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Chapter 17 Spontaneity, entropy and free energy

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Page 1: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17

Spontaneity, entropy and free energy

Page 2: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17Thermodynamics: Spontaneity,

Entropy, and Free Energy

General Chemistry: An Integrated Approach

Hill, Petrucci, 4th Edition

Mark P. HeitzState University of New York at Brockport

© 2005, Prentice Hall, Inc.

Page 3: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 3

Introductory Concepts Thermodynamics examines the relationship between heat (q) and work (w)

Spontaneity is the notion of whether or not a process can take place unassisted

Entropy is a measure of how energy is spread out among the particles of a system

EOS

Page 4: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 4

Introductory Concepts

Free energy is a thermodynamic function that relates enthalpy and entropy to spontaneity

EOS

Free energy is connected with the ability to do work

e.g., the chemical reaction in a battery generates electricity to light a flashlight bulb

Page 5: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 5

Spontaneous ChangeA spontaneous process is one that can occur in a system left to itself; no action from outside the system is necessary to bring the change about

Example: spontaneous combustion of damp hay or silo explosions from gases evolved from decomposing grain

EOS

If a process is spontaneous, the reverse process is nonspontaneous and vice versa

Page 6: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 6

Spontaneity A general rule: that exothermic reactions are spontaneous and endothermic reactions are nonspontaneous works in many cases

EOS

However, enthalpy change is not a sufficient criterion for predicting spontaneous change

Page 7: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 7

The Concept of EntropyConsider mixing two gases: this occurs spontaneously, and the gases form a homogeneous mixture.

The driving force is a thermodynamic quantity called entropy, a mathematical concept that is difficult to portray visually

EOS

There is essentially no enthalpy change involved, so why is the process spontaneous?

Page 8: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 8

Entropy The total energy of a system remains unchanged in the mixing of the gases but the number of possibilities for the distribution of that energy increases

This spreading of the energy and increase of entropy correspond to a greater physical disorder at the microscopic level

EOS

Page 9: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 9

EntropyThere are two natural tendencies behind spontaneous processes: the tendency to achieve a lower energy state and the tendency toward a more disordered state

EOS

Page 10: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 10

Entropy (S)

Entropy (S) is a state function: it is path independent

Sfinal – Sinit = S

EOS

S = qrev/T

The greater the number of configurations of the microscopic particles (atoms, ions, molecules) among the energy levels in a particular state of a system, the greater the entropy of the system

Page 11: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 11

Reversible Process

A process that is never more than an infinitesimal step away from equilibrium

EOS

The process can reverse directions by a miniscule change in a variable

Page 12: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 12

Standard Molar EntropiesThe standard molar entropy, So, is the entropy of one mole of a substance in its standard state.

S = vpSo(products) – vrSo(reactants)

EOS

According to the Third Law of Thermodynamics, the entropy of a pure, perfect crystal can be taken to be zero at 0 K

Page 13: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 13

Standard Molar EntropiesIn general, the more atoms in its molecules, the greater is the entropy of a substance

EOS

Entropy is a function of temperature

Page 14: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 14

The Second Lawof Thermodynamics

The Second Law of Thermodynamics establishes that all spontaneous or natural processes increase the entropy of the universe

Stotal = Suniverse = Ssystem + Ssurroundings

EOS

In a process, if entropy increases in both the system and the surroundings, the process is surely spontaneous

Page 15: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 15

Free Energy ChangeThe free energy change (G) for a process at constant temperature and pressure is given by the Gibbs equation

Gsys = Hsys – TSsys

EOS

If G < 0 (negative), a process is spontaneous.

If G > 0 (positive), a process is nonspontaneous.

If G = 0, the process is at equilibrium.

Page 16: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 16

Criterion for Spontaneous Change

EOS

Page 17: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 17

Standard Free Energy Change

The standard free energy change, Go, of a reaction is the free energy change when reactants and products are in their standard states

e.g., O2 is a gas, Br2 is liquid, etc. ...

