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Non-ideal Flow and Behavior of Real
Bioreactors
• There are two ideal flow patterns, well-mixed and plug flow.
• Although real bioreactors never fully follow these flow patterns, a large
number of fermentation operations approximate these ideal flows with
negligible error.
• However, some cases involving in biological reaction systems provide the
flow patterns which are obviously different from these two ideal
conditions.
• For example, fermenters in cascade which are widely used for ethanol
fermentation process; when bioreactors are scaled up, some stagnant zones
may be developed, especially for high- viscous non-Newtonian biofluids.
• Furthermore, bypassing or short-circuiting flows also exist inside
continuously operated bioreactors.
• The theory of non-ideal flow in bioreacter engineering mainly focuses on
describing all of these phenomena.
Residence Time Distribution
• In an ideal plug-flow or batch reactor, all the elements of material leaving
the reactors have been inside them for exactly the same amount of time.
• The time reaction elements has spent in a reactor is called residence time.
• The ideal plug flow and batch reactors are the only two classes of reactors
in which all the reaction elements present the same residence time.
• In all of the other reactors the elements in the feed spend different times
inside the reactors before they finally leave; that is, there is a distribution of
residence times for the reaction elements within the reactors.
• For example, consider the CSTR; the feed introduced into it at any given
time becomes completely mixed with the material already inside the
reactor.
• In other words, some of the elements entering the CSTR leave it
immediately, because product stream is being continuously withdrawn from
the reactor; at the same time, others maybe remain in the reactor forever
because all the material is never removed from the reactor at one time.
• Residence time distribution (RTD) function (E function) is proposed to
describe residence time presented by different reaction elements inside a reactor,
therefore:
• The direct reason responsible for RTD is mixing within a reactor, thus, RTD can
be used to describe all kinds of non-ideal flow presented within real reactors
mathematically.
Experimental Methods to determine RTD
• In order to characterize the extent of non-ideal flow by
means of RTD, we should like to know how to evaluate
E for any flow.
• For this we resort to the experimental method named
stimulus response technique.
• In this, stimulus is usually a tracer input into the feed,
whereas the response is a time record of the tracer
leaving the vessel.
• Any material that can be detected and which does not
disturb the flow pattern in the vessel can be used as
tracer, and any type of input signal such as a random
signal, a periodic signal, a step signal, or a pulse signal,
etc. may be used.
The F and C curve
• The F Curve:
With no tracer initially present anywhere, impose a step input of tracer of
concentration C0 on the fluid stream entering the vessel. Then a time record of tracer
concentration in the exit stream from the vessel, measured as C/C0, is called the F
curve.
• The C Curve:
With no tracer initially present anywhere, impose an idealized instantaneous pulse of
tracer on the feed stream. Such an input is often called a delta function or impulse.
The normalized response is then called the C curve.
Models for Non-Ideal Flow reactors
• Many types of models can be used to characterize non-ideal flow
presented within real bioreactors.
• One-Parameter Models such as the tanks-in-series model and
the dispersion model are widely used in bioreaction engineering.
• The dispersion model is mainly used to design medium
continuous sterilization processes or some enzyme catalytic
reactions carried out within tubular reactors.
• There are also Two-Parameter Model of CSTR with Bypassing
and Dead Space.
1. The Tanks-in-Series Model
• The RTD will be analyzed from a tracer pulse injected into the
first reactor and gives:
2. CSTR with Biomass Recycle
• Cell concentration in a single CSTR can be increased by recycling biomass
from the product stream back to the bioreactor.
• By this way, much higher rate of substrate conversion and product formation
can be achieved.
• With cell recycling, the critical dilution rate for washout is also increased
allowing greater operating flexibility.
3. The Dispersion Model
4. Two-Parameter Model, CSTR with Bypassing
and Dead Space
• Dead space where no reaction takes place and bypassing flow are
inevitable within a large scale fermenter.
• The model of CSTR with Bypassing and Dead Space can be used to
describe this non-ideal flow existing inside a real bioreactor.
