lecture 8

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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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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. Today’s lecture. Block 1: Mole Balances on PFRs and PBR Must Use the Differential Form Block 2: Rate Laws - PowerPoint PPT Presentation

TRANSCRIPT

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

Today’s lectureBlock 1: Mole Balances on PFRs and PBRMust Use the Differential Form

Block 2: Rate LawsBlock 3: StoichiometryPressure Drop:Liquid Phase Reactions: Pressure Drop does not affect the concentrations in liquid phase rx.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 IsothermalP=f(W)Combine then Separate Variables (X,W) and Integrate

2

Page 3: Lecture  8

Reactor Mole Balances in terms of conversionReactor Differential Algebraic Integral

A

0A

r

XFV

CSTR

A0A rdV

dXF

X

0 A0A r

dXFVPFR

Vrdt

dXN A0A

Vr

dXNt

X

0 A0A Batch

X

t

A0A rdW

dXF

X

0 A0A r

dXFWPBR

X

W3

Page 4: Lecture  8

Gas Phase Flow System:

Concentration Flow System:

0

00A

0

00

0AAA P

P

T

T

X1

X1C

PP

TT

X1

X1FFC

A

A

FC

P

P

T

TX1 0

00

0

0B0A

0

00

B0AB

B P

P

T

T

X1

Xab

C

PP

TT

X1

Xab

FF

C

4

Page 5: 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

A0A rdW

dXF

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

5

Page 6: Lecture  8

CA FACA 0

1 X 1X

P

P0

T0

TStoichiometry:

CA CA 0

1 X 1X

P

P0

Isothermal, T=T0

2

02

2

0A

20A

P

P

X1

X1

F

kC

dW

dX

Combine:

Need to find (P/P0) as a function of W (or V if you have a PFR)

Pressure Drop in Packed Bed Reactors

6

Page 7: Lecture  8

TURBULENT

LAMINAR

p3

pc

G75.1D

11501

Dg

G

dz

dPErgun Equation:

Pressure Drop in Packed Bed Reactors

7 0

00 T

T

P

P)X1(

0

0

0T

T0 T

T

P

P

F

F

00

00

0mm Constant mass flow:

Page 8: Lecture  8

0T

T

0

0

p3

pc0 F

F

T

T

P

PG75.1

D

11501

Dg

G

dz

dP

T

0T0

00 F

F

T

T

P

PVariable

Density

G75.1

D

11501

Dg

G

p3

pc00Let

Pressure Drop in Packed Bed Reactors

8

Page 9: Lecture  8

0T

T

0

0

cc

0

F

F

T

T

P

P

1AdW

dP

ccbc 1zAzAW Catalyst Weight

b bulk density

c solid catalyst density

porosity (a.k.a., void fraction)

Where

0cc

0

P

1

1A

2

Let

Pressure Drop in Packed Bed Reactors

9

Page 10: Lecture  8

We will use this form for single reactions:

X1

T

T

PP

1

2dW

PPd

00

0

0T

T

0 F

F

T

T

y2dW

dy

0P

Py

X1T

T

y2dW

dy

0

X1y2dW

dy

Isothermal case

Pressure Drop in Packed Bed Reactors

10

Page 11: 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

0A

220A y

X1F

X1kC

dW

dX

P,XfdW

dX P,Xf

dW

dP X,yf

dW

dyand or

Pressure Drop in Packed Bed Reactors

11

Page 12: Lecture  8

PBR

1) Mole Balance:0A

A

F

r

dW

dX

2) Rate Law:

2

2

20AA y

X1

X1kCr

AB

y

X1

X1C

P

P

X1

X1CC 0A

00AA

12

Page 13: Lecture  8

PBR

13

2/1

2

2

)W1(y

)W1(y

dWdy

1y0WWhen

y2dW

dy

0For

Page 14: Lecture  8

W

21W1y

P1

14

Page 15: Lecture  8

CA CA 0 1 X PP0

CA

2

W

P

No P

15

Page 16: Lecture  8

No P

rA kCA2

-rA

3

P

W16

Page 17: Lecture  8

No P

X4

W

P

17

Page 18: Lecture  8

0

00 T

T

P

P)X1(

18

P

Py,TT 0

0

y)X1(

1f 0

Page 19: Lecture  8

No P

5

W

P

1.0

19

Page 20: Lecture  8

Example 1: Gas Phase Reaction in PBR for δ = 0Gas Phase Reaction in PBR with δ = 0

