Lecture 2 Non Ideal Flow
Lecture 2 Non Ideal Flow
Lecture 2 Non Ideal Flow
flow
Review of lecture 1
oReviewed Ideal flow
oFactors that make up the flow pattern:
RTD, state of aggregation, earliness or
lateness of mixing
oExit age distribution
oExperimental methods for finding exit
age distribution
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Relationship between the F and
E Curves
The dimensionless form of the curve is called
the F curve.
It is found by having the tracer concentration
rise from zero to unity
and on differentiating
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𝑑𝐹
= E (8)
𝑑𝑡
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EXAMPLE FINDING THE RTD BY
EXPERIMENT
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Table 1
Time t, min Tracer output
concentration,
(g/L)
0 0
5 3
10 5
15 5
20 4
25 2
30 1
35 0
10
The mean residence time, from pulse
equations is
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12
This area gives the total amount of tracer
introduced.
13 We thus have’
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EXAMPLE 2. FINDING THE E CURVE
FOR LIQUID FLOWING THROUGH A
VESSEL
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(d) The vessel has a strong recirculation of liquid, probably
induced by the rising bubbles.
The Convolution Integral
• A convolution is an integral that
expresses the amount of overlap
of one function g as it is shifted
over another function f.
• It therefore "blends" one function
with another.
• Suppose we introduce into a
vessel a one-shot tracer signal Cin
versus t as shown in the Fig. below
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• In passing through the vessel the signal will
be modified to give an output signal Cout
versus t.
• Since the flow with its particular RTD is
responsible for this modification let us
relate Cin, E, and C,.
• Focus attention on tracer leaving at time
about t.
• This is shown as the narrow rectangle B in
the figure above.
• We may then write
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the tracer which enters t' seconds earlier than t as the narrow
rectangle A. In terms of this rectangle the above equation may be
written
We say that Coutis the convolution of E with Cin and we write concisely
Modification of an input tracer signal Cin on passing
through three successive regions.
Application of These Tools.
To illustrate the uses of these mathematical tools consider three
independent flow units a, b, and c, which are closed and
connected in series
Problem 1. If the input signal Cin is measured and the exit age
distribution functions Ea, Eb, and Ec are known, then C1 is the
convolution of Ea with Cin and so on, thus
(a) the reactant starts at high concentration and reacts away rapidly because.
(b) the fluid drops immediately to a low concentration.
Since the rate of reaction drops more rapidly than does the concentration you will end
up with a lower conversion.
For macrofluids, imagine little clumps of fluid staying for different lengths
of time in the reactor (given by the E function). Each clump reacts away
as a little batch reactor, thus fluid elements will have different
compositions.
So the mean composition in the exit stream will have to account for these
two factors, the kinetics and the RTD. In words, then
which says that the pulse occurs at t = to, as seen in Fig. The
two
properties of this function which we need to know are
EXAMPLE 4: CONVERSION IN REACTORS HAVING
NON-IDEAL FLOW
Find the fraction of reactant unconverted in the real reactor and compare
this with the fraction unconverted in a plug flow reactor of the same
size. Using a reaction time of 15 minutes.
For the plug flow reactor with negligible density change we have
and with
For the real reactor the fraction unconverted, given by above Eq. for macrofluids,
is found in Table. Hence the fraction of reactant unconverted in the real reactor
From the table we see that the unconverted
material comes mostly from the early
portion of the E curve.
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• Note that since this is a first-order reaction we can treat it as a
microfluid, or a macrofluid, whatever we wish.
• In this problem we solved the plug flow case as a microfluid, and
we solved the non-ideal case as a macrofluid.
E= CAo/Area
Area = 2x2 =4
E = 2/4 = 0.5
Next Lecture:
Heterogeneous processes
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