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Spontaneity, Entropy, & Free Energy Chapter 16. 1st Law of Thermodynamics The first law of thermodynamics is a statement of the law of conservation of.

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Presentation on theme: "Spontaneity, Entropy, & Free Energy Chapter 16. 1st Law of Thermodynamics The first law of thermodynamics is a statement of the law of conservation of."— Presentation transcript:

1 Spontaneity, Entropy, & Free Energy Chapter 16

2 1st Law of Thermodynamics The first law of thermodynamics is a statement of the law of conservation of energy: energy can neither be created nor destroyed. The energy of the universe is constant, but the various forms of energy can be interchanged in physical and chemical processes.

3 Spontaneous Processes and Entropy Thermodynamics lets us predict whether a process will occur but gives no information about the amount of time required for the process. A spontaneous process is one that occurs without outside intervention.

4 Kinetics & Thermodynamics Chemical kinetics focuses on the pathway between reactants and products--the kinetics of a reaction depends upon activation energy, temperature, concentration, and catalysts. Thermodynamics only considers the initial and final states. To describe a reaction fully, both kinetics and thermodynamics are necessary.

5 The rate of a reaction depends on the pathway from reactants to products. Thermodynamics tells whether the reaction is spontaneous and depends upon initial & final states only.

6 Entropy The driving force for a spontaneous process is an increase in the entropy of the universe. Entropy, S, can be viewed as a measure of randomness, or disorder. Nature spontaneously proceeds toward the states that have the highest probabilities of existing.

7 The expansion of an ideal gas into an evacuated bulb.

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9 Positional Entropy A gas expands into a vacuum because the expanded state has the highest positional probability of states available to the system. Therefore, S solid < S liquid << S gas

10 Positional Entropy Which of the following has higher positional entropy? a) Solid CO 2 or gaseous CO 2 ? b) N 2 gas at 1 atm or N 2 gas at 1.0 x 10 -2 atm?

11 Entropy What is the sign of the entropy change for the following? a) Solid sugar is added to water to form a solution?  S is positive b) Iodine vapor condenses on a cold surface to form crystals?  S is negative

12 The Second Law of Thermodynamics...in any spontaneous process there is always an increase in the entropy of the universe.  S univ > 0 for a spontaneous process.

13  S Universe  S universe is positive -- reaction is spontaneous.  S universe is negative -- reaction is spontaneous in the reverse direction.  S universe = 0 -- reaction is at equilibrium.

14  G -- Free Energy Two tendencies exist in nature: tendency toward higher entropy --  Stendency toward higher entropy --  S tendency toward lower energy --  Htendency toward lower energy --  H If the two processes oppose each other (e.g. melting ice cube), then the direction is decided by the Free Energy,  G, and depends upon the temperature.

15 Free Energy  G =  H  T  S (from the standpoint of the system) A process (at constant T, P) is spontaneous in the direction in which free energy decreases:  G sys means +  S univ Entropy changes in the surroundings are primarily determined by the heat flow. An exothermic process in the system increases the entropy of the surroundings.

16  G,  H, &  S Spontaneous reactions are indicated by the following signs:  G = negative  H = negative  S = positive

17 Temperature Dependence  H o &  S o are  H o &  S o are not temperature dependent.  G o is temperature dependent.  G =  H  T  S

18  S surroundings  S surr is positive -- heat flows into the surroundings out of the system.  S surr is negative -- heat flows out of the surroundings and into the system.  S surr = -  H system T

19 Sb 2 S 3(s) + 3Fe (s) ---> 2Sb (s) + 3FeS (s)  H = -125 kJ Sb 4 O 6(s) + 6C (s) ---> 4Sb (s) + 6CO (g)  H = 778 kJ What is  S surr for these reactions at 25 0 C & 1 atm.  S surr = -  H system T  S surr = -(-125kJ/298K)  S surr = 419 J/K  S surroundings Calculations  S surr = -  H system T  S surr = -(778kJ/298K)  S surr = -2.61 x 10 3 J/K

20 Effect of  H and  S on Spontaneity

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22 Calculations showing that the melting of ice is temperature dependent. The process is spontaneous above 0 o C.

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24 Free Energy  G  G =  H  T  S  G = negative -- spontaneous  G = positive -- spontaneous in opposite direction  G = 0 -- at equilibrium

25 Boiling Point Calculations What is the normal boiling point for liquid Br 2 ? Br 2(l) ---> Br 2(g)  H o = 31.0 kJ/mol &  S o = 93.0 J/Kmol  G o = 0 At equilibrium,  G o = 0  G o =  H o  T  S 0 = 0  H o = T  S 0 T =  H o /  S 0 T = 3.10 x 10 4 J/mol/(93.0J/Kmol) T = 333K

26 The Third Law of Thermodynamics... the entropy of a perfect crystal at 0 K is zero. Because S is explicitly known (= 0) at 0 K, S values at other temps can be calculated. See Appendix 4 for values of S 0.

27  S o reaction Calculate  S  at 25 o C for the reaction 2NiS (s) + 3O 2(g) ---> 2SO 2(g) +2NiO (s)  S  =  n p S  (products)   n r S  (reactants)  S  = [(2 mol SO 2 )(248 J/Kmol) + (2 mol NiO)(38 J/Kmol)] - [(2 mol NiS)(53 J/Kmol) + (3 mol O 2 )(205 J/Kmol)]  S  = 496 J/K + 76 J/K - 106 J/K - 615 J/K  S  = -149 J/K # gaseous molecules decreases!

