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Title: Spontaneity, Entropy and Free energy


1
Chapter 16
  • Spontaneity, Entropy and Free energy

2
Contents
  • Spontaneous Process and Entropy
  • Entropy and the second law of thermodynamics
  • The effect of temperature on spontaneity
  • Free energy
  • Entropy changes in chemical reactions The Third
    Law of Thermodynamics
  • Free energy and chemical reactions
  • The dependence of free energy on pressure
  • Free energy and equilibrium
  • Free energy and work

3
16.1 Spontaneous Process and Entropy
  • A process that will occur without outside
    intervention.
  • Thermodynamics cant determine how fast the
    process is (may be fast or slow).
  • Kinetics tell us that the rate of reaction
    depends on activation energy temperature,
    concentration and catalysts i.e, it depends on
    the pathway of process.
  • Thermodynamics compares initial and final states
    and does not require knowledge of the pathway.
  • Kinetics describes pathway between reactants and
    products.
  • We need both thermodynamics and kinetics to
    describe a reaction completely.

4
Spontaneity
  • process that will occur without outside
  • intervention.
  • Rolling a ball down a hill (gravity) steel
    rusting (?) wood burning (exothermic process)
    transfer of heat from hot to cold (exothermic)
    freezing of water (exothermic) Melting of ice
    (endothermic!!) etc.
  • What common characteristic derives all those
    processes to be spontaneous?
  • It is an increase in a property called Entropy,
    S.
  • Thus all spontaneous processes occur as a result
    of an increase of the S of the universe.

5
What is Entropy?
  • Entropy, S, is measure of randomness, or
    disorder in the system. For example molecular
    randomness.
  • Naturally, things move from order to disorder!
    (from lower S to higher S.)

6
Entropy
  • S defined in terms of probability.
  • Substances take the most likely arrangement (that
    have more probabilities).
  • The most likely arrangement is the most random.
  • Can we calculate the number of arrangements for a
    system?

7
Entropy and Gases
  • Gas placed in one bulb of a container will
    spontaneously expand to fill the entire vessel
    (vessel of two bulbs) evenly.
  • Probabilities of finding equal number of
    molecules in each bulb are huge.
  • Finding molecules in one bulb is highly
    improbable thus the process does not occur
    spontaneously.

8
Entropy and state of matter
  • Gases completely fill their chamber because there
    are many more ways to do that than to leave half
    empty.
  • Ssolid ltSliquid ltltSgas
  • In solids, molecules are very close and thus they
    have relatively few positions available to them
  • Entropy also describes the number of possible
    positions of a molecule
  • There are many more ways for the molecules to be
    arranged as a liquid than a solid.
  • Gases have a huge number of positions possible.

9
Example
  • Which has higher positional S?
  • Solid CO2 or gaseous CO2?
  • N2 gas at 1 atm or N2 gas at 0.01 atm?
  • Predict the sign of DS
  • Solid sugar is added to water
  • because larger volume
  • Iodine vapor condenses on cold surface to form
    crystals
  • - because g?s, less volume

10
Positional Entropy
  • Entropy also describes the number of
  • possible positions of a molecule
  • A gas expands into a vacuum because
  • the expanded state has the highest
  • positional probability of states available
  • to the system i.e., the highest positional
  • entropy
  • Probability depends on the number of
  • configurations in space ( positional
  • microstates)

11
16.2 Entropy and the second law of thermodynamics
  • Solutions form because there are many more
  • possible arrangements of dissolved pieces than
    if
  • they stay separate there is an increase in
    entropy
  • Generally, in any spontaneous process, there is
  • always an increase in the entropy of the
    universe
  • This is the second law of thermodynamics
  • DSuniv DSsys DSsurr
  • If DSuniv is positive the process is
    spontaneous.
  • If DSuniv is negative the process is spontaneous
    in
  • the opposite direction.
  • ?Suniv gt 0 for any spontaneous process
  • First law The energy of a universe is constant

12
16.3 The effect of temperature on spontaneity
  • For exothermic processes DSsurr is positive
  • For endothermic processes DSsurr is negative
  • Consider this process (endothermic)
  • H2O(l) H2O(g)
  • DSsys is positive (change from L to G)
  • DSsurr is negative (random motion of atoms in the
    surrounding decreases)
  • Which one will control the process DSsys or
    DSsurr?
  • DSuniv
  • If the ?Ssys and ?Ssurr have different signs, the
    temperature determines the ?Suniv

