ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

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ChE 452 Lecture 20 Collision Theory 1

Transcript of ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Page 1: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

ChE 452 Lecture 20 Collision Theory

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Page 2: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

So Far This Course Has Shown

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1) How to get rate equations from experiments

2) How to get rate equations from mechanisms

3) How to predict the mechanism Next part of the course: Theory of rate constants:

Page 3: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Theory Of Reaction Rates Has Two Parts

Theory of PreexponentialsCollision Theory, Transition State Theory, RRKM, Molecular Dynamics

Theory of Activation BarriersPolanyi Relationship, Marcus Equation, Blowers-Masel, Quantum Methods

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Page 4: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Models For Preexponentials

Collision theory (old collision theory) – simple model for preexponential - ~1013/sec, ~1013Å3/sec, ~1013A6/sec

Transition state theory – slightly better model for preexponential – bimolecular (small correction to collision theory).

RRKM – better model for preexponential – unimolecular-explains rate constraints at 1018/sec

Molecular Dynamics & Tunneling – accurate method, but time consuming

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Page 5: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Plan For Today

Describe Arrhenius’ Model (1889) Describe Trautz and Lewis model

(1918) Show limitations

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Page 6: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Arrhenius Model For AB

Cold unreactive molecules Hot reactive molecules

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0 1 2 3 4 5

Velocity, cm/sec x 1000

Num

ber

Of M

olec

ules

Hot Reactive Molecules

Cold Unreactive Molecules

Figure 7.1 The Boltzmann distribution of molecular velocities.

Divides molecules into two populations

Page 7: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Next Derive Equation For Rate

Equilibrium:

Rate equ

7

B

ΔG†-

k T1 ok =k e

(7.4)

B

ΔG†-

k T† uA AC =C e

(7.2)

Page 8: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Derivation Continued

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††

B B

ΔHΔS-

k k T1 ok = k e e

(7.6)

B

(ΔS )

k

0 ok =k e

a

B

E-k T

1 0k =k e

(7.7)

(7.8)

††† STHG

(7.4)

(7.5)

B

ΔG†-k T

1 ok =k e

Page 9: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Result of Arrhenius’ Model

Rate constantvaries exponentially

with T-1

No expression for Ko

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(7.8)

B

(ΔS )

k

0 ok =k e

Page 10: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Collision Theory

Assume Ko

equals the collision rate

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(7.2)

B

ΔG†-k T† u

A AC =C e

Page 11: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Collision Theory

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A

A

B B

C

C

AA

B B

CC

Figure 7.2 A collision between an A molecule and BC molecules.

B

ΔG-

k TA BC ABCr =Z e

(7.12)

(7.10)

(7.11)

B

ΔG-

k TreactionP =e

A BC ABC reactionr =Z P

Page 12: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Next: Consider Billiard Ball Collisions

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BC

A

A

BC

A

BC

A

A

A

Collisions occur whenever molecules get close

Figure 7.3 Some typical billiard ball collisions

Page 13: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Next: Calculate How Many Collisions Occur

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A

A

BC

bcoll

XY

LABC

AA

A

A

AA

Consider the volume swept out by a BC molecule in time to

LABC = vABC tc(7.13)

Page 14: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Next: Calculate How Many Collisions Occur

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# collisions

of the given

BC molecule

Volume of

cylinderCA

(7.14)

where CA is the concentration of the A molecules in the reacting mixture, measured in molecules/cm3. The volume of the cylinder is

Volume of

cylinderb ) Lcoll

2ABC

(

(7.15)

Page 15: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Pages Of Algebra Yields Trautz & Lewis’ Approximation

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k = v 0 A BC A BCc

(7.26)

Equation (7.26) is the key result for simple collision theory.

Derivation

Page 16: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Additional Assumption

Calculate the molecular velocity ignoring that molecules are hot.

Where:

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v =8 T

A BCB

ABC

1 2/

(7.27)

1 1

m

1

m mABC A B C

(7.28)

and mA, mB and mC are the masses of A, B and C in

atomic mass units (1 AMU = 1.66 10-24g).

k

Page 17: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Simplified Equation

In lecture 14 we showed

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v 2.52 10Å

sec

T

300K

1AMUABC

131/2

ABC

1/2

(7.29)

Page 18: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Example 7.A A Collision Theory Calculation

Use collision theory to calculate the preexponential for the reaction:

H+CH3CH3 H2+CH2CH3

(7.A.1)

at 500K.

