SlideShare a Scribd company logo
1 of 57
Download to read offline
Thermodynamics
and Equilibrium
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–2
– We introduced the thermodynamic property of
enthalpy, H, in Chapter 6.
– We noted that the change in enthalpy equals the
heat of reaction at constant pressure.
Thermodynamics
• Thermodynamics is the study of the
relationship between heat and other
forms of energy in a chemical or
physical process.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–3
– Heat is energy that moves into or out of a system
because of a temperature difference between
system and surroundings.
– Work, on the other hand, is the energy exchange
that results when a force F moves an object
through a distance d; work (w) = FĂ—d
First Law of Thermodynamics
• To state the laws of thermodynamics,
we must first understand the internal
energy of a system and how you can
change it.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–4
– Remembering our sign convention.
Work done by the system is negative.
Work done on the system is positive.
Heat evolved by the system is negative.
Heat absorbed by the system is positive.
First Law of Thermodynamics
• To state the laws of thermodynamics,
we must first understand the internal
energy of a system and how you can
change it.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–5
– In general, the first law of thermodynamics
states that the change in internal energy, ΔU,
equals heat plus work.
First Law of Thermodynamics
• To state the laws of thermodynamics, we
must first understand the internal energy of a
system and how you can change it.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–6
– We do not calculate this, only think of how
expanding volume can move something.
Heat of Reaction and Internal Energy
• When a reaction is run in an open
vessel (at constant P), any gases
produced represent a potential source
of “expansion” work.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–7
– Examples include:
A rock at the top of a hill rolls down.
Heat flows from a hot object to a cold one.
An iron object rusts in moist air.
– These processes occur without requiring an
outside force and continue until equilibrium is
reached.
Spontaneous Processes and Entropy
• A spontaneous process is a physical or
chemical change that occurs by itself.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–8
– Entropy, S , is a thermodynamic quantity
that is a measure of the randomness or
disorder of a system.
– The SI unit of entropy is joules per Kelvin
(J/K) and, like enthalpy, is a state function.
Entropy and the Second Law of
Thermodynamics
• The second law of thermodynamics
addresses questions about spontaneity
in terms of a quantity called entropy.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–9
– When temperature is raised, however, the
substance becomes more disordered as it
absorbs heat.
– The entropy of a substance is determined
by measuring how much heat is required to
change its temperature per Kelvin degree.
Standard Entropies and the Third Law
of Thermodynamics
• The third law of thermodynamics
states that a substance that is perfectly
crystalline at 0 K has an entropy of zero.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–10
– Standard state implies 25 o
C, 1 atm
pressure, and 1 M for dissolved
substances.
Standard Entropies and the Third Law
of Thermodynamics
• The standard entropy of a substance
or ion (Table 19.1), also called its
absolute entropy, So
, is the entropy
value for the standard state of the
species.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–11
– Note that the elements have nonzero values,
unlike standard enthalpies of formation, ΔHf
o
,
which by convention, are zero.
Standard Entropies and the Third Law
of Thermodynamics
• The standard entropy of a substance
or ion (Table 19.1), also called its
absolute entropy, So
, is the entropy
value for the standard state of the
species.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–12
– The symbol So
, rather than ΔSo
, is used for
standard entropies to emphasize that they
originate from the third law.
Standard Entropies and the Third Law
of Thermodynamics
• The standard entropy of a substance
or ion (Table 19.1), also called its
absolute entropy, So
, is the entropy
value for the standard state of the
species.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–13
– Even without knowing the values for the entropies
of substances, you can sometimes predict the sign
of ΔSo
for a reaction.
Entropy Change for a Reaction
• You can calculate the entropy change
for a reaction using a summation law,
similar to the way you obtained ΔSo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–14
1. A reaction in which a molecule is broken into
two or more smaller molecules.
– The entropy usually increases in the
following situations:
Entropy Change for a Reaction
• You can calculate the entropy change
for a reaction using a summation law,
similar to the way you obtained ΔSo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–15
– The entropy usually increases in the
following situations:
2. A reaction in which there is an increase in the
moles of gases.
Entropy Change for a Reaction
• You can calculate the entropy change
for a reaction using a summation law,
similar to the way you obtained ΔSo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–16
– The entropy usually increases in the
following situations:
3. A process in which a solid changes to liquid or
gas or a liquid changes to gas.
Entropy Change for a Reaction
• You can calculate the entropy change
for a reaction using a summation law,
similar to the way you obtained ΔSo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–17
– The calculation is similar to that used to obtain
ΔHo
from standard enthalpies of formation.
A Problem To Consider
• Calculate the change in entropy, ΔSo
, at 25o
C
for the reaction in which urea is formed from
NH3
and CO2
. The standard entropy of
NH2
CONH2
is 174 J/(mol.K). See Table 19.1
for other values.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–18
– It is convenient to put the standard entropies
(multiplied by their stoichiometric coefficients)
below the formulas.
So
: 2 x 193 214 174 70
A Problem To Consider
• Calculate the change in entropy, ΔSo
, at 25o
C
for the reaction in which urea is formed from
NH3
and CO2
. The standard entropy of
NH2
CONH2
is 174 J/(mol.K). See Table 19.1
for other values.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–19
– We can now use the summation law to calculate
the entropy change.
A Problem To Consider
• Calculate the change in entropy, ΔSo
, at 25o
C
for the reaction in which urea is formed from
NH3
and CO2
. The standard entropy of
NH2
CONH2
is 174 J/(mol.K). See Table 19.1
for other values.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–20
A Problem To Consider
• Calculate the change in entropy, ΔSo
, at 25o
C
for the reaction in which urea is formed from
NH3
and CO2
. The standard entropy of
NH2
CONH2
is 174 J/(mol.K). See Table 19.1
for other values.
– We can now use the summation law to calculate
the entropy change.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–21
– This quantity gives a direct criterion for
spontaneity of reaction.
Free Energy Concept
• The American physicist J. Willard Gibbs
introduced the concept of free energy
(sometimes called the Gibbs free energy),
G, which is a thermodynamic quantity defined
by the equation G=H-TS.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–22
– Thus, if you can show that ΔG is negative
at a given temperature and pressure, you
can predict that the reaction will be
spontaneous.
Free Energy and Spontaneity
• Changes in H an S during a reaction
result in a change in free energy, ΔG ,
given by the equation
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–23
– The next example illustrates the calculation
of the standard free energy change, ΔGo
,
from ΔHo
and ΔSo
.
Standard Free-Energy Change
• The standard free energy change, ΔGo
,
is the free energy change that occurs
when reactants and products are in their
standard states.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–24
ΔHo
ΔSo
ΔGo
Description
– + – Spontaneous at all T
+ – + Nonspontaneous at all T
– – + or – Spontaneous at low T;
Nonspontaneous at high T
+ + + or – Nonspontaneous at low T;
Spontaneous at high T
Spontaneity and Temperature Change
• All of the four possible choices of signs for
ΔHo
and ΔSo
give different temperature
behaviors for ΔGo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–25
– Place below each formula the values of ΔHf
o
and
So
multiplied by stoichiometric coefficients.
So
: 3 x 130.6
191.5 2 x 193 J/K
ΔHf
o
: 0
0 2 x (-45.9) kJ
A Problem To Consider
• What is the standard free energy change, ΔGo
,
for the following reaction at 25o
C? Use values
of ΔHf
o
and So
, from Tables 6.2 and 19.1.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–26
– You can calculate ΔHo
and ΔSo
using their
respective summation laws.
A Problem To Consider
• What is the standard free energy change, ΔGo
,
for the following reaction at 25o
C? Use values
of ΔHf
o
and So
