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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 4
Lecture 4
2
 Block 1
 Mole Balances
 Size CSTRs and PFRs given –rA=f(X)
 Block 2
 Rate Laws
 Reaction Orders
 Arrhenius Equation
 Block 3
 Stoichiometry
 Stoichiometric Table
 Definitions of Concentration
 Calculate the Equilibrium Conversion, Xe
Chapter 4
Reactor Differential Algebraic Integral

V 
FA 0X
rA
CSTR

FA0
dX
dV
 rA  

X
A
A
r
dX
F
V
0
0
PFR
V
r
dt
dX
N A
A 

0
0
0  

X
A
A
V
r
dX
N
t
Batch
X
t
FA 0
dX
dW
  
rA  


X
A
A
r
dX
F
W
0
0
PBR
X
W
3
Reactor Mole Balances Summary
in terms of conversion, X
Review Lecture 2
Levenspiel Plots
4

FA 0
rA

X
Review Lecture 2
5
PFR
Review Lecture 2
6
Reactors in Series
reactor
first
to
fed
A
of
moles
i
point
to
up
reacted
A
of
moles
Xi 
Only valid if there are no side streams
Review Lecture 2
7
Reactors in Series
Review Lecture 2
8
 
i
A C
g
r 

Step 1: Rate Law
   
X
h
Ci 
Step 2: Stoichiometry
 
X
f
rA 

Step 3: Combine to get
Two steps to get

rA  f X
 
Review Lecture 2
Building Block 2: Rate Laws
9
Power Law Model:


B
A
A C
kC
r 

β
α
β
α


Order
Rection
Overall
B
in
order
A
in
order
C
B
A 3
2 

A reactor follows an elementary rate law if the reaction
orders just happens to agree with the stoichiometric
coefficients for the reaction as written.
e.g. If the above reaction follows an elementary rate law
2nd order in A, 1st order in B, overall third order
B
A
A
A C
C
k
r 2


Review Lecture 3
Arrhenius Equation
10
E = Activation energy (cal/mol)
R = Gas constant (cal/mol*K)
T = Temperature (K)
A = Frequency factor (same units as rate constant k)
(units of A, and k, depend on overall reaction order)
RT
E
Ae
k 


T  k A
T 0 k 0
A 1013
T
k
Review Lecture 3
Reaction Engineering
11
These topics build upon one another
Mole Balance Rate Laws Stoichiometry
Review Lecture 3
Algorithm
12
 
i
A C
g
r 

Step 1: Rate Law
   
X
h
Ci 
Step 2: Stoichiometry
 
X
f
rA 

Step 3: Combine to get
How to find  
X
f
rA 

Review Lecture 3
Building Block 3: Stoichiometry
13
We shall set up Stoichiometry Tables using species
A as our basis of calculation in the following
reaction. We will use the stoichiometric tables to
express the concentration as a function of
conversion. We will combine Ci = f(X) with the
appropriate rate law to obtain -rA = f(X).
A is the limiting reactant.
D
a
d
C
a
c
B
a
b
A 


Chapter 4
Stoichiometry
14
NA  NA0 NA0X
NB = NB0 -
b
a
NA0X = NA0
NB0
NA0
-
b
a
X
æ
è
ç
ö
ø
÷
For every mole of A that reacts, b/a moles of B react. Therefore
moles of B remaining:
Let ΘB = NB0/NA0
Then:








 X
a
b
N
N B
A
B 0
NC  NC 0 
c
a
NA 0X  NA 0 C 
c
a
X






Chapter 4
Batch System - Stoichiometry Table
15
Species Symbol Initial Change Remaining
B B NB0=NA0ΘB -b/aNA0X NB=NA0(ΘB-b/aX)
A A NA0 -NA0X NA=NA0(1-X)
Inert I NI0=NA0ΘI ---------- NI=NA0ΘI
FT0 NT=NT0+δNA0X
Where:
0
0
0
0
0
0
0
0
0
0
A
i
A
i
A
i
A
i
i
y
y
C
C
C
C
N
N







1




a
b
a
c
a
d

and
C C NC0=NA0ΘC +c/aNA0X NC=NA0(ΘC+c/aX)
D D ND0=NA0ΘD +d/aNA0X ND=NA0(ΘD+d/aX)
δ = change in total number of mol per mol A reacted
Chapter 4
Stoichiometry Constant Volume Batch
16
Note: If the reaction occurs in the liquid phase
or
if a gas phase reaction occurs in a rigid (e.g. steel)
batch reactor

