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 8
Lecture 8 – Tuesday 2/1/2011Block 1: Mole Balances on PFRs and PBR
Must Use the Differential Form of Mole Balance
Block 2: Rate LawsBlock 3: StoichiometryBlock 4: CombinePressure Drop: Liquid Phase Reactions:
Pressure Drop does not affect the concentrations in liquid phase rxn. Gas Phase Reactions: Epsilon not Equal to Zero
d(P)/d(W)=. Polymath will combine with d(X)/f(W)=..for you
Epsilon = 0 and Isothermal P=f(W) Combine then Separate Variables (X,W) and IntegrateEngineering Analysis of Pressure Drop
2
Gas Phase Flow System:
Concentration Flow System:
0
00
0
00
0
11
1
1PP
TT
XXC
PP
TTX
XFFC AAAA
A
AFC
PP
TTX 0
00 1
0
00
0
00
0
11 PP
TT
X
XabC
PP
TTX
XabF
FCBABA
BB
3
Pressure Drop in Packed Bed Reactors
Note: Pressure drop does NOT affect liquid phase reactionsSample Question:
Analyze the following second order gas phase reaction that occurs isothermally in a PBR:
AB
AA rdWdXF 0
Mole Balance:Must use the differential form of the mole balance to separate variables:
2AA kCr Second order in A and
irreversible:
Rate Law:
Pressure Drop in Packed Bed Reactors
4
CA FA
CA 0
1 X 1X
PP0
T0
TStoichiometry:
CA CA 01 X 1X
PP0
Isothermal, T=T0
2
02
2
0
20
11
PP
XX
FkC
dWdX
A
A
Combine:
Need to find (P/P0) as a function of W (or V if you have a PFR)5
Pressure Drop in Packed Bed Reactors
TURBULENT
LAMINAR
ppc
GDDg
GdzdP 75.111501
3
Ergun Equation:
6 0
00 )1(
TT
PPX
0
0
00 T
TPP
FF
T
T
00
00
0
mm Constant mass flow:
Pressure Drop in Packed Bed Reactors
00
03
0
75.111501
T
T
ppc FF
TT
PPG
DDgG
dzdP
T
T
FF
TT
PP 00
00 Variable
Density
G
DDgG
ppc
75.1115013
00
Let
7
Pressure Drop in Packed Bed Reactors
00
00
1 T
T
cc FF
TT
PP
AdWdP
ccbc zAzAW 1Catalyst Weight
b bulk density
c solid catalyst density
porosity (a.k.a., void fraction )
Where
0
0 112
PA cc
Let8
Pressure Drop in Packed Bed Reactors
We will use this form for single reactions:
XTT
PPdWPPd
112 00
0
002 T
T
FF
TT
ydWdy
0PPy
XTT
ydWdy
12 0
XydW
dy 1
2Isothermal case
9
Pressure Drop in Packed Bed Reactors
The two expressions are coupled ordinary differential equations. We can only solve them simultaneously using an ODE solver such as Polymath. For the special case of isothermal operation and epsilon = 0, we can obtain an analytical solution. Polymath will combine the mole balance, rate law and stoichiometry.
22
0
220
11 y
XFXkC
dWdX
A
A
PXfdWdX , PXf
dWdP , Xyf
dWdy ,and or
10
Pressure Drop in Packed Bed Reactors
PBR
11
2/1
2
2
)1(
)1(
10
)1(2
0
Wy
Wy
dWdy
yWWhen
XydW
dyFor
W
P
1
12
Pressure Drop in a PBR
No P
CA CA 0 1 X PP0
CA
W
P
13
Concentration Profile in a PBR2
No P
rA kCA2
-rA
P
W14
Reaction Rate in a PBR3
No P
X
W
P
15
Conversion in a PBR4
No P
W
P
1.0
16
PP
For
00
:0
Flow rate in a PBR5
17
0TT
0
00 1
TT
PPX
yXf
)1(10
PPy 0
Example 1: Gas Phase Reaction in PBR for δ = 0Gas Phase Reaction in PBR with δ = 0
(Analytical Solution) A + B 2C Repeat the previous one with equimolar feed of A and B and
kA = 1.5dm6/mol/kg/minα = 0.0099 kg-1
Find X at 100 kg
18
00 BA CC
0AC
0BC?X
1) Mole Balance:0
'
A
A
Fr
dWdX
2) Rate Law: BAA CkCr '
3) Stoichiometry: yXCC AA 10
yXCC AB 10
19
Example 1: Gas Phase Reaction in PBR for δ = 0
ydWdy
2
, dWydy 2
Wy 12
211 Wy
WXkCyXkCr AAA 111 220
2220
0
220 11
A
A
FWXkC
dWdX
20
0W 1y,
4) Combine:
Example 1: Gas Phase Reaction in PBR for δ = 0
dWW
FkC
XdX
A
A
11 0
20
2
21
2
0
20 WW
FkC
XX
A
A
XXWWXW , ,0 ,0
0.., 75.0
6.0
eidroppressurewithoutX
droppressurewithX
21
Example 1: Gas Phase Reaction in PBR for δ = 0
Example 2: Gas Phase Reaction in PBR for δ ≠ 0Polymath Solution A + 2B C is carried out in a packed bed reactor in which there is pressure drop.The fed is stoichiometric in A and B.
Plot the conversion and pressure ratio y = P/P0 as a function of catalyst weight upto 100 kg.Additional InformationkA = 6dm9/mol2/kg/minα = 0.02 kg-1
22
A + 2B C1) Mole Balance:
0A
A
Fr
dWdX
2) Rate Law: 2BAA CkCr
3) Stoichiometry: Gas, Isothermal
PPX 0
0 1
yX
XCC AA
11
0
23
Example 2: Gas Phase Reaction in PBR for δ ≠ 0
4) y
XXCC B
AB
1
20
5) XydW
dy 1
2
6) yXf
1
0
7) 02.0 , 6 , 2 , 2 , 32
00 kFC AA
Initial values: W=0, X=0, y=1 W=100Combine with Polymath.If δ≠0, polymath must be used to solve.24
Example 2: Gas Phase Reaction in PBR for δ ≠ 0
25
Example 2: Gas Phase Reaction in PBR for δ ≠ 0
26
Example 2: Gas Phase Reaction in PBR for δ ≠ 0
27
T = T0
Pressure Drop
Pressure Drop Engineering Analysis
29
30
Pressure Drop Engineering Analysis
31
Pressure Drop Engineering Analysis
Mole BalanceRate Laws
StoichiometryIsothermal Design
Heat Effects
32
End of Lecture 8
33
Pressure Change – Molar Flow Rate
cc
0
0
0T
T0
1ATT
PP
FF
dWdP
cc0
00T
T0
1AyPTT
FF
dWdy
CC0
0
1AP2
00T
T
TT
FF
y2dWdy
Use for heat effects, multiple rxns
X1FF
0T
T Isothermal: T = T0 X1y2dW
dX
34
Example 1: Gas Phase Reaction in PBR for δ = 0A + B 2C
Case 1:
Case 2:
35
0AC
0BC?X
001
6
,0099.0,min
5.1 AB CCkgkgmoldmk
?,?,100 PXkgW
?,?,21,2 01021 PXPPDD PP
PBR
36
ParametersWy
CC
yFFC
CkCr
rdWdXF
BA
T
AA
BAA
AA
2/1
0
)1(
'