Go = Ho – TSo

EOS

Be mindful of units; H is usually in kJ and S is in J K–1

Page 18: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 18

Standard Free Energy Change

The standard free energy of formation, Gof, is

the free energy change that occurs in the formation of 1 mol of a substance in its standard state from the reference forms of its elements in their standard states

EOS

Go = vp Gof(products) – vr Go

f(reactants)

Page 19: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 19

Free Energy Changeand Equilibrium

At equilibrium, G = 0. Therefore, at the equilibrium temperature, the free energy change expression becomes

H = TS and S = H/T

EOS

Entropy and enthalpy of vaporization can be related to normal boiling point

Page 20: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 20

Vaporization Energies

Trouton’s rule implies that about the same amount of disorder is generated in the passage of one mole of substance from liquid to vapor when comparisons are made at the normal boiling point

EOS

S°vapn = H°vapn/Tbp 87 J mol–1 K–1

Page 21: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 21

Trouton’s Rule This rule works best with nonpolar substances and generally fails for liquids with a more ordered structure, such as those with extensive hydrogen bonding

EOS

Page 22: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 22

Raoult’s Law Revisited

Psolv = xsolv · Posolv

EOS

Because the mole fraction of solvent in a solution (xsolv) is less than 1, the vapor pressure of the solvent (Psolv) in an ideal solution is lower than that of the pure solvent (Po

solv)

Page 23: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 23

Raoult’s Law RevisitedA solution has a higher entropy than the pure solvent

Because a solution has a higher entropy than the pure solvent, the vapor from the solution must also have a higher entropy than the vapor from the pure solvent

EOS

The entropy of the vapor increases if molecules can roam more freely, that is, they are at a lower pressure

Page 24: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 24

Relationship of Go and Keq

G = 0 is a criterion for equilibrium at a single temperature, the one temperature at which the equilibrium state has all reactants and products in their standard states

G and Go are related through the reaction quotient, Q

G = Go + RT ln Q

Under the conditions of G = 0 and Q = Keq, the equation above becomes

EOS

Go = RT ln Keq

Page 25: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 25

The Equilibrium Constant, Keq

Activities are the dimensionless quantities needed in the equilibrium constant expression Keq

For pure solid and liquid phases: activity, a, = 1

For gases: Assume ideal gas behavior, and replace the activity by the numerical value of the gas partial pressure in atm.

EOS

For solutes in aqueous solution: Assume intermolecular or interionic attractions are negligible and replace solute activity by the numerical value of the solute molarity

Page 26: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 26

The Significance of the Sign and Magnitude of Go

Go is a large, negative quantity and equilibrium is very far to the right

Gprod << Greac

EOS

Page 27: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 27

The Significance of the Sign and Magnitude of Go

Go is a large, positive quantity and equilibrium is very far to the left

Gprod >> Greac

EOS

Page 28: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 28

The Significance of the Sign and Magnitude of Go

the equilibrium lies more toward the center of the reaction profile

Gprod Greac

EOS

Page 29: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 29

The Dependence ofGo and Keq on Temperature

To obtain equilibrium constants at different temperatures, it will be assumed that H and S do not change much with temperature

EOS

the 25 oC values of Ho and So along with the desired temperature are substituted

Go = Ho – TSo

Page 30: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

G=H-TSHS Spontaneous?

+ - At all Temperatures

+ + At high temperatures,

“entropy driven”

- - At low temperatures,

“enthalpy driven”

+- Not at any temperature,

Reverse is spontaneous

Page 31: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 31

The Dependence ofGo and Keq on Temperature

To obtain Keq at the desired temperature, the following equation is used …

EOS

This is the van’t Hoff equation

2eq

1 1 2

1 1ln lnoK HK

K R T T

Page 32: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 32

Equilibrium with VaporHo for either sublimation or vaporization is used depending on the other component

EOS

This is the Clausius–Clapeyron equation

211

2 11ln

TTR

H

P

Povap

Partial pressures are exchanged for K’s

Page 33: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 33

Temperature Dependence of Keq

EOS

Page 34: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 34

Summary of Concepts

• A spontaneous change is one that occurs by itself without outside intervention

• The third law of thermodynamics states that the entropy of a pure, perfect crystal at 0 K can be taken to be zero

• The direction of spontaneous change is that in which total entropy increases

EOS

• The free energy change, G, is equal to –TS, and it applies just to the system itself

Page 35: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 35

Summary (cont’d)

• The standard free energy change, Go, can be calculated by substituting standard enthalpies and entropies of reaction and a Kelvin temperature into the Gibbs equation, or, by combining standard free energies of formation

EOS

• The condition of equilibrium is one for which G = 0

Page 36: Chapter 17 Spontaneity, entropy and free energy. Chapter 17 Thermodynamics: Spontaneity, Entropy, and Free Energy General Chemistry: An Integrated Approach

Chapter 17: Thermodynamics 36

Summary (cont’d)

• The value of Go is in itself often sufficient to determine how a reaction will proceed

• Values of Gof, Ho

f, and S are generally tabulated for 25 oC. To obtain values of Keq at other temperatures, the van’t Hoff equation must be used

EOS

• The Clausius–Clapeyron equation connects solid/vapor or liquid/vapor equilibria to varying temperature