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Chapter 13 Thermodynamics: Spontaneous Processes, Entropy, and Free Energy

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Chapter 13. Thermodynamics: Spontaneous Processes, Entropy, and Free Energy. Chapter 13: Entropy and Free Energy In chapter 13 the question of why some chemical (or physical) processes are spontaneous is asked. R → P - PowerPoint PPT Presentation

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Page 1: Chapter 13

Chapter 13

Thermodynamics: Spontaneous Processes, Entropy, and Free Energy

Page 2: Chapter 13

Chapter 13: Entropy and Free EnergyIn chapter 13 the question of why some chemical (or physical) processes are spontaneous is asked.

R → PThe answer is found within the 2nd Law of thermodynamics. Spontaneous processes occur due to and increase in the total entropy (S), i.e. S > 0 for the system plus the surrounding.For example, exothermic chemical reactions are often spontaneous because of increases in disorder of the surrounding caused by the release of heat.

Page 3: Chapter 13

Suniverse = Ssystem + Ssurrounding

Entropy is also a measure of the unavailability of the system’s energy to do work.

Consider that heat and work are both forms of energy. Which is the more ordered form?

Page 4: Chapter 13

Entropy (S) is defined quantitatively by the amount of heat absorbed (isothermally) by the system divided by the absolute temperature

S = q/T (Joule/K)

For a glass of ice melting the heat from the room is transferred to the ice until the temperatures are equal.

The dispersal of energy…warmer to cooler result always results in an increase in entropy.

Page 5: Chapter 13

Maxwell’s Demon…a gedanken experiment.

Two containers are filled with the same gas at equal temperatures. When a faster than average molecule flies near the door the demon opens it. Over time the average temperature will increase in one side and decrease in the other…driving the system out of equilibrium.

Page 6: Chapter 13

ENTROPY AND WHY ENDOTHERMIC PROCESSES OCCUR.

Entropy (S°) is a measure of randomness or disorder in a system or its surrounding.

Spontaneous processes are accompanied by a net increase in the entropy of the universe. This statement is know as the 2nd Law of thermodynamics.

Suniverse = Ssystem + Ssurrounding

So that…

Suniverse = Ssystem + Ssurrounding > O

Page 7: Chapter 13

Third Law of Thermodynamics

• Third Law of Thermodynamics - the entropy of a perfect crystal is zero at absolute zero. S is explicitly known (=0) at 0 K, S values at other

temps can be calculated.• Absolute entropy is the entropy change of a

substance taken from S = 0 (at T = 0 K) to some other temperature.

• Standard molar entropy (So) is the absolute entropy of 1 mole of a substance in its standard state.

Page 8: Chapter 13

The 3rd Law of Thermodynamics defines the entropy of a perfect crystal, at zero Kelvin to be equal to zero.

Graphite has a higher standard molar entropy than diamond. Why might that be?

S° = 5.7 J/mol KS° = 2.4 J/mol K

Page 9: Chapter 13

The entropy of a substance like water is linked to the motion (i.e. the temperature) of the molecules

Page 10: Chapter 13

Select Standard Molar Entropy Values (1 atm, 298 K)

Formula So (J/(mol•K) Formula Name So

(J/(mol•K)Br2(g) 245.5 CH4(g) methane 186.2

Br2(l) 152.2 CH3CH3(g) Ethane 229.5

Cdiamond(s) 2.4 CH3OH(g) Methanol 239.7

Cgraphite(s) 5.7 CH3OH(l) 126.8

CO(g) 197.7 CH3CH2OH(g) Ethanol 282.6

CO2(g) 213.8 CH3CH2OH(l) 160.7

H2(g) 130.6 CH3CH2CH3(g) Propane 269.9

N2(g) 191.5 CH3(CH2)2CH3(g) n-Butane 310.0

O2(g) 205.0 CH3(CH2)2CH3(l) 231.0

H2O(g) 188.8 C6H6(g) Benzene 269.2

H2O(l) 69.9 C6H6(l) 172.8

NH3(g) 192.3 C12H22O11(s) Sucrose 360.2

Page 11: Chapter 13

Molecular entropy is also linked to the complexity of molecular structure, i.e. the internal motions of the molecules and molar mass.

