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Lecture 8

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Lecture 8. 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 – Tuesday 2/1/2011. Block 1: Mole Balances on PFR s and PBR - PowerPoint PPT Presentation
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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 8
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Page 1: Lecture  8

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

Page 2: 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

Page 3: Lecture  8

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

Page 4: Lecture  8

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

Page 5: Lecture  8

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

Page 6: Lecture  8

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

Page 7: Lecture  8

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

Page 8: Lecture  8

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

Page 9: Lecture  8

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

Page 10: Lecture  8

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

Page 11: Lecture  8

PBR

11

2/1

2

2

)1(

)1(

10

)1(2

0

Wy

Wy

dWdy

yWWhen

XydW

dyFor

Page 12: Lecture  8

W

P

1

12

Pressure Drop in a PBR

Page 13: Lecture  8

No P

CA CA 0 1 X PP0

CA

W

P

13

Concentration Profile in a PBR2

Page 14: Lecture  8

No P

rA kCA2

-rA

P

W14

Reaction Rate in a PBR3

Page 15: Lecture  8

No P

X

W

P

15

Conversion in a PBR4

Page 16: Lecture  8

No P

W

P

1.0

16

PP

For

00

:0

Flow rate in a PBR5

Page 17: Lecture  8

17

0TT

0

00 1

TT

PPX

yXf

)1(10

PPy 0

Page 18: Lecture  8

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

Page 19: Lecture  8

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

Page 20: Lecture  8

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

Page 21: Lecture  8

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

Page 22: Lecture  8

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

Page 23: Lecture  8

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

Page 24: Lecture  8

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

Page 25: Lecture  8

25

Example 2: Gas Phase Reaction in PBR for δ ≠ 0

Page 26: Lecture  8

26

Example 2: Gas Phase Reaction in PBR for δ ≠ 0

Page 27: Lecture  8

27

T = T0

Pressure Drop

Page 28: Lecture  8
Page 29: Lecture  8

Pressure Drop Engineering Analysis

29

Page 30: Lecture  8

30

Pressure Drop Engineering Analysis

Page 31: Lecture  8

31

Pressure Drop Engineering Analysis

Page 32: Lecture  8

Mole BalanceRate Laws

StoichiometryIsothermal Design

Heat Effects

32

Page 33: Lecture  8

End of Lecture 8

33

Page 34: Lecture  8

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

Page 35: Lecture  8

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

Page 36: Lecture  8

PBR

36

ParametersWy

CC

yFFC

CkCr

rdWdXF

BA

T

AA

BAA

AA

2/1

0

)1(

'


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