Temperature and Spontaneity

Fig. 19.3 pg. 805

Spontaneous Processes


Gas Molecules Confined

http://www.chem.lsu.edu/htdocs/people/jchogan/CHEM_1202/Images/Entropy01.jpg

Entropy


Gas Molecules Liberated

http://www.chem.lsu.edu/htdocs/people/jchogan/CHEM_1202/Images/Entropy02.jpg

Entropy

When the stopcock is opened the gas will spread out into both flasks and its entropy will increase because intermolecular forces will be diminished as gas molecules spread apart from one another; gas will become less structured (more chaotic, more spread out) and thus gain entropy.


Importance of Disorder

Fig. 19.1 pg. 804

Entropy and the Second Law of Thermodynamics


Structure of Ice

Fig. 19.9 pg. 815

Entropy and the Second Law of Thermodynamics

Entropy


Frozen and Unmixed Substances

http://www.chem.lsu.edu/htdocs/people/jchogan/CHEM_1202/Images/Entropy.jpg

Melting, Vaporization, and Mixing


Melting, Vaporization, and Mixing

http://www.chem.lsu.edu/htdocs/people/jchogan/CHEM_1202/Images/Entropy.gif

Entropy and Mixing


Dissolution of an Ionic Substance

Fig. 19.10 pg.816

Entropy and the Second Law of Thermodynamics

Entropy


Dissolution of NaCl

http://hogan.chem.lsu.edu/matter/chap26/animate1/an26_004.mov

Dissolution of NaCl


Gas Molecules and Entropy

Adapted from Fig. 19.11 pg. 816

A Molecular Interpretation of Entropy


Entropy Changes Upon Heating

Fig. 19.14 pg. 819

A Molecular Interpretation of Entropy


Standard Molar Entropies

Table 19.2 pg. 820

Calculation of Entropy Changes


Gibbs Free Energy I

Text slide.

Gibbs Free Energy

DG = DH - TDS

Gibbs Free Energy II

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Gibbs Free Energy


Gibbs Free Energy III

Text slide.

Gibbs Free Energy

What contributes to instability gain/loss (DG)?

  1. Enthalpy (H). Loss of heat (negative DH) from system contributes favorably to process. Negative DH means heat balance in system is negative because system has dumped heat into the surroundings. This causes entropy of surroundings to increase.
  2. System entropy (DS). Gain of entropy (positive DS) in system contributes favorably to a process. To put system entropy change (DS) into same units as the DH which causes surroundings entropy change (comparison purposes) we multiply DS by T (ie. TDS).

Temperature and Spontaneity

Table 19.4 pg. 828

Free Energy and Temperature


Gibbs Free Energy IV

Text slide.

Gibbs Free Energy


Gibbs Free Energy V

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Gibbs Free Energy


Gibbs Free Energy VI

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Gibbs Free Energy


Gibbs Free Energy VII

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Gibbs Free Energy


DG and Temperature

Text slide.

DG and Temperature

DGoT ~ DHo298 - TDSo298

Often works at temperatures other than T = 298 K, because DH and DS are often fairly temperature-independent.

One consequence of this is it is possible to calculate temperature at which a process is at balance point between being spontaneous and nonspontaneous by assuming:

DGoT ~ DHo298 - TDSo298 = 0, or:

DHo298 ~ TDSo298 (ie. T ~ DHo298/DSo298)


Free Energy Changes

Fig. 19.17 pg. 823

Gibbs Free Energy

G = H - TS

DG = DH - T DS

DG and Concentration

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DG and Concentration

DG = DGo + RT ln Q

DG and Equilibrium Constant

Text slide.

DG and Equilibrium Constant

At equilibrium product and reactant are equally unstable (each falls apart to make the other at equal speed), so at equilibrium:

DG = DGo + RT ln Q = 0, or:

DGo = -RT ln Qeq

Since Qeq = K (equilibrium constant):

DGo = -RT ln K;

K = e-DG/(RT)


Driving Nonspontaneous Reactions

Fig. 19.19 pg. 833

Gibbs Free Energy

Driving Nonspontaneous Reactions

C6H12O6(s) + 6O2 6CO2 + 6H2O(l); DGo = -2880 kJ/equiv