Standard Molar Entropies (298K, 1 bar)

Compound (g) S° (J/mol۰K)

He 126

Ar 155

CH4 186

C2H6 230

C3H8 270

C4H10 310

Page 12: Chapter 13

Standard Molar Entropies values increase with mass (number of electrons) which leads to more accessible energy levels (microstates)

Page 13: Chapter 13

Problem

Rank the compounds in each of the following groups in order of increasing standard molar entropy, S°.

a. CH4(g), C2H6(g), and C2H8(g)

b. CCl4(l), CHCl3(l), and CH2Cl2(l)

c. CO2(s), CO2(g), and CS2(g)

Find the compounds in Appendix 4 and compare the actual values.

Page 14: Chapter 13

Problem 36

Predict the sign of S for each of the following processes.

a. Zn(s) + 2 HCl(aq) → H2(g) + ZnCl2(aq)

b. C3H8(g) + 5 O2(g) → 3 CO2(g) + 4 H2O(l)

c. N2O5(g) → NO2(g) + NO3(g)

Page 15: Chapter 13

Entropy Calculations

We can calculate the entropy of a chemical reaction using standard molar entropies and the stoichiometry of the balanced chemical equation.

Srxn = nS°[products] – mS°[reactants]

Use the standard molar entropies in Appendix 4 to calculate the S° value for the following reaction.

H2S(g) + 3/2 O2(g) ↔ H2O(g) + SO2(g)

Page 16: Chapter 13
Page 17: Chapter 13
Page 18: Chapter 13

Free Energy

The magnitudes and signs of Ssys and Ssurr determine the magnitude and sign of Suni.

If Suni > 0 then the reaction is spontaneous

Page 19: Chapter 13
Page 20: Chapter 13

Free Energy (Gsys) is the maximum amount of energy available to do work.

For

Gsys < 0 (i.e. negative) the reaction is spontaneous (exergonic).

Gsys > 0 (i.e. positive) the reaction is not spontaneous (endergonic)

Gsys = 0 ; the system is at Equilibrium

Since Gsys depends on temperature, some reactions will become spontaneous as the temperature of the system increases or decreases.

Page 21: Chapter 13

Gibbs Free Energy Function

Gsys = Hsys - TSsys

Changes in entropy, enthalpy and free energy for ice melting

G<0

Page 22: Chapter 13

Calculate and compare values for Ssys and ssurr for the reaction:

H2(g) + ½ O2(g) → H2O(g)

Page 23: Chapter 13
Page 24: Chapter 13

Grxn = nGf°[products] – mGf°[reactants]

Free energy (we now see) is the maximum amount of energy available to do work. It can also be calculated using Standard Free Energy of Formation Values (Appendix 4)

Use the values in Appendix 4 to calculate the G°rxn for the following reaction:

H2S(g) + 3/2 O2(g) ↔ H2O(g) + SO2(g)

Page 25: Chapter 13

Driving Forces for Spontaneous Chemical Processes

1. The formation of low energy products (exothermic processes; H < 0)

2. The formation of products that have greater entropy than the reactants (S > 0).

• The free energy (G) relates enthalpy, entropy, and temperature for a process.

G = H - TS or G = H - TS

Page 26: Chapter 13

Effects of H, S, and T on G*

H S G Spontaneity

<0 >0 Always <0 Always Spontaneous

<0 <0 <0 at low temp Spontaneous at Low Temperatures

>0 >0 <0 at high temp Spontaneous at High Temperatures

>0 <0 Always >0 Never Spontaneous

G = H - TS

Page 27: Chapter 13

Show that hydrogen cyanide (HCN) is a gas at 25°C by estimating its normal boiling point from the following data: 

H°f, kJ/mol S°, J/(mol · K)

HCN(l) 108.9 113

HCN(g) 135.4 202

Page 28: Chapter 13

Spontaneous Processes

• In thermodynamics, a spontaneous process is one that proceeds in a given direction without outside intervention. Spontaneous process can take forever!

• A non-spontaneous process only occurs for as long as energy is continually added to the system.

Page 29: Chapter 13

Thermodynamics

• The second law of thermodynamics states that the total entropy of the universe increases in any spontaneous process.

• Entropy (S) is a measure of the distribution of energy in a system at a specific temperature.