(Polymath Solution) A + B 2C

Repeat the previous one with equil molar feed of A and B and kA = 1.5dm9/mol2/kg/minα = 0.0099 kg-1

Find X at 100 kg

20

Page 21: Lecture  8

A + B 2C

min kg mol

dm5.1k

6

1kg 0099.0

kg 100W ?X ?P

1PP D2D 0102 P2

1P Case 2:

Example 1: Gas Phase Reaction in PBR for δ = 0

21

Case 1:

?X ?P

Page 22: Lecture  8

1) Mole Balance:0A

A

F

'r

dW

dX

2) Rate Law: BAA CkC'r

3) yX1CC 0AA

4) yX1CC 0AB

0W 1y

Example 1: Gas Phase Reaction in PBR for δ = 0

22

Page 23: Lecture  8

y2dW

dy 5) dWydy2

W1y2

21W1y

W1X1kCyX1kCr 220A

2220AA

0A

220A

F

W1X1kC

dW

dX

Example 1: Gas Phase Reaction in PBR for δ = 0

23

Page 24: Lecture  8

dWW1

F

kC

X1

dX

0A

20A

2

2

WW

F

kC

X1

X 2

0A

20A

XX ,WW ,0X ,0W

0.e.i,droppressurewithout 75.0X

droppressurewith 6.0X

Example 1: Gas Phase Reaction in PBR for δ = 0

24

Page 25: Lecture  8

25

Example A + B → 2C

Page 26: Lecture  8

26

Example A + B → 2C

Page 27: 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-127

Page 28: Lecture  8

A + 2B C

1) Mole Balance:0A

A

F

'r

dW

dX

2) Rate Law: 2BAA CkC'r

3) Stoichiometry: Gas, Isothermal

P

PX1VV 0

0

y

X1

X1CC 0AA

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

28

Page 29: Lecture  8

4)

5) X1y2dW

dy

6)

7) 02.0 6k 2F 2C 3

20A0A

Initial values: W=0, X=0, y=1 W=100

Combine with Polymath.

If δ≠0, polymath must be used to solve.

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

29

Page 30: Lecture  8

30

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

Page 31: Lecture  8

31

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

Page 32: Lecture  8

32

T = T0

Page 33: Lecture  8

Engineering Analysis

33

Page 34: Lecture  8

Engineering Analysis

34

Page 35: Lecture  8

Engineering Analysis

35

Page 36: Lecture  8

Pressure Change – Molar Flow Rate

cc

0

0

0T

T0

1A

TT

P

P

FF

dW

dP

cc0

00T

T0

1AyP

TT

FF

dW

dy

CC0

0

1AP

2

00T

T

T

T

F

F

y2dW

dy Use for heat effects,

multiple rxns

X1F

F

0T

T Isothermal: T = T0 X1y2dW

dX

36

Page 37: Lecture  8

Mole Balance

Rate Laws

Stoichiometry

Isothermal Design

Heat Effects

37

Page 38: Lecture  8

Gas Phase Flow System:

Concentration Flow System:

0

00A

0

00

0AAA P

P

T

T

X1

X1C

PP

TT

X1

X1FFC

A

A

FC

P

P

T

TX1 0

00

0

0B0A

0

00

B0AB

B P

P

T

T

X1

Xab

C

PP

TT

X1

Xab

FF

C

38

Gas Phase Reaction with Pressure Drop

Page 39: Lecture  8

A + 2B C

1) Mole Balance:

2) Rate Law:

3) Stoichiometry: Gas, Isothermal

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

39

Page 40: Lecture  8

End of Lecture 8

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