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Page 19: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Solution:

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According to collision theory:

ABCcoll2

0 vdk (7.A.2)

Page 20: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Step 1: Calculate VABC

According to equation (7.26):

with

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v 2.4 10 Å / secT

300K

1AMUABC

131/2

ABC

1/2

BCA

ABC

M

1

M

11

(7.A.3)

(7.A.4)

Page 21: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Step 1 Continued

For reaction (7.A.1)

(7.A.5)

Substituting the numbers shows that 500K:

(7.A.6)

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A-BC1

1

1AMU

1

30AMU

0.968AMU

1/213 13

ABC

500K 1AMUv 2.52 10 3.31 10 Å/sec

300K 0.968AMU

Page 22: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Step 2: Estimate dcoll

Trautz’s approximation

Were dA and dB are the Van der Waals radii of A and B

Therefore

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2

ddd BA

coll

Å53d Å,51d6H2C2H ..

Å522

3.5Å Å51dcoll .

. (7.A.7)

Page 23: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Solution Continued

Substituting (7.A.5) and (7.A.6) into equation (7.A.2) yields:

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(7.A.8)

23

13 140

2.5Å Å Åk =π 3.31 10 =6.49 10

molecule second molecule second

Page 24: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Discussion Problem

Use collision theory to calculate the rate constant for the reaction

F + H2 H + HF

Assume a collision diameter of 2.3Å

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Page 25: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Solution: Step 1 Calculate

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AMU19

1

AMU2

1

m

1

m

11

FH2

= 1.81 AMU

Page 26: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Step 2: Calculate v

V xAMU T

K

V xK

K

V x

2 52 101

300

2 52 101

181

300

300

187 10

131 2 1 2

131 2 1 2

13

.sec

..

.

/ /

/ /

Å

Å

sec

Å

sec

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v

v

v

Page 27: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Solution

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2o collk =v π(d )

ko=(41012Å/sec) ((3Å)2) = 1.1 × 1014 Å3/sec

Page 28: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Key Predictions Of Collision Theory

Preexponentials always between 1013 and 1014/sec for small molecules

No special configurations effects Lighter species (i.e. H atoms tend to

react faster). Larger molecules have larger cross

sections than smaller molecules

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Page 29: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Preexponentials Usually The Same Order As Collision Theory?

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Table 7.2 a selection of the preexponentials reported by Wesley [1980]

Reaction Preexponential

Å3/molecule Sec

Reaction Preexponential

Å3/molecule SecH+C2H6

C2H5+H2 1.6 1014 O+C2H6 OH+C2H5 2.5 1013

H+CH H2+C 1.1 1012 O+C3H8 (CH3)2CH+OH 1.4 1010

H+CH4 H2+CH3 1 1014 O2+H OH+O 1.5 1014

O+H2 OH+H 1.8 1013 OH+OH H2O+O 1 1013

O+OH O2+H 2.3 1013 OH+CH4 H2O+CH3 5 1013

O+CH4 CH3+OH 2.1 1013 OH+H2CO H2O+HCO 5 1013

O+CH3 H+CH3O 5 1013 OH+CH3

H+CH3O 1 1013

O+HCO H+CO2 5 1012 OH+CH3 H2O+CH2 1 1013

Page 30: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Comparisons Between Collision Theory And Experiments

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Calculated Preexponential

assuming bcoll=van Der Waals radius

Calculated Preexponential assuming bcoll=covalent radius

Experimental

Å3/molec sec Å3/molec sec Preexponential

6.2 1014 2.0 1014 1.6 1014

4 1014 2.0 1014 1.1 1012

1.9 1014 7.6 1013 2.5 1013

1.25 1014 5.8 1013 1 1013

4.0 1014 2 1014 1.5 1014

Table 7.3 Preexponentials calculated from equation (7.30) for a number of reactions compared to experimental data.

Reaction

25262 HHCHCH

H CH H C2

O C H OH C H2 6 2 5

OH OH H O+O2

H O OH O2

Page 31: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Cases Where Collision Theory Fails

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CH CH CH O: CH C HCH + OH3 2 3 3 3

(7.30)

ko=1.41010 Å3/molecule-sec

2O 2O O2 2 (7.31)

ko=5.81015 Å3/molecule-sec

Page 32: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Why Does Collision Theory Fail For Reaction 7.30

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Reaction 7.30 requires a special collision geometry:

(7.33)

(7.34)

3 2 3 3 3

3 2 3 2 2 3

CH CH CH +O: CH C HCH +•OH (7.32a)

CH CH CH +O: CH CH CH +•OH (7.32b)

B

S

kConfigurations = e

B

ΔS

k configurations which lead to reactions e =

average number of configurations of the reactants

Page 33: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Summary

Collision theory: reaction occurs whenever reactants collide.

 Gives correct order of magnitude or

slightly high pre-exponential Some spectacular failures TST theory after exam

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Page 34: ChE 452 Lecture 20 Collision Theory 1. So Far This Course Has Shown 2.

Class Question

What did you learn new today?

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