V V0
Then

CA 
NA
V

NA 0 1 X
 
V0
 CA 0 1 X
 
CB 
NB
V

NA 0
V0
B 
b
a
X





 CA 0 B 
b
a
X






etc.
Chapter 4
Stoichiometry Constant Volume Batch
17
Suppose

rA  kACA
2
CB
Batch: 0
V
V 
-rA = kACA0
3
1- X
( )
2
QB -
b
a
X
æ
è
ç
ö
ø
÷
Equimolar feed: 1

B
Stoichiometric feed:
a
b
B 

Chapter 4
Stoichiometry Constant Volume Batch
18
 
X
f
rA 

and we have
If B
A
A
A C
C
k
r 2

 , then
  









 X
a
b
X
C
r B
A
A
2
3
0 1 Constant Volume Batch
A
r

1
X
Chapter 4
Batch Reactor - Example
19
Consider the following elementary reaction with
KC=20 dm3/mol and CA0=0.2 mol/dm3.
Find Xe for both a batch reactor and a flow reactor.
Calculate the equilibrium conversion for gas phase
reaction, Xe .









C
B
A
A
A
K
C
C
k
r
2
B
A 
2
Chapter 4
Batch Reactor - Example
20
Step 1:
0
A
A
N
V
r
dt
dX 

3
0 2
.
0 dm
mol
CA 
mol
dm
KC
3
20

Step 2: rate law: B
B
2
A
A
A C
k
C
k
r 


Calculate Xe
B
A
C
k
k
K 









C
B
2
A
A
A
K
C
C
k
r
Chapter 4
Batch Reactor - Example
21
Symbol Initial Change Remaining
B 0 ½ NA0X NA0 X/2
A NA0 -NA0X NA0(1-X)
Totals: NT0=NA0 NT=NA0 -NA0 X/2
@ equilibrium: -rA=0
C
Be
Ae
K
C
C 
 2
0
Ke 
CBe
CAe
2 CAe 
NAe
V
 CA0 1 Xe
 
CBe  CA0
Xe
2
Chapter 4
Batch Reactor - Example
22
Species Initial Change Remaining
A NA0 -NA0X NA=NA0(1-X)
B 0 +NA0X/2 NB=NA0X/2
NT0=NA0 NT=NA0-NA0X/2
Solution:
2
Ae
Be
C
C
C
K 










C
Be
2
Ae
A
A
K
C
C
k
0
r
At equilibrium
0
V
V 
2
/
B
A 
Stoichiometry:
Constant Volume:
Batch
Chapter 4
Batch Reactor - Example
23
 
   2
e
0
A
e
2
e
0
A
e
0
A
e
X
1
C
2
X
X
1
C
2
X
C
K




 
   8
2
.
0
20
2
X
1
X
C
K
2 2
e
e
0
A
e 



Xeb 0.703
Chapter 4
Flow System – Stoichiometry Table
24
A A FA0 -FA0X FA=FA0(1-X)
Species Symbol Reactor Feed Change Reactor Effluent
B B FB0=FA0ΘB -b/aFA0X FB=FA0(ΘB-b/aX)
i 
Fi0
FA 0

Ci00
CA 00

Ci0
CA 0

yi0
yA 0
Where:
Chapter 4
Flow System – Stoichiometry Table
25
Species Symbol Reactor Feed Change Reactor Effluent
0
A
0
i
0
A
0
i
0
0
A
0
0
i
0
A
0
i
i
y
y
C
C
C
C
F
F







Where:
Inert I FI0=A0ΘI ---------- FI=FA0ΘI
FT0 FT=FT0+δFA0X
C C FC0=FA0ΘC +c/aFA0X FC=FA0(ΘC+c/aX)
D D FD0=FA0ΘD +d/aFA0X FD=FA0(ΘD+d/aX)
1
a
b
a
c
a
d





and

 A
A
F
C
Concentration – Flow System
Chapter 4
26
Species Symbol Reactor Feed Change Reactor Effluent
A A FA0 -FA0X FA=FA0(1-X)
B B FB0=FA0ΘB -b/aFA0X FB=FA0(ΘB-b/aX)
C C FC0=FA0ΘC +c/aFA0X FC=FA0(ΘC+c/aX)
D D FD0=FA0ΘD +d/aFA0X FD=FA0(ΘD+d/aX)
Inert I FI0=FA0ΘI ---------- FI=FA0ΘI
FT0 FT=FT0+δFA0X
0
A
0
i
0
A
0
i
0
0
A
0
0
i
0
A
0
i
i
y
y
C
C
C
C
F
F






 1
a
b
a
c
a
d





Where: and

 A
A
F
C
Concentration – Flow System
Flow System – Stoichiometry Table
Chapter 4
27
Stoichiometry

