Lecture 20
description
Transcript of Lecture 20
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Chemical Reaction Engineering (CRE) is the field that studies the rates and mechanisms of
chemical reactions and the design of the reactors in which they take place.
Lecture 20
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0
0 0 0 0
i iH H
sysi i i i i i S
dEF U PV F U PV Q W
dt
0 0sys
i i i i S
dEF H FH Q W
dt
Last Lecture Energy Balance Fundamentals
2
Substituting for W
000 iiiiS HFHFWQ
dtdE
WQEFEF sysiiii 00
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Web Lecture 20Class Lecture 16-Thursday 3/14/2013
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Reactors with Heat ExchangeUser friendly Energy Balance DerivationsAdiabaticHeat Exchange Constant Ta
Heat Exchange Variable Ta Co-currentHeat Exchange Variable Ta Counter Current
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The feed consists of both - Inerts I and Species A with the ratio of inerts I to the species A being 2 to 1.
A B
FA0
FI
Elementary liquid phase reaction carried out in a CSTR
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Adiabatic Operation CSTR
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Adiabatic Operation CSTR
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Assuming the reaction is irreversible for CSTR, A B, (KC = 0) what reactor volume is necessary to achieve 80% conversion?If the exiting temperature to the reactor is 360K, what
is the corresponding reactor volume?Make a Levenspiel Plot and then determine the PFR
reactor volume for 60% conversion and 95% conversion. Compare with the CSTR volumes at these conversions.Now assume the reaction is reversible, make a plot of
the equilibrium conversion as a function of temperature between 290K and 400K.
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1) Mole Balances:exitA
0A
rXFV
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CSTR: Adiabatic Example
A B
FA0
FI
(exothermic)
𝑇=?
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T1
T1
RHexpKK
ekk
KCCkr
2
Rx1CC
T1
T1
RE
1
C
BAA
1
2) Rate Laws:
XCC
X1CC
0AB
0AA
3) Stoichiometry:
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CSTR: Adiabatic Example
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4) Energy Balance Adiabatic, ∆Cp=0
X
36164000,20300X
182164000,20300T
CCXHT
CXHTT
IAi PIP
Rx0
Pi
Rx0
X 100300T
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CSTR: Adiabatic Example
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Irreversible for Parts (a) through (c)
)K (i.e., X1kCr C0AA
(a) Given X = 0.8, find T and V
Given X Calc T Calc k Calc rACalc V
Calc KC(if reversible)
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CSTR: Adiabatic Example
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A
0A
0A
0A
exitA
0A
dm 82.28.01281.3
8.05rXFV
81.33801
2981
989.1000,10exp1.0k
K3808.0100300T
X1kCXF
rXFV
Given X, Calculate T and V
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CSTR: Adiabatic Example
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(b) VrkTXGiven CalcA
CalcCalcCalc
CK Calc(if reversible)
3
1
0
05.24.0283.1
6.05min83.1
6.0100
300360
ble)(Irreversi 1
dmV
k
TX
KTXkCr AA
Given T, Calculate X and V
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CSTR: Adiabatic Example
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(c) Levenspiel Plot
X1kCF
rF
0A
0A
A
0A
Choose X Calc T Calc k Calc rACalc
FA 0
rA
X100300T
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CSTR: Adiabatic Example
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(c) Levenspiel Plot
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CSTR: Adiabatic Example
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CSTR X = 0.95 T = 395 K
0
5
10
15
20
25
30
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
X
-Fa0
/Ra
CSTR 60%
CSTR X = 0.6 T = 360 K
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CSTR: Adiabatic Example
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PFR X = 0.6
PFR X = 0.95
0
5
10
15
20
25
30
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
X
-Fa0
/Ra
PFR 60%
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CSTR: Adiabatic Example
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CSTR X = 0.6 T = 360 V = 2.05 dm3
PFR X = 0.6 Texit = 360 V = 5.28 dm3
CSTR X = 0.95 T = 395 V = 7.59 dm3
PFR X = 0.95 Texit = 395 V = 6.62 dm3
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CSTR: Adiabatic Example - Summary
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dVdF
HdVdH
FdV
HFd
TTUadV
HFd
VTTUaHFHF
ii
ii
ii
aii
aVViiVii
0
0
Energy Balance in terms of Enthalpy
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RPiii TTCHH 0
dVdTC
dVdH
Pii
xRii
AiiPiiii
HH
rHdVdTCF
dVHFd
PFR Heat Effects
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Aiii rr
dVdF
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0
TTUarH
dVdTFC aARiPi
aARPii TTUarHdVdTCF
Pii
aAR
CFTTUarH
dVdT
19 Need to determine Ta
PFR Heat Effects
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Heat Exchange:
iPi
aRxA
CFTTUaHr
dVdT
)B16( CF
TTUaHrdVdT
iPi0A
aRxA
20Need to determine Ta
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Energy Balance:
Adiabatic (Ua=0) and ΔCP=0
)A16( C
XHTTiPi
Rx0
Heat Exchange Example: Case 1 - Adiabatic
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A. Constant Ta e.g., Ta = 300K
)17( 0 , CTTV
CmTTUa
dVdT
aoaP
aa
cool
B. Variable Ta Co-Current
C. Variable Ta Counter Current Guess ? 0
aP
aa TVCm
TTUadVdT
cool
Guess Ta at V = 0 to match Ta0 = Ta0 at exit, i.e., V = Vf
User Friendly Equations
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Coolant Balance:
In - Out + Heat Added = 0
0
0
aC
C
aVVCCVCC
TTUadVdH
m
TTVUaHmHm
Heat Exchanger Energy Balance Variable Ta Co-current
dVdTC
dVdH
TTCHH
aPC
C
raPC0CC
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0 0 , aa
PCC
aa TTVCm
TTUadVdT
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In - Out + Heat Added = 0
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0
0
PCC
aa
aC
C
aVCCVVCC
CmTTUa
dVdT
TTUadVdH
m
TTVUaHmHm
Heat Exchanger Energy Balance Variable Ta Co-current
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Elementary liquid phase reaction carried out in a PFR
The feed consists of both inerts I and species A with the ratio of inerts to the species A being 2 to 1.