, from Tables 6.2 and 19.1.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–27
– You can calculate ΔHo
and ΔSo
using their
respective summation laws.
A Problem To Consider
• What is the standard free energy change, ΔGo
,
for the following reaction at 25o
C? Use values
of ΔHf
o
and So
, from Tables 6.2 and 19.1.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–28
– Now substitute into our equation for ΔGo
. Note that
ΔSo
is converted to kJ/K.
A Problem To Consider
• What is the standard free energy change, ΔGo
,
for the following reaction at 25o
C? Use values
of ΔHf
o
and So
, from Tables 6.2 and 19.1.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–29
– By tabulating ΔGf
o
for substances, as in Table
19.2, you can calculate the ΔGo
for a reaction by
using a summation law.
Standard Free Energies of Formation
• The standard free energy of formation,
ΔGf
o
, of a substance is the free energy
change that occurs when 1 mol of a
substance is formed from its elements in their
stablest states at 1 atm pressure and 25o
C.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–30
ΔGf
o
: -174.8 0 2(-394.4) 3(-228.6)kJ
– Place below each formula the values of ΔGf
o
multiplied by stoichiometric coefficients.
A Problem To Consider
• Calculate ΔGo
for the combustion of 1 mol of
ethanol, C2
H5
OH, at 25o
C. Use the standard
free energies of formation given in Table
19.2.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–31
ΔGf
o
: -174.8 0 2(-394.4) 3(-228.6)kJ
– You can calculate ΔGo
using the summation law.
A Problem To Consider
• Calculate ΔGo
for the combustion of 1 mol of
ethanol, C2
H5
OH, at 25o
C. Use the standard
free energies of formation given in Table 19.2.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–32
– You can calculate ΔGo
using the summation law.
A Problem To Consider
ΔGf
o
: -174.8 0 2(-394.4) 3(-228.6)kJ
ΔGf
o
: -174.8 0 2(-394.4) 3(-228.6)kJ
• Calculate ΔGo
for the combustion of 1 mol of
ethanol, C2
H5
OH, at 25o
C. Use the standard
free energies of formation given in Table 19.2.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–33
1. When ΔGo
is a large negative number
(more negative than about –10 kJ), the
reaction is spontaneous as written, and
the reactants transform almost entirely to
products when equilibrium is reached.
ΔGo
as a Criteria for Spontaneity
• The following rules are useful in judging
the spontaneity of a reaction.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–34
2. When ΔGo
is a large positive number
(more positive than about +10 kJ), the
reaction is nonspontaneous as written,
and reactants do not give significant
amounts of product at equilibrium.
• The following rules are useful in judging
the spontaneity of a reaction.
ΔGo
as a Criteria for Spontaneity
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–35
3. When ΔGo
is a small negative or positive
value (less than about 10 kJ), the reaction
gives an equilibrium mixture with
significant amounts of both reactants
and products.
• The following rules are useful in judging
the spontaneity of a reaction.
ΔGo
as a Criteria for Spontaneity
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–36
– Figure 19.9 illustrates the change in free energy
during a spontaneous reaction.
– As the reaction proceeds, the free energy
eventually reaches its minimum value.
– At that point, ΔG = 0, and the net reaction stops; it
comes to equilibrium.
Free Energy Change During Reaction
• As a system approaches equilibrium,
the instantaneous change in free energy
approaches zero.
Figure 19.9 Free-energy change during a spontaneous reaction.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–38
– Here Q is the thermodynamic form of the
reaction quotient.
Relating ΔGo
to the Equilibrium
Constant
• The free energy change when reactants
are in non-standard states (other than
1 atm pressure or 1 M) is related to the
standard free energy change, ΔGo
, by
the following equation.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–39
– ΔG represents an instantaneous change in
free energy at some point in the reaction
approaching equilibrium.
• The free energy change when reactants
are in non-standard states (other than
1 atm pressure or 1 M) is related to the
standard free energy change, ΔGo
, by
the following equation.
Relating ΔGo
to the Equilibrium
Constant
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–40
– At equilibrium, ΔG=0 and the reaction
quotient Q becomes the equilibrium
constant K.
• The free energy change when reactants
are in non-standard states (other than
1 atm pressure or 1 M) is related to the
standard free energy change, ΔGo
, by
the following equation.
Relating ΔGo
to the Equilibrium
Constant
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–41
– At equilibrium, ΔG=0 and the reaction
quotient Q becomes the equilibrium
constant K.
• The free energy change when reactants
are in non-standard states (other than
1 atm pressure or 1 M) is related to the
standard free energy change, ΔGo
, by
the following equation.
Relating ΔGo
to the Equilibrium
Constant
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–42
– When K > 1 , the ln K is positive and ΔGo
is
negative.
– When K < 1 , the ln K is negative and ΔGo
is positive.
• This result easily rearranges to give the
basic equation relating the standard
free-energy change to the equilibrium
constant.
Relating ΔGo
to the Equilibrium
Constant
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–43
– Rearrange the equation ΔGo
=-RTlnK to give
A Problem To Consider
• Find the value for the equilibrium constant, K,
at 25o
C (298 K) for the following reaction. The
standard free-energy change, ΔGo
, at 25o
C
equals –13.6 kJ.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–44
– Substituting numerical values into the equation,
A Problem To Consider
• Find the value for the equilibrium constant, K,
at 25o
C (298 K) for the following reaction. The
standard free-energy change, ΔGo
, at 25o
C
equals –13.6 kJ.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–45
– Hence,
A Problem To Consider
• Find the value for the equilibrium constant, K,
at 25o
C (298 K) for the following reaction. The
standard free-energy change, ΔGo
, at 25o
C
equals –13.6 kJ.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–46
ΔHo
ΔSo
ΔGo
Description
– + – Spontaneous at all T
+ – + Nonspontaneous at all T
– – + or – Spontaneous at low T;
Nonspontaneous at high T
+ + + or – Nonspontaneous at low T;
Spontaneous at high T
Spontaneity and Temperature Change
• All of the four possible choices of signs for
ΔHo
and ΔSo
give different temperature
behaviors for ΔGo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–47
– You get the value of ΔGT
o
at any temperature T by
substituting values of ΔHo
and ΔSo
at 25 o
C into the
following equation.
Calculation of ΔGo
at Various
Temperatures
• In this method you assume that ΔHo
and ΔSo
are essentially constant with respect to
temperature.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–48
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
– Place below each formula the values of ΔHf
o
and
So
multiplied by stoichiometric coefficients.
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–49
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
– You can calculate ΔHo
and ΔSo
using their
respective summation laws.
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–50
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–51
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–52
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
– Now you substitute ΔHo
, ΔSo
(=0.1590 kJ/K), and
T (=298K) into the equation for ΔGf
o
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–53
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
– Now you substitute ΔHo
, ΔSo
(=0.1590 kJ/K), and
T (=298K) into the equation for ΔGf
o
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–54
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
– Now you substitute ΔHo
, ΔSo
(=0.1590 kJ/K), and
T (=298K) into the equation for ΔGf
o
.
So the reaction is
nonspontaneous
at 25o
C.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–55
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
– Now we’ll use 1000o
C (1273 K) along with our
previous values for ΔHo
and ΔSo
.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–56
So
: 38.2
92.9 213.7 J/K
ΔHf
o
: -635.1
-1206.9 -393.5 kJ
A Problem To Consider
• Find the ΔGo
for the following reaction at 25o
C
and 1000o
C. Relate this to reaction
spontaneity.
– Now we’ll use 1000o
C (1273 K) along with our
previous values for ΔHo
and ΔSo
.
So the reaction is
spontaneous at
1000o
C.
Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–57
Operational Skills
• Calculating the entropy change for a phase transition
• Predicting the sign of the entropy change of a reaction
• Calculating ΔSo
for a reaction
• Calculating ΔGo
from ΔHo
and ΔSo
• Calculating ΔGo
from standard free energies of
formation
• Interpreting the sign of ΔGo
• Writing the expression for a thermodynamic
equilibrium constant
• Calculating K from the standard free energy change
• Calculating ΔGo
and K at various temperatures

