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Chemical Kinetics

CHAPTER 14

Part B

Chemistry: The Molecular Nature of Matter, 6 th edition

By Jesperson, Brady, & Hyslop

CHAPTER 14 Chemical Kinetics

Learning Objectives:

 Factors Affecting Reaction Rate: o Concentration o State o Surface Area o Temperature o Catalyst

 Collision Theory of Reactions and Effective Collisions

 Determining Reaction Order and Rate Law from Data

 Integrated Rate Laws

 Rate Law

Concentration vs Rate

 Integrated Rate Law

Concentration vs Time

 Units of Rate Constant and Overall Reaction Order

 Half Life vs Rate Constant (1 st Order)

 Arrhenius Equation

 Mechanisms and Rate Laws

 Catalysts

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

2

CHAPTER 14 Chemical Kinetics

Lecture Road Map:

① Factors that affect reaction rates

② Measuring rates of reactions

③ Rate Laws

④ Collision Theory

⑤ Transition State Theory & Activation Energies

⑥ Mechanisms

⑦ Catalysts

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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CHAPTER 14 Chemical Kinetics

Integrated Rate

Laws

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Integrated

Rate Laws

Concentration & Time

Rate law tells us how speed of reaction varies with concentrations.

Sometimes want to know o Concentrations of reactants and products at given time during reaction o How long for the concentration of reactants to drop below some minimum optimal value

 Need dependence of rate on time

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

5

Integrated

Rate Laws

First Order Integrated Rate Law

Rate

D

[ t

A

]

=

k

[

A

]

• Corresponding to reactions

– A

 products

• Integrating we get ln

[

[

A ]

0

A ] t

= kt

• Rearranging gives ln[ A ] t

= kt + ln[

• Equation of line y = mx + b

A ]

0

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

6

Integrated

Rate Laws

First Order Integrated Rate Law

ln[

A

]

t

  kt

ln[

A

]

0

Slope = –k

Yields straight line o Indicative of first order kinetics o Slope = –k o Intercept = ln [A]

0 o If we don't know already

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

7

Integrated

Rate Laws

2 nd Order Integrated Rate Law

Rate

= k [ B ]

2 = - D

[ B ]

D t

• Corresponding to special second order reaction

– 2B

 products

• Integrating we get

[

1

B ] t

• Rearranging gives

1

[ B ] t

=

-

[

1

B ] kt +

0

=

1 kt

[ B ]

0

• Equation of line y = mx + b

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

8

Integrated

Rate Laws

2 nd Order Integrated Rate Law

1

[

B

]

t

 kt

1

[

B

]

0

Yields straight line o Indicative of 2 nd order kinetics o Slope = +k o Intercept = 1/[B]

0

Slope

= +k

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Integrated

Rate Laws

Graphically determining Order

Make two plots:

1. ln [ A ] vs. time

2. 1/[ A ] vs. time o If ln [ A ] is linear and 1/[ A ] is curved, then reaction is 1 st order in [ A ] o If 1/[A] plot is linear and ln [ A ] is curved, then reaction is 2 nd order in [ A ] o If both plots give horizontal lines, then 0 th order in [ A ]

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Integrated

Rate Laws

Graphically determining Order

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

11

Integrated

Rate Laws

Example: SO

2

Cl

2



SO

2

+ Cl

2

Time, min [SO

2

Cl

2

], M ln[SO

2

Cl

2

]

0 0.1000

-2.3026

100

200

0.0876

0.0768

-2.4350

-2.5666

300

400

0.0673

0.0590

-2.6986

-2.8302

500

600

700

800

900

1000

1100

0.0517

0.0453

0.0397

0.0348

0.0305

0.0267

-2.9623

-3.0944

-3.2264

-3.3581

-3.4900

-3.6231

Molecular Nature of Matter, 6E

1/[SO

2

Cl

2

] (L/mol)

10.000

11.416

13.021

14.859

16.949

19.342

22.075

25.189

28.736

32.787

37.453

42.735

12

Integrated

Rate Laws

Example: SO

2

Cl

2



SO

2

+ Cl

2

-2.2

-2.4

-2.6

-2.8

-3.0

-3.2

-3.4

-3.6

-3.8

0

First Order Plot for SO

2

Cl

2

Decomposition

200 400 600 time (min)

800 1000 1200

45

Second order plot for SO

2

Cl

2

Decomposition

40

35

30

25

20

15

10

0 200 400 600 time (min)

800 1000 1200

Reaction is 1

st

order in SO

Jesperson, Brady, Hyslop. Chemistry: The

2

Cl

2

Molecular Nature of Matter, 6E

13

Integrated

Rate Laws

Time

(s)

0

50

100

150

200

250

300

350

Example:

HI(g)  H

2

(g) + I

2

(g)

[HI]

(mol/L)

0.1000

0.0716

0.0558

0.0457

0.0387

0.0336

ln[HI]

-2.3026

-2.6367

-2.8860

-3.0857

-3.2519

-3.3932

0.0296

-3.5200

0.0265

-3.6306

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

1/[HI]

(L/mol)

10.000

13.9665

17.9211

21.8818

25.840

29.7619

33.7838

37.7358

14

Integrated

Rate Laws

Example:

HI(g)  H

2

(g) + I

2

(g)

-2.2

First Order Plot for HI Decomposition at 508 o

C

-2.4

40

Second order plot for HI

Decomposition at 508 o

C

35

-2.6

-2.8

30

-3.0

-3.2

-3.4

25

20

-3.6

-3.8

0 50 100 150 200 250 300 350 time (s)

15

10

0 50 100 150 200 250 300 350 time (s)

Reaction is second order in HI.