 A
A
F
C
Concentration Flow System:
0



Liquid Phase Flow System:
CA 
FA


FA 0 1 X
 
0
 CA 0 1 X
 
CB 
NB


NA0
0
B 
b
a
X





 CA 0 B 
b
a
X






Flow Liquid Phase
etc.
We will consider CA and CB for gas phase
reactions in the next lecture
Chapter 4
Mole Balance
Rate Laws
Stoichiometry
Isothermal Design
Heat Effects
28
Algorithm
End of Lecture 4
29

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Lec4_PDF.pdf

  • 1. 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 4
  • 2. Lecture 4 2  Block 1  Mole Balances  Size CSTRs and PFRs given –rA=f(X)  Block 2  Rate Laws  Reaction Orders  Arrhenius Equation  Block 3  Stoichiometry  Stoichiometric Table  Definitions of Concentration  Calculate the Equilibrium Conversion, Xe Chapter 4
  • 3. Reactor Differential Algebraic Integral  V  FA 0X rA CSTR  FA0 dX dV  rA    X A A r dX F V 0 0 PFR V r dt dX N A A   0 0 0    X A A V r dX N t Batch X t FA 0 dX dW    rA     X A A r dX F W 0 0 PBR X W 3 Reactor Mole Balances Summary in terms of conversion, X Review Lecture 2
  • 6. 6 Reactors in Series reactor first to fed A of moles i point to up reacted A of moles Xi  Only valid if there are no side streams Review Lecture 2
  • 8. 8   i A C g r   Step 1: Rate Law     X h Ci  Step 2: Stoichiometry   X f rA   Step 3: Combine to get Two steps to get  rA  f X   Review Lecture 2
  • 9. Building Block 2: Rate Laws 9 Power Law Model:   B A A C kC r   β α β α   Order Rection Overall B in order A in order C B A 3 2   A reactor follows an elementary rate law if the reaction orders just happens to agree with the stoichiometric coefficients for the reaction as written. e.g. If the above reaction follows an elementary rate law 2nd order in A, 1st order in B, overall third order B A A A C C k r 2   Review Lecture 3
  • 10. Arrhenius Equation 10 E = Activation energy (cal/mol) R = Gas constant (cal/mol*K) T = Temperature (K) A = Frequency factor (same units as rate constant k) (units of A, and k, depend on overall reaction order) RT E Ae k    T  k A T 0 k 0 A 1013 T k Review Lecture 3
  • 11. Reaction Engineering 11 These topics build upon one another Mole Balance Rate Laws Stoichiometry Review Lecture 3
  • 12. Algorithm 12   i A C g r   Step 1: Rate Law     X h Ci  Step 2: Stoichiometry   X f rA   Step 3: Combine to get How to find   X f rA   Review Lecture 3
  • 13. Building Block 3: Stoichiometry 13 We shall set up Stoichiometry Tables using species A as our basis of calculation in the following reaction. We will use the stoichiometric tables to express the concentration as a function of conversion. We will combine Ci = f(X) with the appropriate rate law to obtain -rA = f(X). A is the limiting reactant. D a d C a c B a b A    Chapter 4
  • 14. Stoichiometry 14 NA  NA0 NA0X NB = NB0 - b a NA0X = NA0 NB0 NA0 - b a X æ è ç ö ø ÷ For every mole of A that reacts, b/a moles of B react. Therefore moles of B remaining: Let ΘB = NB0/NA0 Then:          X a b N N B A B 0 NC  NC 0  c a NA 0X  NA 0 C  c a X       Chapter 4
  • 15. Batch System - Stoichiometry Table 15 Species Symbol Initial Change Remaining B B NB0=NA0ΘB -b/aNA0X NB=NA0(ΘB-b/aX) A A NA0 -NA0X NA=NA0(1-X) Inert I NI0=NA0ΘI ---------- NI=NA0ΘI FT0 NT=NT0+δNA0X Where: 0 0 0 0 0 0 0 0 0 0 A i A i A i A i i y y C C C C N N        1     a b a c a d  and C C NC0=NA0ΘC +c/aNA0X NC=NA0(ΘC+c/aX) D D ND0=NA0ΘD +d/aNA0X ND=NA0(ΘD+d/aX) δ = change in total number of mol per mol A reacted Chapter 4