28 SoSo SoSo S o increases with: solid ---> liquid ---> gassolid ---> liquid ---> gas greater complexity of molecules (have a greater number of rotations and vibrations)greater complexity of molecules (have a greater number of rotations and vibrations) greater temperature (if volume increases)greater temperature (if volume increases) lower pressure (if volume increases)lower pressure (if volume increases)

29 Free Energy Change and Chemical Reactions  G  = standard free energy change that occurs if reactants in their standard state are converted to products in their standard state.  G  =  n p  G f  (products)   n r  G f  (reactants) The more negative the value of  G  the further a reaction will go to the right to reach equilibrium.

30  G  Calculations Calculate ,  S  G  for the reaction  SO 2(g) + O 2(g) ----> 2 SO 3(g)  =  n p  H f  (products)   n r  H f  (reactants)  = [(2 mol SO 3 )(-396 kJ/mol)]-[(2 mol SO 2 )(-297 kJ/mol) + (0 kJ/mol)]  H  = - 792 kJ + 594 kJ  H  = -198 kJ

31  G  Calculations Continued  S  =  n p S  (products)   n r S  (reactants)  S  = [(2 mol SO 3 )(257 J/Kmol)]-[(2 mol SO 2 )(248 J/Kmol) + (1 mol O 2 )(205 J/Kmol)]  S  = 514 J/K - 496 J/K - 205 J/K  S  = -187 J/K

32  G  Calculations Continued  G o =  H o  T  S o  G o = - 198 kJ - (298 K)(-187 J/K)(1kJ/1000J)  G o = - 198 kJ + 55.7 kJ  G o = - 142 kJ The reaction is spontaneous at 25 o C and 1 atm.

33 Hess’s Law &  G o C diamond(s) + O 2(g) ---> CO 2(g) C diamond(s) + O 2(g) ---> CO 2(g)  G o = -397 kJ C graphite(s) + O 2(g) ---> CO 2(g) C graphite(s) + O 2(g) ---> CO 2(g)  G o = -394 kJ Calculate  G o for the reaction C diamond(s) ---> C graphite(s) C diamond(s) + O 2(g) ---> CO 2(g) C diamond(s) + O 2(g) ---> CO 2(g)  G o = -397 kJ CO 2(g) ---> C graphite(s) + O 2(g) CO 2(g) ---> C graphite(s) + O 2(g)  G o = +394 kJ C diamond(s) ---> C graphite(s)  G o = -3 kJ Diamond is kinetically stable, but thermodynamically unstable.

34  G o & Temperature  G o depends upon temperature. If a reaction must be carried out at temperatures higher than 25 o C, then  G o must be recalculated from the  H o &  S o values for the reaction.

35 Free Energy & Pressure The equilibrium position represents the lowest free energy value available to a particular system (reaction).  G is pressure dependent  S is pressure dependent  is not pressure dependent

36 Free Energy and Pressure  G =  G  + RT ln(Q) Q = reaction quotient from the law of mass action.

37 Free Energy Calculations CO (g) + 2H 2(g) ---> CH 3 OH (l). CO (g) + 2H 2(g) ---> CH 3 OH (l) Calculate Calculate  G o for this reaction where CO (g) is 5.0 atm and H 2(g) is 3.0 atm are converted to liquid methanol.  G  =  n p  G f  (products)   n r  G f  (reactants)  G  =  mol CH 3 OH)(- 166 kJ/mol)]-[(1 mol CO)(-137 kJ/mol) + (0 kJ)]  G  =  kJ + 137 kJ  G  =  x 10 4 J

38 Free Energy Calculations Continued = 2.2 x 10 -2

39 Free Energy Calculations Continued  G =  G  + RT ln(Q)  G = (-2.9 x 10 4 J /mol rxn) + (8.3145 J/Kmol)(298 K) ln(2.2 x 10 -2 )  G =  x 10 4 J/mol rxn) - (9.4 x 10 3 J/mol rxn)  G = - 38 kJ/ mol rxn Note:  G is significantly more negative than  G  implying that the reaction is more spontaneous at reactant pressures greater than 1 atm. Why?

40 A system can achieve the lowest possible free energy by going to equilibrium, not by going to completion.

41 As A is changed into B, the pressure and free energy of A decreases, while the pressure and free energy of B increases until they become equal at equilibrium.

42 Graph a) represents equilibrium starting from only reactants, while Graph b) starts from products only. Graph c) represents the graph for the total system.

43 Free Energy and Equilibrium  G  =  RT ln(K) K = equilibrium constant This is so because  G = 0 and Q = K at equilibrium.

44  G o & K  G o = 0K = 1  G  1 (favored)  G  not favored)

45 Equilibrium Calculations 4Fe (s) + 3O 2(g) 2Fe 2 O 3(s) Calculate K for this reaction at 25 o C.  G o = - 1.490 x 10 6 J  H o = - 1.652 x 10 6 J  S o = -543 J/K  G  =  RT ln(K) K = e -  G  R  K = e 601 or 10 261 K is very large because  G  is very negative.

46 Temperature Dependence of K y = mx + b y = mx + b (  H  and S   independent of temperature over a small temperature range) If the temperature increases, K decreases for exothermic reactions, but increases for endothermic reactions.

47 Free Energy & Work The maximum possible useful work obtainable from a process at constant temperature and pressure is equal to the change in free energy: w max =  G

48 Reversible vs. 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).  w < All real processes are irreversible -- (some work is changed to heat).  w <  G Work is changed to heat in the surroundings and the entropy of the universe increases.

49 Laws of Thermodynamics First Law: You can’t win, you can only break even. Second Law: You can’t break even.


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