mixing – Turbulence in fluids produces bulk mixing on ascale equal to the smallest eddy size. Within the smallest eddies,flow is largely streamline so that further mixing must occur bydiffusion of fluid components.
Solid phase reaction – in biological systems, reaction aresometimes mediated by catalyst in solid form. When cells or enzymemolecules are clumped together into a solid particle, substrates mustbe transported into the solid before reaction can take place.
Mass transfer across a phase boundary – mass transfer betweenphases occurs often in bioprocessing. Oxygen transfer from gasbubbles to fermentation broth, penicillin recoveryfrom aqueous toorganic fluid, and glucose transfer from liquid medium into mouldpellets are typical examples.
Gas-Liquid Mass Transfer
It is important in bioprocessing because of the requirement for oxygen in aerobic fermentation.
From the figure beside, assume A is transferred from gas phase into the liquid.
The concentration of A in the liquid bulk is CAL; at the interface is CALi
whereas in gas CAG in bulk and CAGi at the interface.
Concentration gradients for gas-
liquid mass transfer
Gas-Liquid Mass Transfer (cont’d)
The rate of mass transfer of A through the gas boundary layer is:
AGiAGGAG CCakN
The rate of mass transfer of A through the liquid boundary layer is:
ALALiLAL CCakN
For some gasses equilibrium concentration in the gas phase is a linear function of liquid concentration, where m is distribution factor:
m
CC AGi
ALi
Gas-Liquid Mass Transfer (cont’d)The equilibrium relationship between gas phase and liquid phase at steady state are:
ALAG
LG
A
ALAG
LG
A
Cm
C
akamkN
mCCak
m
akN
11
1
The overall gas-phase mass transfer coefficient KG:
aK
m
akaK LGG
11
The overall liquid-phase mass transfer coefficient KL:
aKamkaK LGL
111
Gas-Liquid Mass Transfer (cont’d)The rate of mass transfer in gas-liquid systems can therefore be expressed in:
AL
AGLA C
m
CaKN
The equation is usually expressed in equilibrium, where mCAL is equal to C*AG, and (CAG/m) is equal to C*AL. Therefore the equation become:
ALALLA
AGAGGA
CCaKN
CCaKN
*
*
Gas-Liquid Mass Transfer (cont’d)When solute A is very soluble in liquid (e.g ammonia to water), the liquid side resistance is small compared with that posed by the gas interfacial film. Therefore, KGa is approximately equal to kGa due liquid side resistance is small and kLa is large:
*
AGAGGA CCakN
Conversely, if solute A is poorly soluble in liquid (e.g
oxygen in aqueous solution), the liquid phase mass
transfer ressistance dominates and kGa >>kLa,
therefore KLa approximately equal to kLa:
ALALLA CCaKN *
Oxygen Transfer in Cell Cultures
Cell in aerobic culture take up oxygen from the
liquid.
Therefore, the mass transfer of oxygen from gas to
liquid is importance, especially at high densities
when cell growth is likely to be limited by availablity
of oxygen in the medium.
The difference (C*AL-CAL) between the maximum
possible and actual oxygen concentration represent
concentration-difference driving force for mass
transfer.
Oxygen Transfer in Cell Cultures (cont’d)
where:
NA = rate of oxygen per unit volume (gmol m-3 s-1)
kL = liquid phase mass transfer coefficient (ms-1)
a= gas-liquid interfacial area per unit volume fluid (m2 m-3)
CAL = the oxygen concentration in broth (gmol m-3)
C*AL = the oxygen concentration in broth in equilibrium with
gas phase (gmol m-3)
ALALLA CCaKN *
Oxygen Transfer in Cell Cultures (cont’d)
The solubility of oxygen in aqueous solution at
ambient temperature and pressure is about 10 ppm
This amount of oxygen is quickly consumed in
aerobic cultures and must be constantly changed by
sparging
Low solubility of oxygen will show the difference
(C*AL-CAL) is very small
Factors Affecting Cellular Oxygen
The rate at which oxygen is consumed by cells in
bioreactors determines the rate which it must be
transferred from gas to liquid
Many factors influence oxygen demand, the most
important of these are:
Cell species
Culture growth phase
Nature of the carbon source in the medium
The concentration of cell increases during course of
batch culture and the total rate of oxygen uptake is
proportional to the no. of cell present
Factors Affecting Cellular Oxygen (cont’d)
The rate of oxygen consumption per cell also known
as oxygen uptake rate (OUR):
xqQ OO where:
Qo = oxygen uptake rate per volume broth (gL-1 s-1)
qo = specific oxygen transfer rate (gg-1 s-1)
Factors Affecting Cellular Oxygen (cont’d)
The demand of an organism for oxygen depends
primarily on the biochemical nature of the cell and its
nutritional environment.
To eliminate oxygen limitation and allow cell
metabolism to function at its fastest, the dissolved
oxygen concentration at every point in the bioreactor
must be above Ccrit.