Page 30: Chapter 13

Entropy and Microstates

• Quantum mechanics teaches that energy is not continuous at the atomic scale; only certain levels of energy are possible.

• The motion of molecules is quantized, which means different states are separated by specific energies.

• An energy state, also called an energy level, is an allowed value of energy.

• A microstate is a unique distribution of particles among energy levels.

Page 31: Chapter 13

Motion

• Three types of motion. Translational Rotational Vibrational

• As the temperature of a sample increases, the amount of motion increases.

Page 32: Chapter 13

Energy States

Page 33: Chapter 13
Page 34: Chapter 13

Statistical Entropy• Entropy is related to the number of

microstates by the following equation:S = k ln(W) S is entropy W is the number of microstates* k is the Boltzmann constant (k = 1.38 x 10-23

J/K) *For an ideal gas, W can be counted as

permutations in a range of positions and momenta.

W = N!/Ni!

Page 35: Chapter 13

Ludwig Boltzmann (1844-1906) founded the field of statistical mechanics and statistical thermodynamics. These ideas pre-suppose the existence of (or the reality of) atoms…which were opposed by the leading physicists of the day, in particular Ernst Mach. Boltzmann turned to philosophy to refute objections to his’ theory, but ultimately committed suicide.

Page 36: Chapter 13

Driving the Human Engine

• Exergonic reactions are spontaneous (G < 0).

• Endergonic reactions are nonspontaneous (G > 0).

• The laws of thermodynamics describe the chemical reactions that power the human engine.

Page 37: Chapter 13

Glycolysis

The conversion of glucose to glucose 6-phosphate is the first step in the catabolism (physiological combustion) of starches.

The energy for this process is provided by the hydrolysis of ATP

Page 38: Chapter 13
Page 39: Chapter 13

ChemTour: Entropy

Click to launch animationPC | Mac

This ChemTour includes an “Entropy Battle” game that challenges students to maintain order within a system as the temperature rises and the phase level moves from solid to gas.

Page 40: Chapter 13

ChemTour: Dissolution of Ammonium Nitrate

Click to launch animationPC | Mac

Page 41: Chapter 13

ChemTour: Gibbs Free Energy

Click to launch animationPC | Mac

Students learn to calculate the maximum potential energy available to do work in a system. An interactive “Gibbs free energy calculator” allows students to manipulate variables entropy, enthalpy, and temperature to explore the effect on DG of a reaction.

Page 42: Chapter 13

 

Entropy of Four Atoms in Two Boxes

Shown to the left are three possible configurations (A, B, and C) for placing 4 atoms in two boxes. Which of the following processes is accompanied by the largest increase in entropy, ΔS?

A) A → B B) B → C C) C → A

Page 43: Chapter 13

Entropy of Four Atoms in Two Boxes

Consider the following arguments for each answer and vote again:

A. The entropy change from state A, which has 1 microstate, to state B, which has 4 microstates, is the greatest.

B. State C is the most probable equilibrium state, so the B → C transition has the largest entropy.

C. The entropy of the C → A transition is equal to the sum of the entropies for the A → B and B → C transitions.

Page 44: Chapter 13

 

Isothermal Expansion of an Ideal Gas

An ideal gas in a sealed piston is allowed to expand isothermally and reversibly against an external pressure of 1.0 atm. What can be said of the change in the entropy of the surroundings, ΔSsurr, for this process?

A) ΔSsurr > 0 B) ΔSsurr = 0 C) ΔSsurr < 0

Page 45: Chapter 13

Isothermal Expansion of an Ideal Gas

Consider the following arguments for each answer

and vote again:

A. The gas is doing work, thereby increasing the entropy of the surroundings.

B. For a reversible expansion, entropy is constant, so ΔSsys = ΔSsurr = ΔSuniv = 0.

C. The expansion is isothermal, ΔSsys > 0, and reversible, ΔSuniv = 0. Therefore, ΔSsurr < 0.

Page 46: Chapter 13

 

Gas Expansion into a Vacuum

An ideal gas is expanded adiabatically (q = 0) into a vacuum. Which of the following statements is true for this process?

