thermodynamics chapter 20. thermodynamics prediction of whether change will occur no indication of...
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Thermodynamics
Chapter 20Chapter 20
Thermodynamics
Prediction of whether change will occurPrediction of whether change will occur
No indication of timeframeNo indication of timeframe
Spontaneous:Spontaneous:
occurs without external interventionoccurs without external intervention
Nonspontaneous:Nonspontaneous:
requires outside “push”requires outside “push”
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En
erg
y
Reaction progress
Reactants
Products
Domain of kinetics(the reaction pathway)
Domain ofthermodynamics
(the initial andfinal states)
Entropy and Spontaneity
Driving force for a spontaneous change is anDriving force for a spontaneous change is an
increase in entropy of the universeincrease in entropy of the universe
Entropy, SEntropy, S:: measure of disordermeasure of disorder
Spontaneous change implies:Spontaneous change implies:
more order more order less order less order
fewer ways of arranging particles fewer ways of arranging particles more more
Second Law of Thermodynamics
In any spontaneous change, there is always an In any spontaneous change, there is always an increase in entropy of the universe.increase in entropy of the universe.
Units:Units: J J
KK
0ΔS ΔS ΔS surrsysuniv
Entropy
1877 Ludwig Boltzmann:1877 Ludwig Boltzmann:
k = Boltzmann constant, R/Nk = Boltzmann constant, R/NAA
W = W = no. of possible arrangementsno. of possible arrangements
Third Law of Thermodynamics:Third Law of Thermodynamics:
The entropy of a perfect crystal at 0 K is zero.The entropy of a perfect crystal at 0 K is zero.
W lnk S
Positional EntropyWhy does a gas expand into a vacuum?Why does a gas expand into a vacuum?
Expanded state has highest positional probability Expanded state has highest positional probability of states available.of states available.
solutiongasor liquid, solid, pure
gasliquidsolid
S S
S S S
Other factors in entropy
Size:Size:
increase in S with increasing size (mass)increase in S with increasing size (mass)
Molecular complexity:Molecular complexity:
increase in S with increasing complexityincrease in S with increasing complexity
Generally effect of physical state >> complexityGenerally effect of physical state >> complexity
Reactions
For a spontaneous reaction:For a spontaneous reaction:
NaOHNaOH(s)(s) + CO + CO2(g)2(g) Na Na22COCO3(s)3(s) + H + H22OO(l)(l)
SS00 64.45 213.7 139 69.94 64.45 213.7 139 69.94 J/KJ/K
Is the reaction spontaneous as written?Is the reaction spontaneous as written?
0Sn Sn ΔS 0rr
0pp
0rxn
Spontaneity and S
Spontaneous:Spontaneous: SSunivuniv > 0 > 0
Nonspontaneous:Nonspontaneous: SSunivuniv < 0 < 0
At equilibrium:At equilibrium: SSunivuniv = 0 = 0
SSsyssys can be positive if can be positive if SSsurrsurr increases enough increases enough
surrsysuniv ΔS ΔS ΔS
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Table 16.3 Interplay of Ssys and Ssurr in Determining the Sign of Suniv
Signs of Entropy Changes
Process Spontaneous?