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

15

Group

Problem

A plot for a zeroth order reaction is shown. What is the proper label for the y-axis in the plot ?

A. Concentration Zeroth Order Plot

B. ln of Concentration

C. 1/Concentration

D. 1/ ln Concentration

0 200 400 600 time (min)

800 1000 1200

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Integrated

Rate Laws

Half Life (t

1/2

) for first order reactions

Half-life = t

½

We often use the half life to describe how fast a reaction takes place

First Order Reactions o Set [ A ] t

=

1

2

[ A ]

0 o Substituting into ln

[

[

A ]

0

A ] t

= kt o Gives ln

1

2

[ A ]

0

[ A ]

0

= kt

1

2 o Canceling gives ln 2 = kt

½ o t

Rearranging gives 1

2

= ln k

2

=

0

1

Jesperson, Brady, Hyslop. Chemistry: The

.

k

693

1

Molecular Nature of Matter, 6E

17

Integrated

Rate Laws

Half Life (t

1/2

) for First Order Reactions

Observe:

1.

t

½ is independent of [A] o o For given reaction (and T ) o Takes same time for concentration to fall from o 2 M to 1 M as from o 5.0

10 –3 M to 2.5

10 –3 M

2.

k

1 has units (time) –1 , so t

½ has units (time) o t

½ called half-life o Time for ½ of sample to decay

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Integrated

Rate Laws

Half Life (t

1/2

)

Does this mean that all of sample is gone in two half-lives (2 × t

½

)?

No! o In 1 st t

½

, it goes to ½[A] o o In 2 nd t

½

, it goes to ½(½[A] o

) = ¼[A] o o In 3 rd t

½

, it goes to ½(¼[A] o

) = ⅛[A] o o In n th t

½

, it goes to [A] o

/2 n

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

19

Integrated

Rate Laws

Half Life (t

1/2

)

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

20

Integrated

Rate Laws

Half Life (t

1/2

): First Order Example

131 I is used as a metabolic tracer in hospitals. It has a half-life, t

½

= 8.07 days.

How long before the activity falls to 1% of the initial value?

N = N o e kt t ln

N

N o

= kt = t ln2 t

1

2

= t

1

2 ln

N ln

2

N o = -

(

8

.

07 days

)ln

æ

è

1

100

ö

ø ln

2

=

53

.

6 days

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

21

Group

Problem

The radioactive decay of a new atom occurs so that after 21 days, the original amount is reduced to 33%. What is the rate constant for the reaction in s

–1

?

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Group

Problem

The half-life of I-132 is 2.295 h. What percentage remains after 24 hours?

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

23

Integrated

Rate Laws

Half Life (t

1/2

): Carbon-14 Dating

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

24

Integrated

Rate Laws

Half Life (t

1/2

): Second Order Reactions

How long before [A ] = ½[A] o

?

t

1/2

=

1 k [ A ]

0 o t

½

, depends on [A] o o t

½

, not useful quantity for a second order reaction

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

25

Group

Problem

The rate constant for the second order reaction 2 A → B is 5.3

× 10

–5

M

–1 s

–1

. What is the original amount present if, after 2 hours, there is 0.35 M available?

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

26

CHAPTER 14 Chemical Kinetics

Collision Theory

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

27

Collision

Theory

Reaction Rates

Collision Theory

As the concentration of reactants increase o The number of collisions increases o Reaction rate increases

As temperature increases o Molecular speed increases o Higher proportion of collisions with enough force (energy) o There are more collisions per second o Reaction rate increases

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Collision

Theory

Reaction Rates

Rate of reaction proportional to number of effective collisions/sec among reactant molecules

Effective collision o One that gives rise to product e.g. At room temperature and pressure o H

2 and I

2 molecules undergoing 10 o Yet reaction takes a long time

10 collisions/sec o Not all collisions lead to reaction

Only very small percentage of all collisions lead to net change

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Collision

Theory

Molecular Orientation

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

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Collision

Theory

Temperature

As T increases o More molecules have E a o So more molecules undergo reaction

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

31

Collision

Theory

Activation Energy (E a

)

Molecules must possess certain amount of kinetic energy

(KE) in order to react

Activation Energy, E a reaction to occur

= Minimum KE needed for o Get energy from collision with other molecules o If molecules move too slowly, too little KE, they just bounce off each other o Without this minimum amount, reaction will not occur even when correctly oriented

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

32

CHAPTER 14 Chemical Kinetics

Transition State

Theory

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

33

Transition

State

Molecular Basis of Transition State Theory

KE KE

KE decreasing as PE increases

Is the combined KE of both molecules enough to overcome

Activation Energy

KE

PE

KE

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

34

Transition

State

Molecular Basis of Transition State Theory

Activation energy (E

a

)