A) ΔEsys < 0 B) ΔGsys < 0 C) ΔSsys < 0

Page 47: Chapter 13

Gas Expansion into a Vacuum

Consider the following arguments for each answer

and vote again:

A. During the expansion, the gas performs work, so the energy decreases.

B. The expansion of a gas into a vacuum is a spontaneous process, so ΔGsys is negative.

C. Although the gas volume increases, the temperature decreases dramatically, thereby reducing the entropy.

Page 48: Chapter 13

 

Formation of CH2Cl2 from CH4 and CCl4

Consider the following possible gas phase reaction:

Which of the following is probably true for this reaction?

A) ΔH > 0 B) ΔS > 0 C) ΔG > 0

Page 49: Chapter 13

Formation of CH2Cl2 from CH4 and CCl4

Consider the following arguments for each answer

and vote again:

A. It is energetically more favorable to have all of the same type of bonds in a molecule than it is to mix and match.

B. There are more microstates for the arrangements of H and Cl atoms on 2 CH2Cl2 molecules than on a CH4 and a CCl4 molecule.

C. Free energy is required to accommodate formation of the electric dipole moment on CH2Cl2.

Page 50: Chapter 13

 

ΔG° for Condensation of Water at 25° C

What can be said of ΔG° for the condensation of water vapor,H2O(g)     →     H2O(),at 25°C if the partial pressure of H2O(g) is 1.0 atm?

A) ΔG° > 0 B) ΔG° = 0 C) ΔG° < 0

Page 51: Chapter 13

ΔG° for Condensation of Water at 25° C

Consider the following arguments for each answer

and vote again:

A. The vaporization of water is spontaneous when the partial pressure of H2O(g) is 1.0 atm at 25°C. Therefore, ΔG° > 0 for the condensation of water vapor.

B. At 25°C, condensation will occur spontaneously only when the partial pressure of H2O(g) rises above the equilibrium partial pressure of 1.0 atm.

C. The equilibrium partial pressure of H2O(g) is less than 1.0 atm at 25°C, so water vapor will condense spontaneously.

Page 52: Chapter 13

 

ΔG° of Vaporization of Ethanol

To the left is a plot of vapor pressure versus temperature for the vaporization of ethanol.

C2H5OH(λ) → C2H5OH(g).

At which temperature is ΔG° = 0 for the vaporization of ethanol at 1.0 atm?

A) > 100°C B) 100°C C) < 100°C

Page 53: Chapter 13

ΔG° of Vaporization of Ethanol

Consider the following arguments for each answer

and vote again:

A. Ethanol has a higher molecular mass than water and so requires more heat for vaporization.

B. The temperature at which ΔG° = 0 for vaporization is 100°C for all liquids.

C. For ethanol, ΔG° = 0 when the vapor pressure equals 1.0 atm, which occurs at a temperature lower than 100°C.

Page 54: Chapter 13

 

ΔG° Versus T for the Sublimation of I2(s)

Which of the following plots shows the correct relationship between ΔG° (y-axis) and temperature (x-axis) for the sublimation of solid iodine to iodine vapor at 1.0 atm?

A) B) C)

Page 55: Chapter 13

ΔG° Versus T for the Sublimation of I2(s)

Consider the following arguments for each answer

and vote again:

A. Once the temperature becomes high enough that the equilibrium partial pressure of I2(g) is greater than 1.0 atm, the reaction will be spontaneous.

B. This process becomes less spontaneous at higher temperatures because more iodine must be vaporized.

C. As the temperature increases and the system approaches equilibrium, ΔG° will decrease. When the system moves past equilibrium, ΔG° will begin to increase.

Page 56: Chapter 13

 

Spontaneity of Ozone Formation

The formation of ozone, O3(g), from molecular oxygen is an endothermic process, with ΔH° = 85 J/mole.

3 O2(g) 2 O3(g)

At what temperatures will the reaction proceed spontaneously if PO2 = PO3 = 1.0 atm?

A) High temperatures B) Low temperatures C) No temperatures

Page 57: Chapter 13

Spontaneity of Ozone Formation

Consider the following arguments for each answer

and vote again:

A. Because the formation of ozone is an endothermic reaction, it will be spontaneous only at high temperatures.

B. The formation of ozone will occur only at low temperatures, where the O2(g) molecules will begin to condense and form O3(g) molecules.

C. The reaction is endothermic and ΔS° < 0, so at no temperature can this reaction be spontaneous at 1.0 atm.