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Lecture 8 Summary Δsys ΔS° surr ΔS° univ ΔΗ° sys < 0 ΔS° sys ΔS° surr ΔS° univ ΔΗ° sys < 0 ΔS° sys ΔS° surr ΔS° univ ΔΗ° sys> 0 Spontaneous, exothermic Spontaneous, exothermic Spontaneous, endothermic
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Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Dec 21, 2015

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Page 1: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Lecture 8 Summary

ΔS°sys ΔS°surrΔS°univ

ΔΗ°sys < 0

ΔS°sys

ΔS°surrΔS°univ

ΔΗ°sys < 0

ΔS°sys

ΔS°surr

ΔS°univ

ΔΗ°sys > 0

Spontaneous, exothermic

Spontaneous, exothermic

Spontaneous, endothermic

Page 2: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Lecture 9: Gibbs Free Energy G

Reading: Zumdahl 10.7, 10.9

OutlineDefining the Gibbs Free Energy (ΔG)

Calculating ΔG (several ways to)Pictorial Representation of ΔG

Page 3: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Defining ΔGRecall, the second law of thermodynamics: ΔSuniv = ΔStotal = ΔSsys + ΔSsurr

Also recall:

ΔSsurr = -ΔHsys/T

SubstitutingΔStotal = ΔSsys+

ΔSsurr

-ΔHsys/T

ΔStotal = -TΔSsys+ ΔHsys

Multipling all by (-T) gives

Page 4: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

We then define:

ΔG = -TΔStotal

Substituting

ΔG = ΔH - TΔS

ΔG = -TΔSsys+

ΔHsys

ΔG = The Gibbs Free Energy @const P

Giving finally

Page 5: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

ΔG and Spontaneous Processes

Recall from the second law the conditions of spontaneity:

Three possibilities:IfΔSuniv > 0…..process is spontaneous

If ΔSuniv < 0…..process is spontaneous in opposite direction.

If ΔSuniv = 0….equilibrium

In our derivation of ΔG, we divided by -T; therefore, the direction of the inequality relative to entropy is now reversed.

Page 6: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Three possibilities in terms of ΔS:IfΔSuniv > 0…..process is spontaneous.

If ΔSuniv < 0…..process is spontaneous in opposite

direction.If ΔSuniv = 0…. system is in equilibrium.

Three possibilities in terms of ΔG:IfΔG < 0…..process is spontaneous.If ΔG > 0…..process is spontaneous in opposite

direction.If ΔG = 0….system is in equilibrium

Page 7: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Spontaneous Processes: temperature dependence

Note that ΔG is composed of both ΔH and ΔS termsΔG = ΔH - TΔS

IfΔH < 0 and ΔS > 0….spontaneous at all T

A reaction is spontaneous if ΔG < 0. So,

IfΔH > 0 and ΔS < 0….not spontaneous at any T

IfΔH < 0 and ΔS < 0…. becomes spontaneous at low T

IfΔH > 0 and ΔS > 0….becomes spontaneous at high T

Page 8: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Example: At what T is the following reaction spontaneous?

Br2(l) Br2(g)

where ΔH° = 30.91 kJ/mol, ΔS° = 93.2 J/mol.K

ΔG° = ΔH° - TΔS°

Page 9: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Try 298 K just to see result at standard conditionsΔG° = ΔH° - TΔS°

ΔG° = kJ/mol - (298K)J/mol.K

ΔG° = kJ/mol = 3.13 kJ/mol> 0

Not spontaneous at 298 K

Page 10: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

At what T then does the process become spontaneous?ΔG° = ΔH° - TΔS°

ΔΔS

= (kJ/mol)J/mol.K

= 0

Just like our previous calculation

= 331.65 K

Page 11: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Calculating ΔG°

In our previous example, we needed to determine

ΔH°rxn and ΔS°rxn separately to determine ΔG°rxn

But ∆ G is a state function; therefore, we can use known ΔG° to determine ΔG°rxn using:

ΔG°rxn = ΔG°prod . −∑ ΔG°react .∑

Page 12: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Standard ΔG of Formation: ΔGf°

Like ΔHf° and S°, the standard Gibbs free energy of formation ΔGf° is defined as the “change in free energy that accompanies the formation of 1 mole of that substance for its constituent elements with all reactants and products in their standard state.”