Yes
No (reaction will occur in opposite direction)
Yes, if Ssys has a larger magnitude than Ssurr
Yes, if Ssurr has a larger magnitude than Ssys
Ssys Ssurr Suniv
Surroundings and Suniv
Surroundings add or remove heatSurroundings add or remove heat
Exothermic:Exothermic:
qqsyssys < 0 < 0
qqsurrsurr > 0 > 0 so so SSsurrsurr > 0 > 0
Endothermic:Endothermic:
qqsyssys > 0 > 0
qqsurrsurr < 0 < 0 so so SSsurrsurr < 0 < 0
Ssurr and Ssys
SSsurrsurr:: SSsurrsurr - - qqsyssys
SSsurrsurr 1/T 1/T
At constant pressure:At constant pressure:
T
qΔS sys
surr
T
HΔS sys
surr
The Math
Given:Given:
@constant P:@constant P:
Multiply by Multiply by T:T:
Result:Result: syssyssys
syssysuniv
syssysuniv
surrsysuniv
TΔΔH ΔG
TΔΔH TΔT
ΔH ΔS ΔS
ΔS ΔS ΔS
S
SS
0ΔS implies 0 ΔG univ
Reactions and G
GG00:: Standard Free EnergyStandard Free Energy
Reactants in standard states areReactants in standard states are
converted to products in standard converted to products in standard statesstates
0rr
0pp
0rxn ΔGn ΔGn ΔG
Gibb’s Free Energy
Overall criterion for spontaneityOverall criterion for spontaneity
from the standpoint of the systemfrom the standpoint of the system
A process at constant temp. and pressure is A process at constant temp. and pressure is spontaneous in the direction spontaneous in the direction G decreasesG decreases
ST -H ΔG
G = H - TS
HH SS GG Spontaneous?Spontaneous?
““Good”: Good”: H < 0H < 0 ““Good”: Good”: S > 0S > 0 ““Good”: Good”: G < 0G < 0 ““Good”: Good”: G < 0G < 0
-- ++ -- At all At all temperaturestemperatures
-- -- ?? At low At low temperaturestemperatures
++ ++ ?? At high At high temperaturestemperatures
++ -- ++ Not at any Not at any temperaturetemperature
Summary
G < 0G < 0 Spontaneous as writtenSpontaneous as written
G > 0G > 0 Not spontaneous as writtenNot spontaneous as written
Reverse process spontaneousReverse process spontaneous
G = 0G = 0 At equilibriumAt equilibrium
A Closer Look…
TTS:S:
energy not avail. for doing workenergy not avail. for doing work
G:G:
E avail. as heat E avail. as heat –– E not avail. for work E not avail. for work
max. work available (constant T and P)max. work available (constant T and P)
Amount of work actually obtained depends on pathAmount of work actually obtained depends on path
ST -H ΔG
G and Work
GG
SpontaneousSpontaneous max. work obtainablemax. work obtainable
NonspontaneousNonspontaneousmin. work requiredmin. work required
Work and path-dependenceWork and path-dependence
wwmaxmax ( (wwminmin)) process performed reversiblyprocess performed reversibly
theoreticaltheoretical
wwactual actual < < wwmaxmax performed irreversiblyperformed irreversibly
real worldreal world
Reversible vs. Irreversible Processes
Reversible:Reversible:
The universe is exactly the same as it was before The universe is exactly the same as it was before the cyclic process.the cyclic process.
Irreversible:Irreversible:
The universe is different after the cyclic process.The universe is different after the cyclic process.
All real processes are irreversible.All real processes are irreversible.
Some work is changed to heat.Some work is changed to heat.
Free Energy and Pressure
Q:Q: reaction quotient from mass action lawreaction quotient from mass action law
RTlnQ GΔG 0
Free Energy and Equilibrium
K:K: equilibrium constantequilibrium constant
At At
equilibrium:equilibrium: G = 0G = 0
K = QK = Q
RTlnKΔG0
RTGΔ
e0
K
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0Fraction of A reacted
0.5 1.0
G
Equilibriumoccurs here
0Fraction of A reacted
0.5 1.0
G
Equilibriumoccurs here
0Fraction of A reacted
0.5 1.0
Equilibriumoccurs here
(a) (b) (c)
G
A B
G and Extent of Reaction
A B
G0B < G0
A
Spontaneous
C D
G0D> G0
C
Nonspontaneous
Temperature Dependence of K
Plot lnK vs. 1/TPlot lnK vs. 1/Tslope = -slope = -HH00/R/R intercept = intercept = SS00/R /R
*assumes *assumes HH00, , SS00 relatively T independent relatively T independent
000 ST - H RTlnK ΔG
bmxy
R
S
T
1
R
H lnK
RT
ΔG
000