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CHEMICAL THERMODYNAMICS The Second Law of Thermodynamics: The is an inherent direction in which any system not at equilibrium moves Processes that are.

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Presentation on theme: "CHEMICAL THERMODYNAMICS The Second Law of Thermodynamics: The is an inherent direction in which any system not at equilibrium moves Processes that are."— Presentation transcript:

1 CHEMICAL THERMODYNAMICS The Second Law of Thermodynamics: The is an inherent direction in which any system not at equilibrium moves Processes that are spontaneous in one direction are not spontaneous in the reverse direction

2 CHEMICAL THERMODYNAMICS Spontaneity, Enthalpy, and Entropy Reactions that are exothermic are generally spontaneous,  H < 0 Reactions that are not exothermic may also be spontaneous  H = 0

3 CHEMICAL THERMODYNAMICS  H > 0

4 CHEMICAL THERMODYNAMICS Spontaneity must, therefore, be a function of the degree of randomness in a system. Spontaneity, Enthalpy, and Entropy Entropy (S) is a “state function” that describes the randomness in a system such that,  S =  S final -  S initial

5 CHEMICAL THERMODYNAMICS The Second Law of Thermodynamics tells us that In any spontaneous process, there is always an increase in the entropy of the universe:  S universe =  S system +  S surroundings > 0

6 CHEMICAL THERMODYNAMICS A Molecular Interpretation of Entropy translational vibrational rotational The Third Law of Thermodynamics: S(0 K) = 0 The entropy of the lattice increases with temperature because the number of possible energy states in which the molecules or atoms are distributed is larger

7 CHEMICAL THERMODYNAMICS Calculation of Entropy Changes The standard entropy (S  ) is expressed in units of J/mol-K For any given reaction: aA + bB + …  cC + dD +...  S  = [cS  (p) + dS  (Q) + … ] - [ aS  (A) + bS  (B) + … ] Sample exercise : Calculate the  S for the synthesis of ammonia from N 2 and H 2 N 2 (g) + 3H 2 (g)  2NH 3 (g)  S  = [2S  (NH 3 )]- [ S  (N 2 ) + S  (H 2 )]  S  = [2(192 J/mol-K)]- [ 191.5 J/mol-K+ 3(130.58 J/mol-K)]  S  = -198.2 J/K

8 4 Ice melting 4 water condensing 4 mixing salt water 4 diffusion 4 butane burning 4 CH 4g + 2O 2g → CO 2g + 2H 2 O g

9 CHEMICAL THERMODYNAMICS Gibbs Free Energy Whether a reaction occurs spontaneously is determined by the changes in enthalpy and entropy for that reaction such that: G = H -TS The change in free energy is therefore:  G =  H - T  S If  G is negative, the reaction is spontaneous in the forward direction If  G is positive, the reaction is not spontaneous in the forward direction Work must be supplied from the surroundings to make it occur. If  G is zero, the reaction is at equilibrium, there is no driving force I get it!!

10 CHEMICAL THERMODYNAMICS aA + bB + …  cC + dD +...  G  = [cG  f (p) + dG  f (Q) + … ] - [aG  f (A) + bG  f (B) + … ] The standard free energy change (  G  ) for any reaction: Calculation of  G  using standard free energy change of formation

11 CHEMICAL THERMODYNAMICS

12 Sample exercise : Using the data from Appendix C, calculate the  G  using  H  and  S  for the following reaction: BaO(s) + CO 2 (g)  BaCO 3 (g)  H  = [-1216.3 kJ/mol] - [ -553.5 kJ/mol - 393.5 kJ/mol] = -269.3 kJ  G  = [-1137.6 kJ/mol] - [ -525.1 kJ/mol - 394.4 kJ/mol] = -218.1 kJ  S  = [112.1 J/mol-K] - [ 70.42 J/mol-K - 213.6 J/mol-K] = -171.9 J/mol-K  G =  H - T  S  G = -269.3 kJ - 298 K (-171.9 J/mol-K)(1 kJ/ 1000 J )  G = -218.07 kJ/mol

13 Free Energy and the Equilibrium Constant What happens when you can’t describe  G under standard conditions ?  G =  G ° + RT ln Q (R 8.314 J/K-mol) When  G = 0 then  G ° = - RT ln K  G ° is negative: K > 1  G ° is zero: K = 1  G ° is positive: K < 1

14 Calculate  G at 298 K for the following reaction if the reaction mixture consists of 1.0 atm N 2, 3.0 atm H 2,and 1.0 atm NH 3 N 2 (g) + 3H 2  2NH 3 Q = (1.0) 2 / (1.0)(3.0) 3 = 3.7 x 10 -2  G =  G ° + RT ln Q where R 8.314 J/K-mol  G = -33.32 kJ + (8.314x 10 -3 kJ/K-mol)(298 K)ln(3.7 x 10 -2 )  G = -41.49 kJ

15 CHEMICAL THERMODYNAMICS E k =  mv 2  E = E final - E initial  E = q + w if  V = 0 then,  E = q v if P is constant,  H =  E + P  V or,  H = q p  H   E  H= H products - H reactants   H f  H rxn =  n n (products) -   H f  m m (reactants) q = n C  T where C is J/mol-  C q = m S  T where is C J/g-  C Chapter 5 Hess’s Law 1st Law of Thermodynamics

16 CHEMICAL THERMODYNAMICS Chapter 19  S =  S final -  S initial  S universe =  S system +  S surroundings > 0 For any given reaction: aA + bB + …  cC + dD +...  S  = [cS  (p) + dS  (Q) + … ] - [ aS  (A) + bS  (B) + … ] where S  = J/mol-K  G =  H - T  S If  G = spontaneous If  G =not spontaneous If  G = zero, K = 0 aA + bB + …  cC + dD +...  G  = [cG  f (p) + dG  f (Q) + … ] - [aG  f (A) + bG  f (B) + … ] for any reaction:  G =  G ° + RT ln Q where R 8.314 J/K-mol if  G ° = 0 then  G ° = RT ln K  G ° is negative: K > 1  G ° is zero: K = 0  G ° is positive: K > 1 2nd Law of Thermodynamics 3rd Law of Thermodynamics


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