thermodynamics of reactions spontaneity, entropy, and free energy chapter 16

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Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

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Page 1: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Thermodynamics of Reactions

Spontaneity, Entropy, and Free Energy

Chapter 16

Page 2: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

1st Law of Thermodynamics

• The energy of the universe is constant

• (conservation of energy)

Page 3: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Spontaneous Processes

• Can be fast OR slow. • Occurs without outside

intervention

Page 4: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

True, or Not True?

• Ball rolls downhill spontaneously.• Ball rolls uphill spontaneously.• Wood burns spontaneously in O2.• CO2 and H2O spontaneously form

wood.• Steel rusts spontaneously.• Rust spontaneously turns into iron

and water.

Page 5: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Its All About Entropy

• Entropy is…• All about the ability of energy to spread

out• Related to probability.• Over-simplified to be about disorder.

Page 6: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Positional Entropy

• When a substance has more opportunities to exist, (ie, particles can have more than one arrangement) it is also said to have more positional entropy.

• Increasing moles of gas• Increasing volume• Decreasing pressure• Changing state of matter ( s l g )• Exothermic rxns **

Page 7: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Try Me Conceptual

• Determine which of the following pairs has the most positional entropy:

− 1 mol H2 at STP or 1 Mol H2 at 100oC, 0.5 atm

− 1 mol N2 at STP or 1 mol N2 at 100 K 2atm

− 1 mol H2O(s) at 0oC or 1 mole H2O(l) at 20oC

Page 8: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

2nd Law of Thermodynamics

• Spontaneous processes increase the entropy of the universe.

Suniverse = Ssystem + Ssurroundings

Page 9: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

The Value of S

• Sign is determined by enthalpy:− exothermic− endothermic

• Magnitude is determined by temperature

T

HS gssurroundin

Page 10: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Try Me Calculation

• The melting point of tungsten (W) is the second highest among the elements, at 3680 K. The enthalpy of fusion for this metal is 35.2 kJ/mol. What is the entropy of fusion?

Page 11: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

3rd Law of Thermodynamics

The entropy of a perfect crystal at 0 Kelvin is zero.

In PhaseOut of Phase

Angle BendingRotation

Translation

Page 12: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Entropy for a chemical reaction

Sorxn = nSo

p - nSor

Page 13: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Try Me

• Calculate the change in entropy at 25oC for the reaction:

2 NiS + 3 O2 2 SO2 + 2 NiO

Given Entropy Values:SO2 = 248 J/KmolNiO = 38 J/KmolO2 = 205 J/KmolNiS = 53 J/Kmol

Page 14: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Free Energy

• Gibbs Free Energy- another method for determining spontaneity.

• Also indicates the amount of available energy that is capable of doing work.

• As an energy source is used, the energy is not destroyed, only converted to a non-usable form.

Page 15: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

G = H - TS

• Defines Gibbs energy in terms of enthalpy and entropy.

• All three factors will contribute to reaction spontaneity.

• When G is negative, the reaction is spontaneous.

Page 16: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Rearrange that formula

• Lets start with the following 3 formulae:

G = H –TSSsurr = -H/T

Suniv = Ssurr + Ssyst

Suniverse = - G /T

Page 17: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Fancy Pants Charts

HH SS GG Spontaneous?

__ + __ Always

__ __ +/- When temp is low

+ + +/- When temp is high

+ __ + Never

Page 18: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Free Energy in Chemical Reactions

• Standard Free energy is used so that we can compare the relative tendency to occur.

• Go = Ho – TSo

Page 19: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

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

• The above rxn. Occurs at 25oC and 1 atm. Calculate Ho, So, and Go using the following data:

substance Hof So

kJ/mol J/Kmol

SO2(g) -297 248

SO3(g) -396 257

O2(g) 0 205

Page 20: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

It also works like Hess’s Law problems:

What is the Go for the reaction if the mechanism is:

Cdi(s) + O2(g) CO2(g) Go = -397kJ

Cgr(s) + O2(g) CO2(g) Go = -394 kJ

Page 21: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Dependence on Pressure

• Enthalpy does not depend on pressure.

• Entropy does depend on temperature.

S low pressure > S high pressure

Page 22: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

G = Go + RT ln(P)

• This can be adapted to reflect partial pressures for the reaction it describes. When that occurs, the formula can be re-written:

Go = -RT ln(Q)

Page 23: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

@ Equilibrium

• K = Q• The free energy is the lowest

possible it will ever be for the system.

Page 24: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Try Me Out

• The overall rxn for rusting iron by oxygen is

4Fe(s) + 3O2(g) 2 Fe2O3(s)

@25oC, find the equilibrium constant given:

Substance Ho So

Fe2O3(s) -826 90Fe(s) 0 27O2(g) 0 205

Page 25: Thermodynamics of Reactions Spontaneity, Entropy, and Free Energy Chapter 16

Free Energy and Work

• Achieving the maximum amount of work from a process is highly unlikely because of transfers of energy.

• G represents the maximum possible quantity of work a system is capable of doing.