13
Determining ?Ssurr
  • Sign of ?Ssurr
  • depends on direction of heat flow
  • ?Ssurr for exothermic reactions
  • ?Ssurr - for endothermic reactions
  • Magnitude of ?Ssurr
  • Depends on temperature
  • Heat flow ?H at constant P
  • Very small at high T, increases as T decreases

14
Entropy of DSys and DSsurr in determining the
sign of DSuniv
DSsurr
DSuniv
Spontaneous?
DSsys
-
-
-
No



Yes

-
?
Yes at High temp.
DSsurr -DH/T
Yes at Low temp.
15
Example
  • A process has a DH of 22 kJ and a DS of -13 J/K.
    At which temperatures is the process spontaneous?
  • if there is no subscript, DS DSsys
  • DSuniv gt 0 to be spontaneous
  • DSsys DSsurr gt 0

16
Example
  • For methanol, the enthalpy of vaporization is
    71.8 kJ/mol and the entropy of vaporization is
    213 J/K. What is the normal boiling point of
    methanol?
  • DSsys 213 J/K and DH 71.8 kJ/molK 71,800
    J/molK
  • at the boiling point, the vaporization begins to
    be spontaneous
  • DSuniv 0 to be at bp ? DSsys DSsurr 0

17
16.4 Free Energy, G
  • G Gibbs free energy
  • G helps the determination of the T dependence
    on spontaneity
  • G H - TS definition of G
  • ?G ? H - T ? S for constant T
  • All quantities refer to the system.
  • When no subscript the quantity refers to the
    system

18
at constant T and P
  • If DG is negative at constant T and P, the
    process is spontaneous.
  • The process is spontaneous in the direction DG
    decreases
  • - DG means DSuniv
  • So what sign would the ?G of reaction with a
    ?Suniv have?
  • Negative

19
Example
  • Is the following reaction spontaneous at -10C
    in
  • the forward direction?
  • H2O(s) ? H2O(l)
  • where ?H6.03x103 J/mol and ?S22.1 J/mol.K

?Go ? Ho - T ? So
20
  • Another way to check for spontaneity of a
    reaction?
  • Check to see if the ?Suniv is positive
  • How can we solve for ?Ssurr?
  • use ?H and T
  • At -10C, is it spontaneous?

NO!- the reverse is spontaneous
21
Example 2
  • At what T is this reaction
  • spontaneous at 1 atm
  • Of pressure?
  • Br2(l) ? Br2(g)
  • ?Ho31.0 kJ/mol,
  • ?So93.0 J/molK

22
DGDH-TDS
-

At all Temperatures


Spontaneous at high temperatures
-
Spontaneous at low temperatures
-

-
Not spontaneous at any temperature, Reverse is
spontaneous
23
16.5 Entropy changes in chemical reactionsThe
Third Law of Thermodynamics
  • So far we dealt with physical changes
  • In a chemical reaction, when the number of
  • gaseous molecules increases, the positional
  • disorder will increase and consequently ?S
    would
  • be Positive and Visa Versa
  • Consider the following examples
  • N2(g) 3H2(g) 2NH3(g)
  • 4NH3(g) 5O2 (g) 4NO(g)
    6H2O(g)
  • CaCO3(s) CaO
    (s) CO2(g)

24
  • The changes in enthalpy determines the
    exothermicity and endothermicity at constant P
  • The changes in entropy determines the
  • spontaneity at constant P and T
  • Are there values given for S?
  • The entropy of a pure crystal at 0 K is 0.
  • Molecular motion is almost zero and only one
    arrangement is possible.
  • Thus, the entropy of a perfect crystal is zero
    this statement is called the Third Law of
    Thermodynamics

25
  • At T gt0, some changes in order will occur,
    consequently, S gt0
  • This value gives us a starting point.
  • Standard Entropies Sº ( at 298 K and 1 atm) of
    substances are listed.
  • DSº can then be determined for products and
    reactants
  • ?S?reaction ?np?S?(products) ?
    ?nr?S?(reactants)
  • Entropy is a state function of the system (It is
    not pathway dependent)

26
  • Entropy is an extensive property. It depends on
    the amount of substance present
  • Number of moles of reactants and products must be
    taken into account
  • What is the expected ?S (0, 0r ve or
  • ve) for the following reaction?
  • Al2O3(s) 3H2(g) 2Al(s)
    3H2O(g)
  • More complex molecules possess higher Sº