= hill or barrier between reactants and products

Heat of reaction

(

H)

= difference in PE between products and reactants

H reaction

= H products

H reactants

Reaction Coordinate (progress of reaction)

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

Products

35

Transition

State

Exothermic Reactions

Exothermic reaction

• Products lower PE than reactants

Exothermic

Reaction

H = –

Products

Reaction Coordinate (progress of reaction)

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

36

Transition

State

Exothermic Reactions o 

H reaction

< 0 (negative) o Decrease in PE of system o Appears as increase in KE o So the temperature of the system increases o Reaction gives off heat o Can ’t say anything about E a from size of could be low and reaction rapid

H o E a

H could be high and reaction slow even if rxn large and negative o E a

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

37

Transition

State

Endothermic Reactions

H

reaction

= H

products

H

reactants

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

Endothermic

Reaction

H = +

38

Transition

State

Endothermic Reactions o 

H reaction

> 0 (positive) o Increase in PE o Appears as decrease in KE o So temperature of the system decreases o Have to add E to get reaction to go o E a

 

H rxn o If

H rxn as E a includes large and positive

H rxn o E a must be high o Reaction very slow

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

39

Transition

State

Activated Complex o Arrangement of atoms at top of activation barrier o Brief moment during successful collision when o bond to be broken is partially broken and o bond to be formed is partially formed

Example

H

3

C N C

N

H

3

C

C

Transition State

H

3

C C N

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

40

Group

Problem

Draw the transition state complex, or the activated complex for the following reaction:

CH

3

CH

2

O + H

3

O +  CH

3

CH

2

OH + H

2

O

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

41

CHAPTER 14 Chemical Kinetics

Activation

Energies

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

42

E a

Arrhenius Equation

The rate constant is dependent on Temperature, which allows us to calculate Activation Energy, E a

Arrhenius Equation:

Equation expressing temperature-dependence of k k = Ae E a

/ RT o A = Frequency factor has same units as k o R = gas constant in energy units

= 8.314 J mol –1 K –1 o E a

= Activation Energy o T = Temperature in K

—has units of J/mol

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

43

E a

Calculating Activation Energy

• Method 1. Graphically

• Take natural logarithm of both sides

• Rearranging ln k

=

ln A

çç

æ

è

E

R a

• Equation for a line

• y = b + mx

÷÷

ö

ø

çç

æ

è

1

T

÷÷

ö

ø

Arrhenius Plot

• Plot ln k ( y axis) vs. 1/T ( x axis)  yield a straight line

• Slope = -E a

/R

• Intercept = A

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

44

E a

Arrhenius Equation: Graphing Example

Given the following data, predict k at 75 ˚C using the graphical approach ln k = -

E a

R

´

1

T

+ ln A ln (k) = –36.025/T – 6.908

k ( M /s) T , ˚C T , K

0.000886 25 298

0.000894 50 348

0.000908 100 398

0.000918 150 448

?

75 348 ln (k) = –36.025/(348) – 6.908 = – 7.011

k = e -

7

.

012 =

9

.

01

´

10

-

4

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

45

E a

Arrhenius Equation: Graphing Example

-6,99

-7,00

-7,01

-7,02 y = –36.025x – 6.908

-7,03

0,0022 0,0024 0,0026 0,0028 0,003 0,0032 0,0034

1/ T (K –1 )

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

46

E a

Arrhenius Equation

Sometimes a graph is not needed o Only have two k s at two T s

Here use van't Hoff Equation derived from

Arrhenius equation: ln

çç

æ

è

k k

2

1

ö

ø

÷÷ =

-

E a

R

çç

æ

è

T

1

2

-

1

T

1

÷÷

ö

ø

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

47

E a

Arrhenius Equation: Ex Vant Hoff Equation

CH

4

+ 2 S

2



CS

2

+ 2 H

2

S

k (L/mol s) T ( ˚ C) T (K)

1.1 = k

1

6.4 = k

2

550

625

823 = T

1

898 = T

2 ln çç

æ

è

E a

6

.

4

1

.

1

=

ö

ø

÷÷ =

E a

8.3145 J/K mol

çç

æ

è

-

(

8.314 J/K mol

çç

æ

è

1

898 K

1

) ln

823 K

÷÷

ö

ø

çç

æ

è

6.4

1.1

898 K

÷÷

ö

ø

1

1

823 K

=

1

.

4

´

10 5

÷÷

ö

ø

J/mol

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

48

Group

Problem

Given that k at 25 ˚C is 4.61 × 10 –1 M /s and that at 50 ˚C it is

4.64 × 10

–1

M /s, what is the activation energy for the reaction?

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

49

Group

Problem

A reaction has an activation energy of 40 kJ/mol. What happens to the rate if you increase the temperature from 70˚C to 80 ˚C?

A. Rate increases approximately 1.5 times

B. Rate increases approximately 5000 times

C. Rate does not increase

D. Rate increases approximately 3 times

Jesperson, Brady, Hyslop. Chemistry: The

Molecular Nature of Matter, 6E

50

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