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FA0
FI
Tacm Heat Exchange
Fluid
A BT
Heat Exchanger – ExampleCase 1 – Constant Ta
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T1
T1
REexpkk )3(
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T1
T1
RHexpKK )4(
2
Rx2CC
FrdVdX )1( 0AA
1) Mole Balance:
C
BAA K
CCkr )2(2) Rate Laws:
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Heat Exchanger – ExampleCase 1 – Constant Ta
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0CP
6 XCC
5 X1CC
0AB
0AA
3) Stoichiometry:
9 CCC PIIPAPii
8 k1
kXC
Ceq
4) Heat Effects: 7 0
PiiA
aAR
CFTTUarH
dVdT
Heat Exchanger – ExampleCase 1 – Constant Ta
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Parameters:
A
IPIPAA
AaC
R
rrateCCC
FTUakkTTREH
, , , ,, , , , ,
, , , , ,
0
021
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Heat Exchanger – ExampleCase 1 – Constant Ta
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Pii
rg
CFQQ
dVdT
Heat removed
Heat generated
XCCFCXFCF PiPii0APiii0APii
XCCFTTUarH
dVdT
PPiiA
aAR
0
PFR Heat Effects
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Energy Balance:
Adiabatic and ΔCP=0Ua=0
)A16( C
XHTTiPi
Rx0
Additional Parameters (17A) & (17B)
IAi PIPPi0 CCC ,T 30
Mole Balance:
dXdV rAFA 0
Heat Exchanger – ExampleCase 2 – Adiabatic
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Adiabatic PFR
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Find conversion, Xeq and T as a function of reactor volume
V
rate
V
T
V
XX
Xeq
Example: Adiabatic
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iPi
aRxA
CFTTUaHr
dVdT
)B16( CF
TTUaHrdVdT
iPi0A
aRxA
Heat Exchange
33Need to determine Ta
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A. Constant Ta (17B) Ta = 300K
Ua ,C ,TiPia
Additional Parameters (18B – (20B):
)17( 0 CTTVCm
TTUadVdT
aoaP
aa
cool
B. Variable Ta Co-Current
C. Variable Ta Countercurrent
? 0
aP
aa TVCm
TTUadVdT
cool
Guess Ta at V = 0 to match Ta0 = Ta0 at exit, i.e., V = Vf
User Friendly Equations
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Coolant balance:
In - Out + Heat Added = 0
0
0
aC
C
aVVCCVCC
TTUadVdHm
TTVUaHmHm
dVdTC
dVdH
TTCHH
aPC
C
raPC0CC
All equations can be used from before except Ta parameter, use differential Ta instead, adding mC and CPC
Heat Exchange Energy Balance Variable Ta Co-current
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0 0 , aa
PCC
aa TTVCm
TTUadVdT
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In - Out + Heat Added = 0
All equations can be used from before except dTa/dV which must be changed to a negative. To arrive at the correct integration we must guess the Ta value at V=0, integrate and see if Ta0 matches; if not, re-guess the value for Ta at V=0
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PCC
aaa
CC
aVCCVVCC
CmTTUa
dVdTTTUa
dVdHm
TTVUaHmHm
0
0
Heat Exchange Energy Balance Variable Ta Co-current
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0HFHFdWTTUaii0i0ia
W
0 B
0dWdHFH
dWdF0TTUa i
iii
aB
Differentiating with respect to W:
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Derive the user-friendly Energy Balance for a PBR
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Aii
i rrdWdF
Mole Balance on species i:
T
TPiRii
R
dTCTHH
Enthalpy for species i:
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Derive the user-friendly Energy Balance for a PBR
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Differentiating with respect to W:
dWdTC0
dWdH
Pii
0dWdTCFHrTTUa
PiiiiAaB
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Derive the user-friendly Energy Balance for a PBR
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0dWdTCFHrTTUa
PiiiiAaB
THH Rii XFF ii0Ai
Final Form of the Differential Equations in Terms of Conversion:
A:
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Derive the user-friendly Energy Balance for a PBR
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Final form of terms of Molar Flow Rate:
Pii
AaB
CF
HrTTUa
dWdT
B: T,Xg
Fr
dWdX
0A
A
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Derive the user-friendly Energy Balance for a PBR
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The rate law for this reaction will follow an elementary rate law.
DCBA
C
DCBAA K
CCCCkr
Where Ke is the concentration equilibrium constant. We know from Le Chaltlier’s law that if the reaction is exothermic, Ke will decrease as the temperature is increased and the reaction will be shifted back to the left. If the reaction is endothermic and the temperature is increased, Ke will increase and the reaction will shift to the right.
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Reversible Reactions
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RTKK P
C
Van’t Hoff Equation:
2
RPRR2
RP
RTTTCTH
RTTH
dTKlnd
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Reversible Reactions
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For the special case of ΔCP=0
Integrating the Van’t Hoff Equation gives:
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RR1P2P T
1T1
RTHexpTKTK
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Reversible Reactions
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endothermic reaction
exothermic reaction
KP
T
endothermic reaction
exothermic reaction
Xe
T
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Reversible Reactions
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End of Lecture 20