  • 16. Stoichiometry Constant Volume Batch 16 Note: If the reaction occurs in the liquid phase or if a gas phase reaction occurs in a rigid (e.g. steel) batch reactor  V V0 Then  CA  NA V  NA 0 1 X   V0  CA 0 1 X   CB  NB V  NA 0 V0 B  b a X       CA 0 B  b a X       etc. Chapter 4
  • 17. Stoichiometry Constant Volume Batch 17 Suppose  rA  kACA 2 CB Batch: 0 V V  -rA = kACA0 3 1- X ( ) 2 QB - b a X æ è ç ö ø ÷ Equimolar feed: 1  B Stoichiometric feed: a b B   Chapter 4
  • 18. Stoichiometry Constant Volume Batch 18   X f rA   and we have If B A A A C C k r 2   , then              X a b X C r B A A 2 3 0 1 Constant Volume Batch A r  1 X Chapter 4
  • 19. Batch Reactor - Example 19 Consider the following elementary reaction with KC=20 dm3/mol and CA0=0.2 mol/dm3. Find Xe for both a batch reactor and a flow reactor. Calculate the equilibrium conversion for gas phase reaction, Xe .          C B A A A K C C k r 2 B A  2 Chapter 4
  • 20. Batch Reactor - Example 20 Step 1: 0 A A N V r dt dX   3 0 2 . 0 dm mol CA  mol dm KC 3 20  Step 2: rate law: B B 2 A A A C k C k r    Calculate Xe B A C k k K           C B 2 A A A K C C k r Chapter 4
  • 21. Batch Reactor - Example 21 Symbol Initial Change Remaining B 0 ½ NA0X NA0 X/2 A NA0 -NA0X NA0(1-X) Totals: NT0=NA0 NT=NA0 -NA0 X/2 @ equilibrium: -rA=0 C Be Ae K C C   2 0 Ke  CBe CAe 2 CAe  NAe V  CA0 1 Xe   CBe  CA0 Xe 2 Chapter 4
  • 22. Batch Reactor - Example 22 Species Initial Change Remaining A NA0 -NA0X NA=NA0(1-X) B 0 +NA0X/2 NB=NA0X/2 NT0=NA0 NT=NA0-NA0X/2 Solution: 2 Ae Be C C C K            C Be 2 Ae A A K C C k 0 r At equilibrium 0 V V  2 / B A  Stoichiometry: Constant Volume: Batch Chapter 4
  • 23. Batch Reactor - Example 23      2 e 0 A e 2 e 0 A e 0 A e X 1 C 2 X X 1 C 2 X C K          8 2 . 0 20 2 X 1 X C K 2 2 e e 0 A e     Xeb 0.703 Chapter 4
  • 24. Flow System – Stoichiometry Table 24 A A FA0 -FA0X FA=FA0(1-X) Species Symbol Reactor Feed Change Reactor Effluent B B FB0=FA0ΘB -b/aFA0X FB=FA0(ΘB-b/aX) i  Fi0 FA 0  Ci00 CA 00  Ci0 CA 0  yi0 yA 0 Where: Chapter 4
  • 25. Flow System – Stoichiometry Table 25 Species Symbol Reactor Feed Change Reactor Effluent 0 A 0 i 0 A 0 i 0 0 A 0 0 i 0 A 0 i i y y C C C C F F        Where: Inert I FI0=A0ΘI ---------- FI=FA0ΘI FT0 FT=FT0+δFA0X C C FC0=FA0ΘC +c/aFA0X FC=FA0(ΘC+c/aX) D D FD0=FA0ΘD +d/aFA0X FD=FA0(ΘD+d/aX) 1 a b a c a d      and   A A F C Concentration – Flow System Chapter 4
  • 26. 26 Species Symbol Reactor Feed Change Reactor Effluent A A FA0 -FA0X FA=FA0(1-X) B B FB0=FA0ΘB -b/aFA0X FB=FA0(ΘB-b/aX) C C FC0=FA0ΘC +c/aFA0X FC=FA0(ΘC+c/aX) D D FD0=FA0ΘD +d/aFA0X FD=FA0(ΘD+d/aX) Inert I FI0=FA0ΘI ---------- FI=FA0ΘI FT0 FT=FT0+δFA0X 0 A 0 i 0 A 0 i 0 0 A 0 0 i 0 A 0 i i y y C C C C F F        1 a b a c a d      Where: and   A A F C Concentration – Flow System Flow System – Stoichiometry Table Chapter 4
  • 27. 27 Stoichiometry   A A F C Concentration Flow System: 0    Liquid Phase Flow System: CA  FA   FA 0 1 X   0  CA 0 1 X   CB  NB   NA0 0 B  b a X       CA 0 B  b a X       Flow Liquid Phase etc. We will consider CA and CB for gas phase reactions in the next lecture Chapter 4
  • 28. Mole Balance Rate Laws Stoichiometry Isothermal Design Heat Effects 28 Algorithm