Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number...

45
Chapter 17 1

Transcript of Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number...

Page 1: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

1

Chapter 17

Page 2: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

S = k ln W

AN

Rk

Boltzmann constant (k)

units on S is J/K

k = 1.38 x 1023J/K

Gas constant

Avogadro constant

Microstates and Entropy

Boltzmann was the founding father of statistical mechanics, a completely new way of thinking about theoretical physics. His work was ridiculed by his fellow professors.

Page 3: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

3

Standard Entropy

• Difficult to count the number of microstates directly.

• Measured by calorimetery.

• Standard entropy (S) absolute entropy of a substance at 1 atm (typically at 25C)

• Units of J K-1 mol-1

• All positive values.

• Absolute values (unlike DH which is relative)

Page 4: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

4

Why is there a –S?

S = k ln W

Al + 6H2O Al(H2O)6 (aq)3+ 2+

Page 5: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

5

Chapter 17

Page 6: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

6

Spontaneity

Spontaneous: process that does occur under a specific set of conditions.

Nonspontaneous: process that does not occur under a specific set of conditions.

The reverse of a spontaneous process is a nonspontaneous one.

Spontaneity depends on temperature.

Page 7: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

7

Enthalpy (H) is used to quantify the heat flow into or out of a system in a process that occurs at constant pressure.

Predicting Spontaneity

DHrxn = Hproducts – Hreactants

Hproducts < Hreactants

DH < 0

Hproducts > Hreactants

DH > 0Exothermic Endothermic

Enthalpically favorable Enthalpically unfavorable

If we mix reactants and products together will the reaction occur?

Not enough information. We need to know the change in entropy to predict if a reaction will spontaneously occur.

Page 8: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

8

Entropy (S) Is a measure of the number of specific ways (microstates) in which a thermodynamic system may be arranged.

Predicting Spontaneity

DSrxn = Sproducts – Sreactants

Sproducts < Sreactants

DS < 0

Sproducts > Sreactants

DS > 0Entropy decreases Entropy increases

Entropically unfavorable Entropically favorable

If we mix reactants and products together will the reaction occur?

Still not enough information. We need to know total entropy change to predict if a reaction will spontaneously occur.

Page 9: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

9

If we mix reactants and products together will the reaction occur?

Predicting Spontaneity

Nonspontaneous process:

DSuniv = DSsys + DSsurr

Equilibrium : DSuniv = 0

DSuniv < 0

Spontaneous process: DSuniv > 0

DSuniv = DSsys + DSsurr

Can calculate from:

DS0rxn nS0(products)= S mS0(reactants)S-

If we know DSsurr we can calculate DSuniv

Page 10: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

10

DSuniv = DSsys + DSsurr

Can calculate from:

DS0rxn nS0(products)= S mS0(reactants)S-

If we know DSsurr we can calculate DSuniv

Predicting Spontaneity

DS0 rx

n

surr

ound

ing

syst

em

DS su

rr

Surrounding = everything in the universe except the system.

Very, very difficult to measure!If not impossible.

Page 11: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

11

Exothermic Reaction Endothermic Process

Heat and Entropy

DSsurr > 0

-DHsys

Surroundings + heat = ↑ S

0 < DHsys

DSsurr < 0

+DHsys

Surroundings - heat = ↓ S

0 > DHsys

DSsurr ∝ -DHsys

Page 12: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

12

Heat and EntropyHeat released by the system increases the disorder of the surroundings.

DSsurr ∝ -DHsys

The effect of -DHsys on the surroundings depends on temperature: – At high temperature, where there is already considerable

disorder, the effect is muted

– At low temperature the effect is much more significant

– The difference between tossing a rock into a calm pool (low T) and a storm-tossed ocean (high T)

DSsurr = -DHsys

T

Page 13: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

13

DSuniv = DSsys + DSsurr

Predicting Spontaneity

DSsurr = -DHsys

TDSuniv = DSsys + -DHsys

T

-TDSuniv = -TDSsys + DHsys

Substitution:

Multiply by -T:

-TDSuniv = DHsys - TDSsysRearrange:

Both in terms of the system.

This equation relates DSuniv to DHsys and DSsys.

Page 14: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

14

Gibbs Free Energy

-TDSuniv = DHsys - TDSsys

Josiah Willard Gibbs (1839-1903)

DG = DHsys - TDSsys

First American Ph.D. in Engineering (Yale, 1863)

Praised by Albert Einstein as "the greatest mind in American history"

Died at 64 from an acute intestinal obstruction.

Gibbs free energy (DG)-

• AKA Free energy.

• Relates S, H and T of a system.

• Can be used to predict spontaneity.

• G is a state function.

in K

Page 15: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

15

Gibbs Free Energy

DG = DHsys - TDSsys

Gibbs free energy (DG)- Can be used to predict spontaneity.

For a constant temperature and constant pressure process:

DG < 0 The reaction is spontaneous in the forward direction.

DG > 0 The reaction is nonspontaneous as written. The reaction is spontaneous in the reverse direction.

DG = 0 The reaction is at equilibrium.

-DG = -T(+DSuniv)

+DG = -T(-DSuniv)

DSuniv > 0

-TDSuniv = DHsys - TDSsys

DSuniv < 0

DG = -T(DSuniv) = 0 DSuniv = 0

Page 16: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

16

Gibbs Free Energy

DG = DH - TDS• If you know DG for reactants and products then you can

calculate if a reaction is spontaneous. • If you know DG for two reaction then you can calculate if the

sum is spontaneous. • If you know DS, DH and T then you can calculate spontaneity. • Can predict the temperature when a reaction becomes

spontaneous.• If you have DHvap or DHfus and DS you can predict boiling and

freezing points.• If you have DHvap or DHfus and T you can predict the entropy

change during a phase change.• Can predict equilibrium shifts.

Page 17: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

17

Standard Free Energy ChangesThe standard free-energy of reaction (DG0 ) is the free-energy change for a reaction when it occurs under standard-state conditions.

rxn

aA + bB cC + dD

DG0rxn nDG0 (products)f= S mDG0 (reactants)fS-

DG0rxn dDG0 (D)fcDG0 (C)f= [ + ] - bDG0 (B)faDG0 (A)f[ + ]

Standard free energy of formation (DG0) is the free-energy change that occurs when 1 mole of the compound is formed from its elements in their standard states.

f

DG0 of any element in its stable form is zero.f

Page 18: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

18

aA + bB cC + dD

Standard Free Energy ChangesDG is a state function so free energy can be calculated from the

table of standard values just as enthalpy and entropy changes.

DG0rxn nDG0 (products)f= S

mDG0 (reactants)fS-

Standard free energy of formation (DG0) is the free-energy change that occurs when 1 mole of the compound is formed from its elements in their standard states.

f

Page 19: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

19

Standard Free Energy Changes

From appendix 3:KClO3(s) DGf = -289.9 kJ/molKCl(s) DGf = -408.3 kJ/molO2(g) DGf = 0 kJ/mol

2KClO3(s) 2KCl(s) + 3O2(g)

Calculate the standard free-energy change for the following reaction:

DG0rxn nDG0 (products)f= S mDG0 (reactants)fS-

DG0rxn = [2(408.3 kJ/mol) + 3(0)] [2(289.9 kJ/mol)]

DG0rxn = 816.6 (579.8)

DG0rxn = 236.8 kJ/mol

DG0rxn < 0 Yes!

Is the reaction spontaneous?

Page 20: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Example

20

17.4

Calculate the standard free-energy changes for the following reactions at 25°C.

(a) CH4(g) + 2O2(g) CO2(g) + 2H2O(l)

From appendix 3:CH4(g) DGf = -50.8 kJ/molO2(g) DGf = 0 kJ/molCO2(g) DGf = -394.4 kJ/molH2O (l) DGf = -237.2 kJ/mol

ΔG°rxn = [ΔG°f (CO2) + 2ΔG°f (H2O)] - [ΔG°f (CH4) + 2ΔG°f (O2)]

ΔG°rxn =[(-394.4 kJ/mol) + (2)(-237.2 kJ/mol)] - [(-50.8 kJ/mol) + (2) (0 kJ/mol)]

ΔG°rxn = -818.0 kJ/mol

Spontaneous?

Yes.

Page 21: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Example

21

17.4

Calculate the standard free-energy changes for the following reactions at 25°C.

(b) 2MgO(s) 2Mg(s) + O2(g)

From appendix 3:MgO(s) DGf = -569.6 kJ/molO2(g) DGf = 0 kJ/molMg(s) DGf = 0 kJ/mol

ΔG°rxn = [2ΔG°f (Mg) + ΔG°f (O2)] - [2ΔG°f (MgO)]

ΔG°rxn = [(2)(0 kJ/mol) + (0 kJ/mol)] - [(2)(-569.6 kJ/mol)]

ΔG°rxn = 1139 kJ/mol

Spontaneous?

No.But the reverse is…

2Mg(s) + O2(g) 2MgO(s)

Page 22: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

22

More DG° Calculations

DG0rxn nDG0 (products)

f= S

mDG0 (reactants)fS-

To predict spontaneity of any rxn:

1) Pick any reactants and products.

2) Write a balanced equation.

3) Calculate DG0rxn.

4) Is the reaction spontaneous?

Appendix 3

Page 23: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

23

Another Example

+ O2

C(s, diamond) + O2(g) CO2(g)

DG°rxn = -396.4 kJ

Therefore, diamonds are contributing to global warming!

very slowly

ΔG°rxn = [ΔG°f (CO2)] - [ΔG°f (C, diamond) + ΔG°f (O2)]

From appendix 3:C, diamond(s) DGf = 2.9 kJ/molO2(g) DGf = 0 kJ/molCO2(g) DGf = -394.4 kJ/mol

Page 24: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

24

More DG° CalculationsSimilar to DH°, one can use the DG° for various reactions to determine DG° for the reaction of interest (a “Hess’ Law” for DG°) Hess’ Law- states that regardless

of the multiple stages or steps of a reaction, the total enthalpy change for the reaction is the sum of all changes. 

What is the DG° for this reaction:

Given:C(s, diamond) + O2(g) CO2(g) DG° = -397 kJ

C(s, graphite) + O2(g) CO2(g) DG° = -394 kJ

Page 25: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

25

More DG° CalculationsWhat is the DG° for this reaction:

C(s, graphite) + O2(g) CO2(g) DG° = -394 kJ

CO2(g) C(s, graphite) + O2(g) DG° = +394 kJ

Given:C(s, diamond) + O2(g) CO2(g) DG° = -397 kJ

C(s, diamond) + O2(g) CO2(g) DG° = -397 kJ

CO2(g) C(s, graphite) + O2(g) DG° = +394 kJ

C(s, diamond) C(s, graphite) DG° = -3 kJ

DG°rxn < 0…..rxn is spontaneous

Page 26: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

26

Alternative DG CalculationIs the following reaction spontaneous at 298 K?

(assume standard conditions)

KCl(s)(s)3KClO(s)4KClO 43

DH°f (kJ/mol) S° (J/mol.K)

KClO3(s) -397.7 143.1

KClO4(s) -432.8 151.0

KCl (s) -436.7 82.6

Given:

DG°rxn = DH°rxn - TDS°rxn

First Calculate

Given

Then Find

Page 27: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

27

Alternative DG CalculationKCl(s)(s)3KClO(s)4KClO 43

DH°f (kJ/mol) S° (J/mol.K)KClO3(s) -397.7 143.1KClO4(s) -432.8 151.0KCl (s) -436.7 82.6

kJ

kJkJkJ

KClOHKClHKClOHH fffrxn

144

)7.397(4)7.436()8.432(3

43 34

KJ

KJ

KJ

KJ

KClOSKClSKClOSS rxn

8.36

)1.143(4)6.82()0.151(3

43 34

Page 28: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

28

Alternative DG CalculationKCl(s)(s)3KClO(s)4KClO 43

DH°f (kJ/mol) S° (J/mol.K)KClO3(s) -397.7 143.1KClO4(s) -432.8 151.0KCl (s) -436.7 82.6

DH°rxn = -144 kJ DS°rxn = -36.8 J/K

G rxn H rxn TS rxn

144kJ 298K 38.6J K 1kJ

1000J

133kJ

DG°rxn < 0…..rxn is spontaneous at 298 K

Enthalpically favorable Entropically unfavorable

What about at 5000 K?

DG°rxn = 50 kJDG°rxn > 0…rxn is nonspontaneous at 5000 K

(Assuming the same DH and S)

Page 29: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

29

DG Temperature Dependence

KCl(s)(s)3KClO(s)4KClO 43

DG°rxn = 50 kJ at 5000 K

DG°rxn = -133 kJ at 298 K Spontaneous

Nonspontaneous

Reaction spontaneity is a temperature dependent phenomenon!

DGrxn = DHrxn - TDSrxn

Page 30: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

30

DG Temperature Dependence

DG = DH - TDS

Enthalpy:DHrxn < 0 The reaction is enthalpically favorable.

Entropy: DSrxn > 0 The reaction is entropically favorable.

Need both to predict spontaneity. And sometimes temperature!DG < 0 SpontaneousDG > 0 NonspontaneousDG = 0 Equilibrium

1) If DH < 0 and DS > 0, then DG is negative at all T

3) If DH < 0 and DS < 0, then DG depends on T

2) If DH > 0 and DS > 0, then DG depends on T

4) If DH > 0 and DS < 0, then DG is positive at all T

Page 31: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

31

DG = DH - TDSDG < 0 SpontaneousDG > 0 NonspontaneousDG = 0 Equilibrium

3) DH < 0 and DS < 0

If DH < TDS, then DG is positive.If DH > TDS, then DG is negative.

DG Temperature Dependence

2) DH > 0 and DS > 0

If DH < TDS, then DG is negative.If DH > TDS, then DG is positive.

Nonspontaneous at high TSpontaneous at low T

(Enthalpically favorable, entropically unfavorable)

(Enthalpically unfavorable, entropically favorable)

Spontaneous at high TNonspontaneous at low T

Page 32: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

32

DG = DH - TDS

DG Temperature Dependence

Page 33: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

33

DG Temperature Dependence

Nonspontaneous

Spontaneous

Four possible scenarios:

(1) H < 0, S > 0

(2) H > 0, S > 0

(3) H < 0, S < 0

(4) H > 0, S < 0

Page 34: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

exothermic

system becomes more disordered

exothermic

system becomes more ordered

endothermic

system becomes more disordered

DSuniv and Spontaneous ReactionsDG = DH - TDS

Class 1: Class 3:

Class 2:

34

Page 35: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

35

Predicting T from Gibbs Equation

KCl(s)(s)3KClO(s)4KClO 43

DG°rxn = 50 kJ at 5000 K

DG°rxn = -133 kJ at 298 K Spontaneous

Nonspontaneous

Reaction spontaneity is a temperature dependent phenomenon!

At what temperature will the reaction become spontaneous?

Find T where DG changes from positive to negative.

I.e. when DG =0.

DG = DH – TDS = 0

T = DH/DS

Page 36: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

36

Predicting T from Gibbs EquationAt what T is the following reaction spontaneous?

Br2(l) Br2(g)

Given: DH°= 30.91 kJ/mol

DS°= 93.2 J/mol.K

DG = DH – TDS = 0

T = DH/DS

T = (30.91 kJ/mol) /(93.2 J/mol.K)

T = 331.7 K

H > 0, S > 0The reaction will be spontaneous when

T > 331.7 K

Page 37: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Predicting T from Gibbs EquationAt what T is the following reaction spontaneous?

CaCO3 (s) CaO (s) + CO2 (g)

DG0 = DH0 – TDS0 = 0

T = D0H/DS0

DH0 = 177.8 kJ/mol

DS0 = 160.5 J/K·mol

DG0 = 0 at 835 oC

Equilibrium Pressure of CO2

37

Page 38: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Chapter 11

38

Page 39: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Liquid ↔ Gas

At time = 0 At time > 0 At time = ∞

Liquid

# of molecules in =# of molecules out

At equilibrium!

rate of evaporation = rate of condensation

DG = DH - TDSDG < 0 SpontaneousDG > 0 NonspontaneousDG = 0 Equilibrium

39

Page 40: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

40

Gibbs Equation and Phase Change

Molar heat of vaporization (DHvap) is the energy required to vaporize 1 mole of a liquid at its boiling point.

H2O (l) H2O (g)

DG = DH – TDS = 0

If we know DHvap and boiling point we can calculate DS!

DS = TDH

= 40.79 kJ/mol

373 KDS

DHvap = 40.79 kJ/molBP(H2O) = 373 K

Page 41: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Example

41

17.5

The molar heats of fusion and vaporization of benzene are 10.9 kJ/mol and 31.0 kJ/mol, respectively. Calculate the entropy changes for the solid → liquid and liquid → vapor transitions for benzene. At 1 atm pressure, benzene melts at 5.5°C and boils at 80.1°C.

solid

liquid

vapor

Page 42: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Example

42

17.5

The molar heats of fusion and vaporization of benzene are 10.9 kJ/mol and 31.0 kJ/mol, respectively. Calculate the entropy changes for the solid → liquid and liquid → vapor transitions for benzene. At 1 atm pressure, benzene melts at 5.5°C and boils at 80.1°C.

Molar heat of vaporization (DHvap) is the energy required to vaporize 1 mole of liquid to gas.

Molar heat of fusion (DHfus) is the energy required to melt 1 mole of solid.

solid → liquid → vaporDHvapDHfus

Page 43: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

Example

43

17.5

The molar heats of fusion and vaporization of benzene are 10.9 kJ/mol and 31.0 kJ/mol, respectively. Calculate the entropy changes for the solid → liquid and liquid → vapor transitions for benzene. At 1 atm pressure, benzene melts at 5.5°C and boils at 80.1°C.

solid → liquid → vaporDHvapDHfus

DG = DH – TDS = 0 DS = TDH

fusfus

f

ΔΔ =

(10.9 kJ/mol)(1000 J/1 kJ) =

(5.5 + 273)K

= 39.1 J / K mol

HS

Tvap

vapb

ΔΔ =

(31.0 kJ/mol)(1000 J/1 kJ) =

(80.1 + 273)K

= 87.8 J / K mol

HS

T

Page 44: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).
Page 45: Chapter 17 1. The Austrian physicist Ludwig Boltzmann introduced a model to relate the total number of microstates (the multiplicity, W) to entropy (S).

45

Chapter 17