The value of Ccrit depends on the organism, but
under average operation it usually falls between 5%-
10% of air saturation.
Oxygen Transfer from Gas Bubble to Cell
(cont’d)
In aerobic fermentation, oxygen molecules must overcome a series of transport resistance before being utilized by the cell
Eight mass transfer steps involved in transport of oxygen from the interior of gas bubbles to the site of intracellular reaction
1. transfer from the interior of the bubble to the gas-liquid interface
2. movement across the gas-liquid interface
3. diffusion through the relatively stagnant liquid film surrounding the bubbles
4. transport through the bulk liquid
5. diffusion through the relatively stagnant liquid film surrounding the cells
6. movement across the liquid-cell interface
7. if the cells in a floc, clump or solid particle, diffusion through the solid to the individual cell
8. transport through the cytoplasm to the site of reaction
Oxygen Transfer from Gas Bubble to Cell
(cont’d)
For most bioreactors, the analysis of mass transfer is as below1. Transfer through the bulk gas phase in the bubble is relative fast
2. The gas-liquid interface itself contributes negligible resistance
3. The liquid film around the bubbles is the major resistance to oxygen transfer
4. In a well-mixed bioreactor, concentration gradients in the bulk liquid are minimized and mass transfer resistance in this region is small
5. Because the single cells are much smaller than gas bubbles, the liquid film surrounding each cell is much thinner than around the bubbles and its effect on mass transfer can generally neglected
6. Resistance at the cell liquid interface is generally neglected
7. When cells are in clumps, intraparticle resistance is likely to be significant as oxygen has to diffuse through the solid pellet to reach the interior cells. The magnitude of resistance depends on the size of the clumps
8. Intracellular oxygen transfer resistance is negligible because of small distance involved
Oxygen Transfer from Gas Bubble to Cell
(cont’d)
When cell are dispersed in the liquid and the bulk fermentation broth is well mixed, the major resistance to oxygen transfer is the liquid film surrounding the gas bubbles
Therefore, transport through this film becomes rate limiting step and controls the overall mass transfer rate
At steady state, no accumulation of oxygen at any location in the bioreactor, therefore rate of oxygen transfer from bubbles must be equal to rate of oxygen consumption by cells:
xqCCaK OALALL *
Oxygen Transfer from Gas Bubble to Cell
(cont’d)
If kLa is small, the ability of the bioreactor to deliver
oxygen is limited
The maximum cell concentration can be supported
by mass transfer function of the bioreactor is:
O
ALL
q
Cakx
*
max
If xmax is lower than the cell concentration required
in fermentation process, kLa must be improved
Another important parameter is the minimum kLa
required to maintain CAL>Ccrit in bioreactor
critAL
O
critLCC
xqak
*
Oxygen Transfer in Bioreactor
Rate of oxygen transfer in fermentation broth is influences by several physical and chemical factors that change the value of kL of value of a or driving force (C*AL-CAL)
kL in fermentation liquid is usually in the range of 3-4 x 10-4 ms-1 for bubbles greater than 2-3 mm diameter, but it can be reduced to 1x10-4 ms-1 if smaller bubbles produced
If substantial improvement in mass transfer rate is required, it is more productive to increase the interfacial area, a
In production scale bioreactor, value of kLa is typically in the range of 0.02s-1 to 0.25s-1
Bubbles
Bubble behavior strongly affects the value of kLa,
which some may affect mainly on kL, whereas some
changes interfacial area, a
Bubble in lab-scale bioreactor frequently subjected
to severe distortion as they interact with turbulent
liquid current, whereas bubble in industrial stirred
tanks spend large proportion of their time floating
free and impeded through the liquid after initial
dispersion at impeller
The most important property of air bubbles in
bioreactor is their size
Bubbles (cont’d)
Advantages of small bubbles such as:
Can produce high level of gas dispersion by providing
more interfacial area, a
Since it has slow rise velocities, they can stay in the liquid
longer, allowing more time for oxygen to dissolve
Therefore, small bubble create high gas hold-up
defined as fraction of fluid volume in the reactor
occupied by gas:
GL
G
VV
V
where
ξ=gas hold upVG = volume of gas bubblesVL= volume of liquid
Bubbles (cont’d)
Disadvantages of small bubbles
Bubbles <<1mm can become nuisance in bioreactor where
oxygen concentration equilibrates with that in the medium
within seconds, so that the gas hold-up no longer reflects the
capacity of the system for mass transfer
Small bubble in non-Newtonian broth (viscous) will remain
lodged for long periods due to its velocity is reduced through
time
Bubble size also affect the value of kL
Bubble with diameter less than 2-3 mm, the surface tension
effects dominate the behaviour of the bubble surface
For bubble with diameter >3 mm, it can develop internal and
relatively mobile surface, depending on liquid properties