27
Example
  • Find the ?S at 25C for
  • 2NiS(s) 3O2(g) ? 2SO2(g) 2NiO(s)
  • 53 205 248 38

28
16.6 Free Energy and Chemical Reactions
  • DGº is needed when dealing with chemical
    reactions
  • DGº standard free energy change.
  • Free energy change that will occur if reactants
    in their standard state turn to products in their
    standard state.
  • N2(g) 3H2(g) 2NH3(g) DGº
    -33.3 kJ
  • DGº cant be measured directly, but can be
    calculated from other measurements.
  • DGºDHº-TDSº

29
Free Energy in Reactions
  • There are tables of DGºf .
  • The standard free energy of formation for any
    element in its standard state is 0.
  • Why DGº is useful?
  • To compare relative tendencies of reactions to
    occur.
  • The more ve the value of DGº, the further a
    reaction will go to the right to reach equilibrium

30
How do we calculate DGº?There are three Ways to
Calculate ?G
  • Use equation ?G ? H - T ? S
  • Use Hesss Law
  • Rearrange equations to get the given equation
  • Add ?G values for the equations
  • Use ?Gf standard free energy of formation

31
  • 1. Use the equation
  • DGºDHº-TDSº
  • This equation is applicable for reactions taking
    place at constant temperature

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2. Claculation of DGº using Hesss law
  • Free energy is a state function just like
    enethalpy, i.e., it depends upon the pathway of
    the reaction
  • It can be found same as DH using Hesss law

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3. Calculation of DGº using the standard free
energies of formation DGºf
  • DGºf of a substance is
  • the change in free energy that accompanies the
    formation of 1 mole of that substance from its
    constituent elements with all reactants and
    products in their standard states
  • DGº for a specific reaction is obtained from the
    equation
  • ?G? ?np?Gf?(products) ??nr?Gf?(reactants)

38
  • There are tables of DGºf .
  • The standard free energy of formation for any
    element in its standard state is 0.
  • Remember also that the number of moles of each
    reactant and product must be used in calculating
    DGº for a reaction

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Exercise
  • Is the following reaction spontaneous under the
    standard conditions?
  • C2H4(g) H2O(l) C2H5OH(l)
  • Find DGº for the reaction using DGºf values from
    the table
  • If DGº is Ve, the process is spontaneous and the
    formation of ethanol is favorable
  • Of course to judge whether the reaction is
    feasible or not, we have to study its kinetics to
    know whether the reaction is fast or slow.
  • If it is slow adding a catalyst may be considered
  • Also, remember that DGº depends on temperature
    DGoDHo-TDSo

41
16.7 The Dependence of Free Energy on Pressure
  • At a large volume the gas has many more positions
    available for its molecules than at low volumes
  • S large V gt S small V
  • S low P gt S high P
  • Since S depends on P then G will depend on P. It
    can be shown that
  • G Go RTln(P)
  • (Go free energy at 1 atm)

42
  • By proper derivation we got
  • DG DGº RTln(Q)
  • where Q is the reaction quotient (P of the
    products /P of the reactants).

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16.8 Free energy and equilibrium
  • According to thermodynamics the equilibrium
    occurs at the lowest value of free energy
    available
  • At equilibrium DG 0, Q K
  • DG DGº RT ln(Q)
  • Thus, DGº -RT lnK

46
DGº K
  • DGº -RT lnK
  • 0 1
  • lt0 gt0
  • gt0 lt0

47
Temperature dependence of K
  • DGº -RT lnK DHº - TDSº
  • ln(K) - DHº/RT DSº/R
  • Plot ln(K) VS 1/T
  • A straight line gives a
  • Slope DHº/R
  • Intercept DSº/R

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Example
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16.9 Free energy and Work
  • Free energy is that energy free to do work.
  • The maximum amount of work possible at a given
    temperature and pressure.
  • Never really achieved because some of the free
    energy is changed to heat during a change, so it
    cant be used to do work.

54
Reversible v. Irreversible Processes
  • Reversible The universe is exactly the same as
    it was before the cyclic process.
  • Irreversible The universe is different after
    the cyclic process.
  • All real processes are irreversible -- (some work
    is changed to heat)
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