More Related Content

Similar to chapter_19 General Chemistry: Thermodynamics and Equilbrium

Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,
Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,
Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,chaturvedijay62
 
Chem7250p4.ppt
Chem7250p4.pptChem7250p4.ppt
Chem7250p4.pptssuser022dab
 
chemical-thermodynamics-2 (3).pptcscscscscs
chemical-thermodynamics-2 (3).pptcscscscscschemical-thermodynamics-2 (3).pptcscscscscs
chemical-thermodynamics-2 (3).pptcscscscscsAliceRivera13
 
Chem7250p4.ppt
Chem7250p4.pptChem7250p4.ppt
Chem7250p4.pptvaskane
 
Chapter 5 lecture- Thermochemistry
Chapter 5 lecture- ThermochemistryChapter 5 lecture- Thermochemistry
Chapter 5 lecture- ThermochemistryMary Beth Smith
 
THE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGY
THE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGYTHE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGY
THE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGYRIYASAMSON
 
Chapter 19
Chapter 19Chapter 19
Chapter 19ewalenta
 
Spontaneity-Entropy-and-Free-Energy.ppt
Spontaneity-Entropy-and-Free-Energy.pptSpontaneity-Entropy-and-Free-Energy.ppt
Spontaneity-Entropy-and-Free-Energy.pptKrizellaKateMagdarao
 
Jatin bhatia art integration project 22
Jatin bhatia art integration project 22Jatin bhatia art integration project 22
Jatin bhatia art integration project 22Dav public school Rohtak
 
1 handout.ppt
1 handout.ppt1 handout.ppt
1 handout.pptRanendraRoy2
 
Chemical Engineering desciption, laws.ppt
Chemical Engineering desciption, laws.pptChemical Engineering desciption, laws.ppt
Chemical Engineering desciption, laws.pptEminaKarahmet1
 
First law of thermodynamics
First law of thermodynamicsFirst law of thermodynamics
First law of thermodynamicsMattSmith321834
 
Chapter 1 - Introduction.pptx
Chapter 1 - Introduction.pptxChapter 1 - Introduction.pptx
Chapter 1 - Introduction.pptxssuser7892e7
 
chemical equilibrium and thermodynamics
chemical equilibrium and thermodynamicschemical equilibrium and thermodynamics
chemical equilibrium and thermodynamicsAayashaNegi
 

Similar to chapter_19 General Chemistry: Thermodynamics and Equilbrium (20)

Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,
Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,
Chem7250p4.pptsmn..nnfsknvsk,nvs,mnvsk,jdnlsk,
 
Chem7250p4.ppt
Chem7250p4.pptChem7250p4.ppt
Chem7250p4.ppt
 
Chem7250p4.ppt
Chem7250p4.pptChem7250p4.ppt
Chem7250p4.ppt
 
chemical-thermodynamics-2 (3).pptcscscscscs
chemical-thermodynamics-2 (3).pptcscscscscschemical-thermodynamics-2 (3).pptcscscscscs
chemical-thermodynamics-2 (3).pptcscscscscs
 
Chem7250p4.ppt
Chem7250p4.pptChem7250p4.ppt
Chem7250p4.ppt
 
THERMODYNAMICS.pptx
THERMODYNAMICS.pptxTHERMODYNAMICS.pptx
THERMODYNAMICS.pptx
 
Thermodynamics
ThermodynamicsThermodynamics
Thermodynamics
 
CHE 101 Thermochem.ppt
CHE 101 Thermochem.pptCHE 101 Thermochem.ppt
CHE 101 Thermochem.ppt
 
Chapter 5 lecture- Thermochemistry
Chapter 5 lecture- ThermochemistryChapter 5 lecture- Thermochemistry
Chapter 5 lecture- Thermochemistry
 
Thermodynamics 1.pdf
Thermodynamics 1.pdfThermodynamics 1.pdf
Thermodynamics 1.pdf
 
THE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGY
THE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGYTHE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGY
THE CONCEPT OF ENTHALPY, ENTROPY AND FREE ENERGY
 
Chapter 19
Chapter 19Chapter 19
Chapter 19
 
Spontaneity-Entropy-and-Free-Energy.ppt
Spontaneity-Entropy-and-Free-Energy.pptSpontaneity-Entropy-and-Free-Energy.ppt
Spontaneity-Entropy-and-Free-Energy.ppt
 
Jatin bhatia art integration project 22
Jatin bhatia art integration project 22Jatin bhatia art integration project 22
Jatin bhatia art integration project 22
 
1 handout.ppt
1 handout.ppt1 handout.ppt
1 handout.ppt
 
Chemical Engineering desciption, laws.ppt
Chemical Engineering desciption, laws.pptChemical Engineering desciption, laws.ppt
Chemical Engineering desciption, laws.ppt
 
First law of thermodynamics
First law of thermodynamicsFirst law of thermodynamics
First law of thermodynamics
 
Chapter 1 - Introduction.pptx
Chapter 1 - Introduction.pptxChapter 1 - Introduction.pptx
Chapter 1 - Introduction.pptx
 
chemical equilibrium and thermodynamics
chemical equilibrium and thermodynamicschemical equilibrium and thermodynamics
chemical equilibrium and thermodynamics
 
Chapter5.pdf
Chapter5.pdfChapter5.pdf
Chapter5.pdf
 

More from mrqueenscience

Biology Text Chapter 6 Lecture Slideshow
Biology Text Chapter 6 Lecture SlideshowBiology Text Chapter 6 Lecture Slideshow
Biology Text Chapter 6 Lecture Slideshowmrqueenscience
 
AP Environmental Science Quick Review Unit 1.pdf
AP Environmental Science Quick Review Unit 1.pdfAP Environmental Science Quick Review Unit 1.pdf
AP Environmental Science Quick Review Unit 1.pdfmrqueenscience
 
Cellular Respiration High School Biology Level
Cellular Respiration High School Biology LevelCellular Respiration High School Biology Level
Cellular Respiration High School Biology Levelmrqueenscience
 
High School Biology Lesson - Photosynthesis.pdf
High School Biology Lesson - Photosynthesis.pdfHigh School Biology Lesson - Photosynthesis.pdf
High School Biology Lesson - Photosynthesis.pdfmrqueenscience
 
Unit 0 Chemistry Review Student Notes.pdf
Unit 0 Chemistry Review Student Notes.pdfUnit 0 Chemistry Review Student Notes.pdf
Unit 0 Chemistry Review Student Notes.pdfmrqueenscience
 
HS Biology - Biotechnology (gen. engineering, cloning, stem cells)
HS Biology - Biotechnology (gen. engineering, cloning, stem cells)HS Biology - Biotechnology (gen. engineering, cloning, stem cells)
HS Biology - Biotechnology (gen. engineering, cloning, stem cells)mrqueenscience
 
Unit 3 Lesson 3- The Marvel of Photosynthesis.
Unit 3 Lesson 3-  The Marvel of Photosynthesis.Unit 3 Lesson 3-  The Marvel of Photosynthesis.
Unit 3 Lesson 3- The Marvel of Photosynthesis.mrqueenscience
 

More from mrqueenscience (7)

Biology Text Chapter 6 Lecture Slideshow
Biology Text Chapter 6 Lecture SlideshowBiology Text Chapter 6 Lecture Slideshow
Biology Text Chapter 6 Lecture Slideshow
 
AP Environmental Science Quick Review Unit 1.pdf
AP Environmental Science Quick Review Unit 1.pdfAP Environmental Science Quick Review Unit 1.pdf
AP Environmental Science Quick Review Unit 1.pdf
 
Cellular Respiration High School Biology Level
Cellular Respiration High School Biology LevelCellular Respiration High School Biology Level
Cellular Respiration High School Biology Level
 
High School Biology Lesson - Photosynthesis.pdf
High School Biology Lesson - Photosynthesis.pdfHigh School Biology Lesson - Photosynthesis.pdf
High School Biology Lesson - Photosynthesis.pdf
 
Unit 0 Chemistry Review Student Notes.pdf
Unit 0 Chemistry Review Student Notes.pdfUnit 0 Chemistry Review Student Notes.pdf
Unit 0 Chemistry Review Student Notes.pdf
 
HS Biology - Biotechnology (gen. engineering, cloning, stem cells)
HS Biology - Biotechnology (gen. engineering, cloning, stem cells)HS Biology - Biotechnology (gen. engineering, cloning, stem cells)
HS Biology - Biotechnology (gen. engineering, cloning, stem cells)
 
Unit 3 Lesson 3- The Marvel of Photosynthesis.
Unit 3 Lesson 3-  The Marvel of Photosynthesis.Unit 3 Lesson 3-  The Marvel of Photosynthesis.
Unit 3 Lesson 3- The Marvel of Photosynthesis.
 

Recently uploaded

GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)Areesha Ahmad
 
Biopesticide (2).pptx .This slides helps to know the different types of biop...
Biopesticide (2).pptx  .This slides helps to know the different types of biop...Biopesticide (2).pptx  .This slides helps to know the different types of biop...
Biopesticide (2).pptx .This slides helps to know the different types of biop...RohitNehra6
 
Labelling Requirements and Label Claims for Dietary Supplements and Recommend...
Labelling Requirements and Label Claims for Dietary Supplements and Recommend...Labelling Requirements and Label Claims for Dietary Supplements and Recommend...
Labelling Requirements and Label Claims for Dietary Supplements and Recommend...Lokesh Kothari
 
GBSN - Microbiology (Unit 2)
GBSN - Microbiology (Unit 2)GBSN - Microbiology (Unit 2)
GBSN - Microbiology (Unit 2)Areesha Ahmad
 
Green chemistry and Sustainable development.pptx
Green chemistry  and Sustainable development.pptxGreen chemistry  and Sustainable development.pptx
Green chemistry and Sustainable development.pptxRajatChauhan518211
 
Hire đź’• 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire đź’• 9907093804 Hooghly Call Girls Service Call Girls AgencyHire đź’• 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire đź’• 9907093804 Hooghly Call Girls Service Call Girls AgencySheetal Arora
 
Botany krishna series 2nd semester Only Mcq type questions
Botany krishna series 2nd semester Only Mcq type questionsBotany krishna series 2nd semester Only Mcq type questions
Botany krishna series 2nd semester Only Mcq type questionsSumit Kumar yadav
 
Presentation Vikram Lander by Vedansh Gupta.pptx
Presentation Vikram Lander by Vedansh Gupta.pptxPresentation Vikram Lander by Vedansh Gupta.pptx
Presentation Vikram Lander by Vedansh Gupta.pptxgindu3009
 
Pests of mustard_Identification_Management_Dr.UPR.pdf
Pests of mustard_Identification_Management_Dr.UPR.pdfPests of mustard_Identification_Management_Dr.UPR.pdf
Pests of mustard_Identification_Management_Dr.UPR.pdfPirithiRaju
 
Pests of cotton_Borer_Pests_Binomics_Dr.UPR.pdf
Pests of cotton_Borer_Pests_Binomics_Dr.UPR.pdfPests of cotton_Borer_Pests_Binomics_Dr.UPR.pdf
Pests of cotton_Borer_Pests_Binomics_Dr.UPR.pdfPirithiRaju
 
Hubble Asteroid Hunter III. Physical properties of newly found asteroids
Hubble Asteroid Hunter III. Physical properties of newly found asteroidsHubble Asteroid Hunter III. Physical properties of newly found asteroids
Hubble Asteroid Hunter III. Physical properties of newly found asteroidsSĂ©rgio Sacani
 
fundamental of entomology all in one topics of entomology
fundamental of entomology all in one topics of entomologyfundamental of entomology all in one topics of entomology
fundamental of entomology all in one topics of entomologyDrAnita Sharma
 
Asymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 b
Asymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 bAsymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 b
Asymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 bSĂ©rgio Sacani
 
Pests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdfPests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdfPirithiRaju
 
Disentangling the origin of chemical differences using GHOST
Disentangling the origin of chemical differences using GHOSTDisentangling the origin of chemical differences using GHOST
Disentangling the origin of chemical differences using GHOSTSĂ©rgio Sacani
 
Physiochemical properties of nanomaterials and its nanotoxicity.pptx
Physiochemical properties of nanomaterials and its nanotoxicity.pptxPhysiochemical properties of nanomaterials and its nanotoxicity.pptx
Physiochemical properties of nanomaterials and its nanotoxicity.pptxAArockiyaNisha
 
Botany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdfBotany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdfSumit Kumar yadav
 
Biological Classification BioHack (3).pdf
Biological Classification BioHack (3).pdfBiological Classification BioHack (3).pdf
Biological Classification BioHack (3).pdfmuntazimhurra
 
Animal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptxAnimal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptxUmerFayaz5
 

Recently uploaded (20)

GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)
 
Biopesticide (2).pptx .This slides helps to know the different types of biop...
Biopesticide (2).pptx  .This slides helps to know the different types of biop...Biopesticide (2).pptx  .This slides helps to know the different types of biop...
Biopesticide (2).pptx .This slides helps to know the different types of biop...
 
Labelling Requirements and Label Claims for Dietary Supplements and Recommend...
Labelling Requirements and Label Claims for Dietary Supplements and Recommend...Labelling Requirements and Label Claims for Dietary Supplements and Recommend...
Labelling Requirements and Label Claims for Dietary Supplements and Recommend...
 
GBSN - Microbiology (Unit 2)
GBSN - Microbiology (Unit 2)GBSN - Microbiology (Unit 2)
GBSN - Microbiology (Unit 2)
 
Green chemistry and Sustainable development.pptx
Green chemistry  and Sustainable development.pptxGreen chemistry  and Sustainable development.pptx
Green chemistry and Sustainable development.pptx
 
Hire đź’• 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire đź’• 9907093804 Hooghly Call Girls Service Call Girls AgencyHire đź’• 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire đź’• 9907093804 Hooghly Call Girls Service Call Girls Agency
 
Botany krishna series 2nd semester Only Mcq type questions
Botany krishna series 2nd semester Only Mcq type questionsBotany krishna series 2nd semester Only Mcq type questions
Botany krishna series 2nd semester Only Mcq type questions
 
Presentation Vikram Lander by Vedansh Gupta.pptx
Presentation Vikram Lander by Vedansh Gupta.pptxPresentation Vikram Lander by Vedansh Gupta.pptx
Presentation Vikram Lander by Vedansh Gupta.pptx
 
Pests of mustard_Identification_Management_Dr.UPR.pdf
Pests of mustard_Identification_Management_Dr.UPR.pdfPests of mustard_Identification_Management_Dr.UPR.pdf
Pests of mustard_Identification_Management_Dr.UPR.pdf
 
The Philosophy of Science
The Philosophy of ScienceThe Philosophy of Science
The Philosophy of Science
 
Pests of cotton_Borer_Pests_Binomics_Dr.UPR.pdf
Pests of cotton_Borer_Pests_Binomics_Dr.UPR.pdfPests of cotton_Borer_Pests_Binomics_Dr.UPR.pdf
Pests of cotton_Borer_Pests_Binomics_Dr.UPR.pdf
 
Hubble Asteroid Hunter III. Physical properties of newly found asteroids
Hubble Asteroid Hunter III. Physical properties of newly found asteroidsHubble Asteroid Hunter III. Physical properties of newly found asteroids
Hubble Asteroid Hunter III. Physical properties of newly found asteroids
 
fundamental of entomology all in one topics of entomology
fundamental of entomology all in one topics of entomologyfundamental of entomology all in one topics of entomology
fundamental of entomology all in one topics of entomology
 
Asymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 b
Asymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 bAsymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 b
Asymmetry in the atmosphere of the ultra-hot Jupiter WASP-76 b
 
Pests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdfPests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdf
 
Disentangling the origin of chemical differences using GHOST
Disentangling the origin of chemical differences using GHOSTDisentangling the origin of chemical differences using GHOST
Disentangling the origin of chemical differences using GHOST
 
Physiochemical properties of nanomaterials and its nanotoxicity.pptx
Physiochemical properties of nanomaterials and its nanotoxicity.pptxPhysiochemical properties of nanomaterials and its nanotoxicity.pptx
Physiochemical properties of nanomaterials and its nanotoxicity.pptx
 
Botany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdfBotany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdf
 
Biological Classification BioHack (3).pdf
Biological Classification BioHack (3).pdfBiological Classification BioHack (3).pdf
Biological Classification BioHack (3).pdf
 
Animal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptxAnimal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptx
 

chapter_19 General Chemistry: Thermodynamics and Equilbrium

  • 2. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–2 – We introduced the thermodynamic property of enthalpy, H, in Chapter 6. – We noted that the change in enthalpy equals the heat of reaction at constant pressure. Thermodynamics • Thermodynamics is the study of the relationship between heat and other forms of energy in a chemical or physical process.
  • 3. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–3 – Heat is energy that moves into or out of a system because of a temperature difference between system and surroundings. – Work, on the other hand, is the energy exchange that results when a force F moves an object through a distance d; work (w) = FĂ—d First Law of Thermodynamics • To state the laws of thermodynamics, we must first understand the internal energy of a system and how you can change it.
  • 4. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–4 – Remembering our sign convention. Work done by the system is negative. Work done on the system is positive. Heat evolved by the system is negative. Heat absorbed by the system is positive. First Law of Thermodynamics • To state the laws of thermodynamics, we must first understand the internal energy of a system and how you can change it.
  • 5. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–5 – In general, the first law of thermodynamics states that the change in internal energy, ΔU, equals heat plus work. First Law of Thermodynamics • To state the laws of thermodynamics, we must first understand the internal energy of a system and how you can change it.
  • 6. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–6 – We do not calculate this, only think of how expanding volume can move something. Heat of Reaction and Internal Energy • When a reaction is run in an open vessel (at constant P), any gases produced represent a potential source of “expansion” work.
  • 7. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–7 – Examples include: A rock at the top of a hill rolls down. Heat flows from a hot object to a cold one. An iron object rusts in moist air. – These processes occur without requiring an outside force and continue until equilibrium is reached. Spontaneous Processes and Entropy • A spontaneous process is a physical or chemical change that occurs by itself.
  • 8. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–8 – Entropy, S , is a thermodynamic quantity that is a measure of the randomness or disorder of a system. – The SI unit of entropy is joules per Kelvin (J/K) and, like enthalpy, is a state function. Entropy and the Second Law of Thermodynamics • The second law of thermodynamics addresses questions about spontaneity in terms of a quantity called entropy.
  • 9. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–9 – When temperature is raised, however, the substance becomes more disordered as it absorbs heat. – The entropy of a substance is determined by measuring how much heat is required to change its temperature per Kelvin degree. Standard Entropies and the Third Law of Thermodynamics • The third law of thermodynamics states that a substance that is perfectly crystalline at 0 K has an entropy of zero.
  • 10. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–10 – Standard state implies 25 o C, 1 atm pressure, and 1 M for dissolved substances. Standard Entropies and the Third Law of Thermodynamics • The standard entropy of a substance or ion (Table 19.1), also called its absolute entropy, So , is the entropy value for the standard state of the species.
  • 11. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–11 – Note that the elements have nonzero values, unlike standard enthalpies of formation, ΔHf o , which by convention, are zero. Standard Entropies and the Third Law of Thermodynamics • The standard entropy of a substance or ion (Table 19.1), also called its absolute entropy, So , is the entropy value for the standard state of the species.
  • 12. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–12 – The symbol So , rather than ΔSo , is used for standard entropies to emphasize that they originate from the third law. Standard Entropies and the Third Law of Thermodynamics • The standard entropy of a substance or ion (Table 19.1), also called its absolute entropy, So , is the entropy value for the standard state of the species.
  • 13. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–13 – Even without knowing the values for the entropies of substances, you can sometimes predict the sign of ΔSo for a reaction. Entropy Change for a Reaction • You can calculate the entropy change for a reaction using a summation law, similar to the way you obtained ΔSo .
  • 14. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–14 1. A reaction in which a molecule is broken into two or more smaller molecules. – The entropy usually increases in the following situations: Entropy Change for a Reaction • You can calculate the entropy change for a reaction using a summation law, similar to the way you obtained ΔSo .
  • 15. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–15 – The entropy usually increases in the following situations: 2. A reaction in which there is an increase in the moles of gases. Entropy Change for a Reaction • You can calculate the entropy change for a reaction using a summation law, similar to the way you obtained ΔSo .
  • 16. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–16 – The entropy usually increases in the following situations: 3. A process in which a solid changes to liquid or gas or a liquid changes to gas. Entropy Change for a Reaction • You can calculate the entropy change for a reaction using a summation law, similar to the way you obtained ΔSo .
  • 17. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–17 – The calculation is similar to that used to obtain ΔHo from standard enthalpies of formation. A Problem To Consider • Calculate the change in entropy, ΔSo , at 25o C for the reaction in which urea is formed from NH3 and CO2 . The standard entropy of NH2 CONH2 is 174 J/(mol.K). See Table 19.1 for other values.
  • 18. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–18 – It is convenient to put the standard entropies (multiplied by their stoichiometric coefficients) below the formulas. So : 2 x 193 214 174 70 A Problem To Consider • Calculate the change in entropy, ΔSo , at 25o C for the reaction in which urea is formed from NH3 and CO2 . The standard entropy of NH2 CONH2 is 174 J/(mol.K). See Table 19.1 for other values.
  • 19. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–19 – We can now use the summation law to calculate the entropy change. A Problem To Consider • Calculate the change in entropy, ΔSo , at 25o C for the reaction in which urea is formed from NH3 and CO2 . The standard entropy of NH2 CONH2 is 174 J/(mol.K). See Table 19.1 for other values.
  • 20. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–20 A Problem To Consider • Calculate the change in entropy, ΔSo , at 25o C for the reaction in which urea is formed from NH3 and CO2 . The standard entropy of NH2 CONH2 is 174 J/(mol.K). See Table 19.1 for other values. – We can now use the summation law to calculate the entropy change.
  • 21. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–21 – This quantity gives a direct criterion for spontaneity of reaction. Free Energy Concept • The American physicist J. Willard Gibbs introduced the concept of free energy (sometimes called the Gibbs free energy), G, which is a thermodynamic quantity defined by the equation G=H-TS.
  • 22. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–22 – Thus, if you can show that ΔG is negative at a given temperature and pressure, you can predict that the reaction will be spontaneous. Free Energy and Spontaneity • Changes in H an S during a reaction result in a change in free energy, ΔG , given by the equation
  • 23. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–23 – The next example illustrates the calculation of the standard free energy change, ΔGo , from ΔHo and ΔSo . Standard Free-Energy Change • The standard free energy change, ΔGo , is the free energy change that occurs when reactants and products are in their standard states.
  • 24. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–24 ΔHo ΔSo ΔGo Description – + – Spontaneous at all T + – + Nonspontaneous at all T – – + or – Spontaneous at low T; Nonspontaneous at high T + + + or – Nonspontaneous at low T; Spontaneous at high T Spontaneity and Temperature Change • All of the four possible choices of signs for ΔHo and ΔSo give different temperature behaviors for ΔGo .
  • 25. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–25 – Place below each formula the values of ΔHf o and So multiplied by stoichiometric coefficients. So : 3 x 130.6 191.5 2 x 193 J/K ΔHf o : 0 0 2 x (-45.9) kJ A Problem To Consider • What is the standard free energy change, ΔGo , for the following reaction at 25o C? Use values of ΔHf o and So , from Tables 6.2 and 19.1.
  • 26. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–26 – You can calculate ΔHo and ΔSo using their respective summation laws. A Problem To Consider • What is the standard free energy change, ΔGo , for the following reaction at 25o C? Use values of ΔHf o and So , from Tables 6.2 and 19.1.
  • 27. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–27 – You can calculate ΔHo and ΔSo using their respective summation laws. A Problem To Consider • What is the standard free energy change, ΔGo , for the following reaction at 25o C? Use values of ΔHf o and So , from Tables 6.2 and 19.1.
  • 28. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–28 – Now substitute into our equation for ΔGo . Note that ΔSo is converted to kJ/K. A Problem To Consider • What is the standard free energy change, ΔGo , for the following reaction at 25o C? Use values of ΔHf o and So , from Tables 6.2 and 19.1.
  • 29. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–29 – By tabulating ΔGf o for substances, as in Table 19.2, you can calculate the ΔGo for a reaction by using a summation law. Standard Free Energies of Formation • The standard free energy of formation, ΔGf o , of a substance is the free energy change that occurs when 1 mol of a substance is formed from its elements in their stablest states at 1 atm pressure and 25o C.
  • 30. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–30 ΔGf o : -174.8 0 2(-394.4) 3(-228.6)kJ – Place below each formula the values of ΔGf o multiplied by stoichiometric coefficients. A Problem To Consider • Calculate ΔGo for the combustion of 1 mol of ethanol, C2 H5 OH, at 25o C. Use the standard free energies of formation given in Table 19.2.
  • 31. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–31 ΔGf o : -174.8 0 2(-394.4) 3(-228.6)kJ – You can calculate ΔGo using the summation law. A Problem To Consider • Calculate ΔGo for the combustion of 1 mol of ethanol, C2 H5 OH, at 25o C. Use the standard free energies of formation given in Table 19.2.
  • 32. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–32 – You can calculate ΔGo using the summation law. A Problem To Consider ΔGf o : -174.8 0 2(-394.4) 3(-228.6)kJ ΔGf o : -174.8 0 2(-394.4) 3(-228.6)kJ • Calculate ΔGo for the combustion of 1 mol of ethanol, C2 H5 OH, at 25o C. Use the standard free energies of formation given in Table 19.2.
  • 33. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–33 1. When ΔGo is a large negative number (more negative than about –10 kJ), the reaction is spontaneous as written, and the reactants transform almost entirely to products when equilibrium is reached. ΔGo as a Criteria for Spontaneity • The following rules are useful in judging the spontaneity of a reaction.
  • 34. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–34 2. When ΔGo is a large positive number (more positive than about +10 kJ), the reaction is nonspontaneous as written, and reactants do not give significant amounts of product at equilibrium. • The following rules are useful in judging the spontaneity of a reaction. ΔGo as a Criteria for Spontaneity
  • 35. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–35 3. When ΔGo is a small negative or positive value (less than about 10 kJ), the reaction gives an equilibrium mixture with significant amounts of both reactants and products. • The following rules are useful in judging the spontaneity of a reaction. ΔGo as a Criteria for Spontaneity
  • 36. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–36 – Figure 19.9 illustrates the change in free energy during a spontaneous reaction. – As the reaction proceeds, the free energy eventually reaches its minimum value. – At that point, ΔG = 0, and the net reaction stops; it comes to equilibrium. Free Energy Change During Reaction • As a system approaches equilibrium, the instantaneous change in free energy approaches zero.
  • 37. Figure 19.9 Free-energy change during a spontaneous reaction.
  • 38. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–38 – Here Q is the thermodynamic form of the reaction quotient. Relating ΔGo to the Equilibrium Constant • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, ΔGo , by the following equation.
  • 39. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–39 – ΔG represents an instantaneous change in free energy at some point in the reaction approaching equilibrium. • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, ΔGo , by the following equation. Relating ΔGo to the Equilibrium Constant
  • 40. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–40 – At equilibrium, ΔG=0 and the reaction quotient Q becomes the equilibrium constant K. • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, ΔGo , by the following equation. Relating ΔGo to the Equilibrium Constant
  • 41. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–41 – At equilibrium, ΔG=0 and the reaction quotient Q becomes the equilibrium constant K. • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, ΔGo , by the following equation. Relating ΔGo to the Equilibrium Constant
  • 42. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–42 – When K > 1 , the ln K is positive and ΔGo is negative. – When K < 1 , the ln K is negative and ΔGo is positive. • This result easily rearranges to give the basic equation relating the standard free-energy change to the equilibrium constant. Relating ΔGo to the Equilibrium Constant
  • 43. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–43 – Rearrange the equation ΔGo =-RTlnK to give A Problem To Consider • Find the value for the equilibrium constant, K, at 25o C (298 K) for the following reaction. The standard free-energy change, ΔGo , at 25o C equals –13.6 kJ.
  • 44. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–44 – Substituting numerical values into the equation, A Problem To Consider • Find the value for the equilibrium constant, K, at 25o C (298 K) for the following reaction. The standard free-energy change, ΔGo , at 25o C equals –13.6 kJ.
  • 45. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–45 – Hence, A Problem To Consider • Find the value for the equilibrium constant, K, at 25o C (298 K) for the following reaction. The standard free-energy change, ΔGo , at 25o C equals –13.6 kJ.
  • 46. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–46 ΔHo ΔSo ΔGo Description – + – Spontaneous at all T + – + Nonspontaneous at all T – – + or – Spontaneous at low T; Nonspontaneous at high T + + + or – Nonspontaneous at low T; Spontaneous at high T Spontaneity and Temperature Change • All of the four possible choices of signs for ΔHo and ΔSo give different temperature behaviors for ΔGo .
  • 47. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–47 – You get the value of ΔGT o at any temperature T by substituting values of ΔHo and ΔSo at 25 o C into the following equation. Calculation of ΔGo at Various Temperatures • In this method you assume that ΔHo and ΔSo are essentially constant with respect to temperature.
  • 48. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–48 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ – Place below each formula the values of ΔHf o and So multiplied by stoichiometric coefficients. A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity.
  • 49. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–49 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ – You can calculate ΔHo and ΔSo using their respective summation laws. A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity.
  • 50. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–50 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity.
  • 51. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–51 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity.
  • 52. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–52 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity. – Now you substitute ΔHo , ΔSo (=0.1590 kJ/K), and T (=298K) into the equation for ΔGf o .
  • 53. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–53 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity. – Now you substitute ΔHo , ΔSo (=0.1590 kJ/K), and T (=298K) into the equation for ΔGf o .
  • 54. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–54 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity. – Now you substitute ΔHo , ΔSo (=0.1590 kJ/K), and T (=298K) into the equation for ΔGf o . So the reaction is nonspontaneous at 25o C.
  • 55. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–55 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity. – Now we’ll use 1000o C (1273 K) along with our previous values for ΔHo and ΔSo .
  • 56. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–56 So : 38.2 92.9 213.7 J/K ΔHf o : -635.1 -1206.9 -393.5 kJ A Problem To Consider • Find the ΔGo for the following reaction at 25o C and 1000o C. Relate this to reaction spontaneity. – Now we’ll use 1000o C (1273 K) along with our previous values for ΔHo and ΔSo . So the reaction is spontaneous at 1000o C.
  • 57. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–57 Operational Skills • Calculating the entropy change for a phase transition • Predicting the sign of the entropy change of a reaction • Calculating ΔSo for a reaction • Calculating ΔGo from ΔHo and ΔSo • Calculating ΔGo from standard free energies of formation • Interpreting the sign of ΔGo • Writing the expression for a thermodynamic equilibrium constant • Calculating K from the standard free energy change • Calculating ΔGo and K at various temperatures