As for ΔHf° , ΔGf° = 0 for an element in its standard state:

Example: ΔGf° (O2(g)) = 0

Page 13: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Example

• Determine the ΔG°rxn for the following:

C2H4(g) + H2O(l) C2H5OH(l)

• Tabulated ΔG°f from Appendix 4:

ΔG°f(C2H5OH(l)) = -175 kJ/mol

ΔG°f(C2H4(g)) = 68 kJ/mol

ΔG°f(H2O (l)) = -237 kJ/mol

Page 14: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

• Using these values:

C2H4(g) + H2O(l) C2H5OH(l)

ΔG°rxnΔG°f(C2H5OH(l)) - ΔG°f(C2H4(g)) ΔG°f(H2O (l))

ΔG°rxn = ΔG°prod . −∑ ΔG°react .∑

ΔG°rxn-175 kJ - 68 kJ -(-237 kJ)

ΔG°rxn-6 kJ< 0 ; therefore, spontaneous

Page 15: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

More ΔG° Calculations

• Similar to ΔH°, one can use the ΔG° for various reactions to determine ΔG° for the reaction of interest (a “Hess’ Law” for ΔG°)

• Example:

C(s, diamond) + O2(g) CO2(g) ΔG° = -397 kJ

C(s, graphite) + O2(g) CO2(g) ΔG° = -394 kJ

Page 16: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

C(s, diamond) + O2(g) CO2(g) ΔG° = -397 kJ

C(s, graphite) + O2(g) CO2(g) ΔG° = -394 kJ

CO2(g) C(s, graphite) + O2(g) ΔG° = +394 kJ

C(s, diamond) C(s, graphite) ΔG° = -3 kJ

ΔG°rxn < 0…..rxn is spontaneous

Page 17: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

ΔG°rxn ≠ Reaction Rate• Although ΔG°rxn can be used to predict if a reaction will be spontaneous as written, it does not tell us how fast a reaction will proceed.

• Example: C(s, diamond) + O2(g) CO2(g)

ΔG°rxn = -397 kJ

But diamonds are forever….

<<0

ΔG°rxn ≠ rate

Page 18: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Example Problem

• Is the following reaction spontaneous under standard conditions?

4KClO3(s) ⏐ → ⏐ 3KClO4 (s) +KCl(s)

ΔH°f

(kJ/mol)S°

(J/mol.K)

KClO3(s) -397.7 143.1

KClO4(s) -432.8 151.0

KCl (s) -436.7 82.6

Page 19: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Example Problem Solution

• Calulating ΔH°rxn

4KClO3(s) ⏐ → ⏐ 3KClO4 (s) +KCl(s)

ΔH°rxn = 3ΔH° f KClO4( ) + ΔH° f KCl( ) − 4ΔH° f KClO3( )

= 3(−432.8kJ) + (−436.7kJ) − 4(397.7kJ)

= −144kJ

• Calulating ΔS°rxn

ΔS°rxn = 3S° KClO4( ) + S° KCl( ) − 4S° KClO3( )

= 3(151.0J K) + (82.6J K) − 4(143.1J K)

= −36.8J K

Page 20: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Example Problem Solution

• Calulating ΔG°rxn

ΔG°rxn = ΔH°rxn −TΔS°rxn

= −144kJ − 298K( ) −38.6J K( )1kJ

1000J

⎝ ⎜

⎠ ⎟

= −133kJ

ΔG°rxn < 0 ;therefore, reaction is spontaneous.

Page 21: Lecture 8 Summary Spontaneous, exothermic Spontaneous, endothermic.

Example Problem Continued

For what temperatures will this reaction be spontaneous?

Answer: For T in which ΔGrxn < 0.

ΔGrxn = ΔHrxn −TΔSrxn0 = ΔHrxn −TΔSrxnΔHrxn

ΔSrxn=

−133kJ

−38.6JK( )1kJ

1000J

⎝ ⎜

⎠ ⎟= 3446K = T

Spontaneous as long as T < 3446 K.