• The total volume of reactor, V, is composed of an ideal CSTR, VS and a
dead zone, VD and a bypass with a volumetric flow rate Fb, as illustrated
below, here we define:

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non-ideal reactors.pptx

  • 1. Non-ideal Flow and Behavior of Real Bioreactors • There are two ideal flow patterns, well-mixed and plug flow. • Although real bioreactors never fully follow these flow patterns, a large number of fermentation operations approximate these ideal flows with negligible error. • However, some cases involving in biological reaction systems provide the flow patterns which are obviously different from these two ideal conditions. • For example, fermenters in cascade which are widely used for ethanol fermentation process; when bioreactors are scaled up, some stagnant zones may be developed, especially for high- viscous non-Newtonian biofluids. • Furthermore, bypassing or short-circuiting flows also exist inside continuously operated bioreactors. • The theory of non-ideal flow in bioreacter engineering mainly focuses on describing all of these phenomena.
  • 2. Residence Time Distribution • In an ideal plug-flow or batch reactor, all the elements of material leaving the reactors have been inside them for exactly the same amount of time. • The time reaction elements has spent in a reactor is called residence time. • The ideal plug flow and batch reactors are the only two classes of reactors in which all the reaction elements present the same residence time. • In all of the other reactors the elements in the feed spend different times inside the reactors before they finally leave; that is, there is a distribution of residence times for the reaction elements within the reactors. • For example, consider the CSTR; the feed introduced into it at any given time becomes completely mixed with the material already inside the reactor. • In other words, some of the elements entering the CSTR leave it immediately, because product stream is being continuously withdrawn from the reactor; at the same time, others maybe remain in the reactor forever because all the material is never removed from the reactor at one time.
  • 3. • Residence time distribution (RTD) function (E function) is proposed to describe residence time presented by different reaction elements inside a reactor, therefore: • The direct reason responsible for RTD is mixing within a reactor, thus, RTD can be used to describe all kinds of non-ideal flow presented within real reactors mathematically.
  • 4. Experimental Methods to determine RTD • In order to characterize the extent of non-ideal flow by means of RTD, we should like to know how to evaluate E for any flow. • For this we resort to the experimental method named stimulus response technique. • In this, stimulus is usually a tracer input into the feed, whereas the response is a time record of the tracer leaving the vessel. • Any material that can be detected and which does not disturb the flow pattern in the vessel can be used as tracer, and any type of input signal such as a random signal, a periodic signal, a step signal, or a pulse signal, etc. may be used.
  • 5.
  • 6. The F and C curve • The F Curve: With no tracer initially present anywhere, impose a step input of tracer of concentration C0 on the fluid stream entering the vessel. Then a time record of tracer concentration in the exit stream from the vessel, measured as C/C0, is called the F curve. • The C Curve: With no tracer initially present anywhere, impose an idealized instantaneous pulse of tracer on the feed stream. Such an input is often called a delta function or impulse. The normalized response is then called the C curve.
  • 7. Models for Non-Ideal Flow reactors • Many types of models can be used to characterize non-ideal flow presented within real bioreactors. • One-Parameter Models such as the tanks-in-series model and the dispersion model are widely used in bioreaction engineering. • The dispersion model is mainly used to design medium continuous sterilization processes or some enzyme catalytic reactions carried out within tubular reactors. • There are also Two-Parameter Model of CSTR with Bypassing and Dead Space.
  • 8. 1. The Tanks-in-Series Model • The RTD will be analyzed from a tracer pulse injected into the first reactor and gives:
  • 9. 2. CSTR with Biomass Recycle • Cell concentration in a single CSTR can be increased by recycling biomass from the product stream back to the bioreactor. • By this way, much higher rate of substrate conversion and product formation can be achieved. • With cell recycling, the critical dilution rate for washout is also increased allowing greater operating flexibility.
  • 11. 4. Two-Parameter Model, CSTR with Bypassing and Dead Space • Dead space where no reaction takes place and bypassing flow are inevitable within a large scale fermenter. • The model of CSTR with Bypassing and Dead Space can be used to describe this non-ideal flow existing inside a real bioreactor. • The total volume of reactor, V, is composed of an ideal CSTR, VS and a dead zone, VD and a bypass with a volumetric flow rate Fb, as illustrated below, here we define: