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Chapter 19. Chemical Thermodynamics. ΔG = ΔH S

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Chapter 19. Chemical Thermodynamics. Δ G = Δ H – T Δ S. Enthalpy (H) and entropy (S). - PowerPoint PPT Presentation

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Page 1: Chapter 19. Chemical Thermodynamics

Chapter 19. Chemical Thermodynamics.

ΔG = ΔH – TΔS

Page 2: Chapter 19. Chemical Thermodynamics

Enthalpy (H) and entropy (S)

In Chapter 5 we discussed the role of enthalpy ( ΔH) in driving reactions. We saw that highly exothermic reactions such as the burning of gasoline proceeded very strongly, while the reverse reaction was highly endothermic, and did not proceed spontaneously at all. (CO2 and H2O do not react spontaneously to form gasoline and oxygen). However, enthalpy is not the only driving force in reactions. There is a second contribution, the entropy. Entropy relates to probability, and the increase in disorder of a system.We can think about probability in terms of a gas moving to occupy two flasks instead of only one:

Page 3: Chapter 19. Chemical Thermodynamics

We connect twoflasks as shown atthe right by a closed stopcock, one of which is evacuated.When the stopcock isopened, the air willrush into the evacu-ated flask to equalizethe pressure. What isthe driving force forthis? It is in factprobability, or entropy.

Page 4: Chapter 19. Chemical Thermodynamics

19.1 Spontaneous Processes.

A spontaneous process is one that proceeds on its own without any outside assistance.A gas will expand from one flask into a second as a spontaneous process, but the reverse will never occur. Processes that are spontaneous in one direction are non-spontaneous in the opposite direction.

Page 5: Chapter 19. Chemical Thermodynamics

The rusting of nails in air – a spontaneous process:

spontaneous

2 Fe (s) + 3 O2 (g) Fe2O3 (s) (‘rust’)

notspontaneous

Fresh nails rusted nails

Page 6: Chapter 19. Chemical Thermodynamics

Examples of spontaneous processes

Ice at 25 oC will spontaneously melt:

The reverse will never happen. Water at 25 oCwill never freeze.

spontaneousice

notspontaneous

water

Page 7: Chapter 19. Chemical Thermodynamics

spontaneous

Examples of spontaneous processes

notspontaneous

But water at -10 oC will spontaneously freeze:

water

ice

Page 8: Chapter 19. Chemical Thermodynamics

Equilibrium:A mixture of water and ice at 0 oC is at equilibrium.

ice

water(at 0 oC)

The relative quantityof ice and water remainsthe same if we don’t addor remove heat. There isno spontaneous process in either direction. If we removesome heat, the temperature remainsat 0 oC, but some water turns to ice.

Page 9: Chapter 19. Chemical Thermodynamics

Reversible processes:

These occur with infinitesmal changes in the system.

The melting and freezing of ice at 0 oC is reversible. Thus, if we add some heat, some of the ice melts, and if we remove some heat, some of the water freezes, but the temperature remains at 0 oC. At all other temperatures an irreversible process occurs.

Melting and freezing of a substance at its melting point are reversible.

Boiling and condensation of a substance at its boiling point are also reversible.

Reversible processes are not spontaneous.

Page 10: Chapter 19. Chemical Thermodynamics

Example:

When benzene vapor converts to benzene liquid at 80.1 oC (B.Pt. of benzene) and 1 atm is this a spontaneous process?

The condensation of a gas to a liquid at the boiling point of a substance is not a spontaneous process. To move the equilibrium in either direction we have to add or subtract energy.

Page 11: Chapter 19. Chemical Thermodynamics

19.2 Entropy and the second Law of Thermodynamics.

Entropy is associated with randomness. The entropy, S, of a system is a state function just like the internal energy. The change in entropy is given by

ΔS = Sfinal - Sinitial

Page 12: Chapter 19. Chemical Thermodynamics

Relating entropy to heat transfer and temperature:

For a process that occurs at constant temperature such as melting of a solid at its melting point:

ΔSsystem = qrev/T

To calculate the entropy change of a system we need to know the heat change, which is qrev, and divide it by the temperature in K. The term qrev is the reversible flow of heat in a reversible process such as enthalpy of melting of a solid at its melting point, or of boiling of a liquid at its boiling point.

Page 13: Chapter 19. Chemical Thermodynamics

Example:The molar enthalpy of fusion of Hg is 2.29 kJ/mol. What is the entropy change when 50 g of Hg freezes at the normal melting point of -38.9 oC? (fusion = melting)

The important thing to realize here is that qrev = ΔH(fusion)

Hg(s) → Hg(l) ΔH = +2.29 kJ/mol

So for freezing:Hg(l) → Hg(s) ΔH = -2.29 kJ/mol

Page 14: Chapter 19. Chemical Thermodynamics

Moles Hg = 50.0 g x 1mole = 0.249 mol200.59 g

kJ = 0.249 mole x -2.29 kJ = -0.571 kJ = -571 J 1 mole

T = 273.15 – 38.9 = 243.3 K

ΔS = qrev/T = -571/243.3 = -2.44 J/K

Note that units of entropy are J/K. A positive change in entropy means an increase in entropy of the system.

ΔH (freezing) Hg(l)

Page 15: Chapter 19. Chemical Thermodynamics

The Second Law of Thermodynamics:

The total entropy of the universe increases in any spontaneous process.

The sum of the entropy change of the system and the surroundings is always positive.

Reversible: ΔSuniverse = ΔSsystem + ΔSsurround = 0

Irreversible: ΔSuniverse = ΔSsystem +ΔSsurround > 0

Page 16: Chapter 19. Chemical Thermodynamics

Example:What happens to the entropy of the universe when a lesser spotted thrush begins to do the makarena?

Answer: It increases, ΔSuniverse > 0

For any spontaneous process, and that’s any process where anything actually happens, the entropy of the universe increases. You may get questions like the above, and if you bear in mind that (except for a reversible process) when anything happens, the entropy of the universe increases.

Page 17: Chapter 19. Chemical Thermodynamics

19.3 The Molecular Interpretation of Entropy.

Molecules can undergo translational, rotational, and vibrational motion. The number of ways a system can be arranged is the number of microstates it has. The entropy of a system is given by

S = k ln W

where W is the number of possible microstates, and kis Boltsmann’s constant =1.38 x 10-23 J/K.

Ludwig Boltzmann (1844-1906)

Boltzmann worked out the nature of entropy.

Page 18: Chapter 19. Chemical Thermodynamics

Probability and gas molecules in interconnected flasks:

Consider a pair of flasks connected by a stop-cock. The probability that all the molecules will be in one flask is (½)n, where n is the number of molecules.

one molecule,probability =(1/2)1 = 1/2

two molecules,probability =(1/2)2 = 1/4

four molecules,probability =(1/2)4 = 1/16

Page 19: Chapter 19. Chemical Thermodynamics

The relationship between probability and entropy:

So if n = 6.02 x 1023, we have a very small probability of finding allthe molecules in one flask!

Entropy relates to probability. The gasmolecules in the apparatus at right are moving randomly, but the probability aspect keeps them evenly distributed between the two flasks.

6.02 x 1023 molecules,probability = (1/2)6.02 x 10 23

There is thus a chancethat all the air moleculesin this room would rushinto one corner, and wewould all die, but it is sosmall that it would never happen.

Page 20: Chapter 19. Chemical Thermodynamics

The standard molar entropy of a substance (Sº):

The entropies of substances may be measured experimentally. The entropy of one mole of a substance in its standard state is known as the standard molar entropy (Sº). The units of Sº are J/mol.K. Some values of standard molar entropies are given overleaf. Note that So values increase solid < liquid < gas, e.g. C6H6 (s) < C6H6 (l) < C6H6 (g); increase with the size of molecules, e.g. HF < HCl < HBr < HI or CH4 < C2H6 < C3H8; and with being a solid or liquid dissolved in solution in another liquid e.g. CH3COOH (l) < CH3COOH (aq).

Page 21: Chapter 19. Chemical Thermodynamics

Standard molar entropies of selected substances at 298 K: (So, J/mol-K):

Gases:H2(g) 130.6N2(g) 191.5O2(g) 205.0C6H6(g) 269.2

Liquids:H2O(l) 69.9 C6H6(l) 172.8

Solids:Li(s) 29.1Fe(s) 27.23FeCl3(s) 142.3NaCl(s) 72.3C(diamond) 2.43C(graphite) 5.69

Page 22: Chapter 19. Chemical Thermodynamics

Making Qualitative predictions about ΔS.

Entropy increases with temperature, since the particles vibrate and move about more rapidly, and so there is greater disorder. It also increases with increasing volume, as with a an expanding gas, and with the number of independ-ently moving particles. Thus, entropy increases solid < liquid < gas.

Figure shows increasein entropy of a substancewith increasing temp. as we pass solidliquidgas.

Page 23: Chapter 19. Chemical Thermodynamics

Ssolid < Sliquid < Sgas

gasliquidsolid

Of all phase states, gases have the highest entropy

In a gas, molecules are more randomly distributed

Page 24: Chapter 19. Chemical Thermodynamics

Larger Molecules generally have a larger entropy

Larger molecules have more internal motion

Ssmall < Smedium < Slarge

Page 25: Chapter 19. Chemical Thermodynamics

} size of moleculesincreases

} Sgas > Sliquid

}dissolving a gas in a liquid is accompanied bya lowering of the entropy

}dissolving a liquid in another liquid is accompanied by an increase in entropy

Page 26: Chapter 19. Chemical Thermodynamics

Often, dissolving a solid or liquid will increase the entropy

dissolves

more disordered arrangement =higher entropy

lower entropy

solid

liquid solution

Page 27: Chapter 19. Chemical Thermodynamics

Dissolving a gas in a liquid decreases the entropy

dissolves

overall more disordered arrangement:

higher entropy

gas

solution of gasin liquid, lower S

Page 28: Chapter 19. Chemical Thermodynamics

Entropy increases with increasing temperature along the series solid <

liquid < gas

Page 29: Chapter 19. Chemical Thermodynamics

What is the sign of S for the following reactions?

FeCl2 (s) + H2 (g) → Fe (s) + 2 HCl (g)solid solidgas gas

1 mol 2 mol

S = +

Ba(OH)2 (s) → BaO (s) + H2O (g)solid solid gas

S = +

2 SO2 (g) + O2 (g) → 2 SO3 (g)gas gas gas

2 mol 1 mol 2 mol

S = -

Ag+ (aq) + Cl- (aq) → AgCl (s) S = -in solution insoluble

Note: S increases with increase in numberof moles of gas in a reaction.

Page 30: Chapter 19. Chemical Thermodynamics

For each of the following pairs of substances, which substance has a higher molar entropyat 25oC ?

HCl (l) HCl (s)

C2H2 (g) C2H6 (g)

Li (s) Cs (s)

Pb2+ (aq) Pb (s)

O2 (g) O2 (aq) HCl (l) HBr (l)

CH3OH (l) CH3OH (aq)N2 (l) N2 (g)

Page 31: Chapter 19. Chemical Thermodynamics

19.4 Entropy Changes in Chemical Reactions.

This parallels the calculation of standard molar enthalpies of reaction.

ΔSo = ΣnSo(products) -

ΣmSo(reactants)

Note that So is not zero for elements.Recall that So is a state function.

Page 32: Chapter 19. Chemical Thermodynamics

Standard molar entropies of selected substances at 298 K: (So, J/mol-K):

Gases:H2(g) 130.6N2(g) 191.5O2(g) 205.0C6H6(g) 269.2

Liquids:H2O(l) 69.9 C6H6(l) 172.8

Solids:Li(s) 29.1Fe(s) 27.23FeCl3(s) 142.3NaCl(s) 72.3C(diamond) 2.43C(graphite) 5.69

Page 33: Chapter 19. Chemical Thermodynamics

Example:Calculate ΔSo for the following reaction:

C2H4(g) + H2(g) → C2H6(g)

So products = So C2H6(g) = 229.5 J/mol-KSo reactants = So C2H4(g) + So H2(g)= 219.4 + 130.58 J/mol-K= 349.98 J/mol-K

So(products) – So(reactants)

= 229.5 – 349.98 J/mol-K

= -120.5 J/mol-K

Page 34: Chapter 19. Chemical Thermodynamics

Entropy Changes in the Surroundings.

The change in entropy in the surroundings is caused entirely by heat transferred from the system to the surroundings, and so we have q = ΔH.

ΔS(surroundings) = -qsys /T = -(ΔH/T)

Thus, if asked to calculate the change in entropy of the surroundings, just use the above equation.

Page 35: Chapter 19. Chemical Thermodynamics

Section 19.5. Gibbs Free Energy.

We have seen that both enthalpy changes (ΔH) and entropy changes (ΔS) contribute to the overall energy that drives a reaction. Josiah Willard Gibbs (1839-1903) proposed a new state function, now called G in his honor, known as the free energy.

G = H - TSJ. Willard Gibbs

(1839 – 1903)

Page 36: Chapter 19. Chemical Thermodynamics

Again, we work with changes in G, so we have:

ΔG = ΔH - TΔS

increase in increase inentropy of entropy ofsurroundings system

-ΔG is in fact the increase in entropy in the universe.

Page 37: Chapter 19. Chemical Thermodynamics

ΔH is the increase in entropy of the surroundings from ΔS(surroundings) = -q/T.

Note:1) If ΔG is negative, the reaction is spontaneous.2) If ΔG is zero, the reaction is at equilibrium.3) If ΔG is positive, the reaction is non- spontaneous , but reverse reaction is spontaneous.

Page 38: Chapter 19. Chemical Thermodynamics

19.6. Free Energy and temperature. (p. 827)

Temperature helps determine whether ΔG will be negative, and the process spontaneous. ΔH ΔS -TΔS ΔG (= ΔH – TΔS)__________________________________________ - + - - (spontaneous) + - + + (non-spontaneous) - - + + or – depends on T

+ + - + or - depends on T__________________________________________

Page 39: Chapter 19. Chemical Thermodynamics

G < 0 reaction is spontaneous(“product favored”)

G > 0 reaction is non-spontaneous

G = 0 reaction is at equilibrium

“exergonic”

“endergonic”

Page 40: Chapter 19. Chemical Thermodynamics

19.4 Free Energy Changes (ΔG) in Chemical Reactions.

This parallels the calculation of standard molar enthalpies of reaction.

ΔGo(rxn) = ΣnΔGf

o(products) -

ΣmΔGfo

(reactants)

Note that ΔGof is zero for elements.

Recall that ΔGof is a state function.

Page 41: Chapter 19. Chemical Thermodynamics

Table of ΔGof , ΔHo

f, (kJ/mol) and So

(J/mol-K) for some substances (p. 1123):Substance ΔHo

f ΔGof So

________________________________________________________

Al(s) 0 0 28.32C(s, graphite) 0 0 5.69C2H6(g) -84.68 -32.89 229.5O2(g)0 0 205.0Ni(s) 0 0 29.9NiCl2(s) -305.3 -259.0 97.65Cl2(g) 0 0 222.96

Page 42: Chapter 19. Chemical Thermodynamics

Example: Calculate ΔGo, ΔHo, and ΔSo for the following: (problem 19.54)

Ni(s) + Cl2(g) = NiCl2(s)

ΔHo = -305.3 – [0 + 0] = -305.3 kJΔSo = 97.65 – [29.9 + 222.96] = -155.21 J/KΔGo = -269.0 – [0 + 0] = -259.0 kJAlternatively, from ΔG = ΔH – TΔSΔGo = -305.3 kJ – (-155.21 J x 1 kJ x 298 K) =

1 K 1000 J-259.0 kJ

Noteunits

Page 43: Chapter 19. Chemical Thermodynamics

2 Na (s) + 2 H2O (l) → 2 NaOH (aq) + H2 (g)

The reaction of sodium metal with water:

Is the reaction spontaneous?

What is the sign of G?

What is the sign of ?

What is the sign of S?

Page 44: Chapter 19. Chemical Thermodynamics

2 Na (s) + 2 H2O (l) → 2 NaOH (aq) + H2 (g)

The reaction of sodium metal with water:

Is the reaction spontaneous?

What is the sign of G?

What is the sign of ?

What is the sign of S?

YesG = negative

H = negative (exothermic!)

S = positive

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