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Ch. 20: Entropy and Free Energy

Ch. 20: Entropy and Free Energy. Thermodynamics: the science of energy transfer Objective: To learn how chemists predict when reactions will be product-favored vs. when they will be reactant-favored Spontaneous Processes and Entropy

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Ch. 20: Entropy and Free Energy

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  1. Ch. 20: Entropy and Free Energy • Thermodynamics: the science of energy transfer • Objective: To learn how chemists predict when reactions will be product-favored vs. when they will be reactant-favored • Spontaneous Processes and Entropy • Spontaneous processes occurs without outside intervention • Spontaneous processes can be fast or slow

  2. Section 20.1 • ØThermodynamics tells us NOTHING about the rate of reaction. • The study of rates and why some reactions are fast and others are slow is called kinetics • activation energy • temperature • concentration • catalysts

  3. Section 20.2 Entropy • Entropy, S:Measure of dispersal or disorder. • ØCan be measured with a calorimeter. Assumes in a perfect crystal at absolute zero, no disorder and S = 0. • ØIf temperature change is very small, can calculate entropy change, DS = q/T (heat absorbed / T at which change occurs) • ØSum of DS can give total entropy at any desired temperature. See Table 20.1

  4. Section 20.2 Entropy • In general, the final state is more probable than the initial one if: • (1)energy can be dispersed over a greater number of atoms and molecules (hot  cold) • (2)the atoms and molecules can be more disordered (dissolving, diffusion of gas)

  5. Section 20.2 Entropy • More specifically, • (1)if energy and matter are both more dispersed, it is definitely product-favored • (2)if only energy or matter is dispersed, then quantitative information is necessary to decide which effects are greater • (3)if neither matter nor energy is more dispersed, then the process will be reactant-favored

  6. Entropy Examples (positive DS) • Boiling water • Melting ice • Preparing solutions • CaCO3 (s)  CaO (s) + CO2 (g)

  7. Entropy Examples (negative DS) • Molecules of gas collecting • Liquid converting to solid at room temp • 2 CO (g) + O2 (g)  2 CO2 (g) • Ag+ (aq) + Cl-(aq)  AgCl (s)

  8. Entropy Generalizations • Sgas > S liquid > Ssolid • Entropies of more complex molecules are larger than those of simpler molecules (Spropane > Sethane>Smethane) • Entropies of ionic solids are higher when attraction between ions are weaker. ØEntropy usually increases when a pure liquid or solid dissolves in a solvent. Entropy increases when a dissolved gas escapes from a solution

  9. Laws of Thermodynamics • First law: Total energy of the universe is a constant. • Second law: Total entropy of the universe is always increasing. • Third law: Entropy of a pure, perfectly formed crystalline substance at absolute zero = 0.

  10. Calculating DSosystem • DSosystem =  So (products) -  So (reactants) Can also relate surroundings to the system! • DSosurroundings = q surroundings / T = - DHsystem / T

  11. Calculating DSouniverse • DSouniverse = DSosurroundings +DSosystem • DSouniverse = - DHsystem / T +DSosystem • Can use 2nd law to predict whether a reaction is product-favored or reactant-favored! • The higher the temperature, the less important the enthalpy term is!

  12. Roald Hoffmann (1981 Nobel prize): “One amusing way to describe synthetic chemistry, the making of molecules that is at the intellectual and economic center of chemistry, is that it is the local defeat of entropy.”

  13. Spontaneity, Entropy & Free Energy • Spontaneous Processes • a ball rolls downhill, but the ball never spontaneously rolls uphill • steel rusts, but the rust never spontaneously forms iron and oxygen • a gas fills its container, but a gas will never spontaneously collect in one corner of the container. • Water spontaneously freezes at temperatures below 0o C

  14. Spontaneity, Entropy & Free Energy • Sign of DS depends on the heat flow • Exothermic Rxn: DSsurr >0 • Endothermic Rxn: DSsurr< 0 • Magnitude of DS is determined by the temperature • DSsurr = - DH T

  15. 20.3 Gibbs Free Energy • DG is a measure of the maximum magnitude of the net useful work that can be obtained from a reaction!

  16. 20.3 Gibbs Free Energy • DGsystem = - T DSuniverse = DHsystem - TDSsystem • DGosystem = DHosystem - T DSosystem • DGorxn = DHorxn - T DSorxn

  17. 20.3 Gibbs Free Energy • DGosystem or DGorxn If negative, then product-favored. If positive, then reactant-favored. • DGoreaction =  Gfo (products) -  Gfo (reactants)

  18. 20.3 Gibbs Free Energy • DG is a measure of the maximum magnitude of the net useful work that can be obtained from a reaction! • Know the meaning of enthalpy-driven vs. entropy-driven reactions. DGs are additive!

  19. 20.4 Thermodynamics and K If not at standard conditions, DG = DGo + RT ln Q  (Equilibrium is characterized by the inability to do work.) At equilibrium, Q = K and DG = O Therefore, substituting into previous equation gives 0 = DGo + RT ln K and DGo = - RT ln K (can use Kp or Kc)

  20. 2020.5      Thermodynamics and Time • First law: Total energy of the universe is a constant. • Second law: Total entropy of the universe is always increasing. • Third law: Entropy of a pure, perfectly formed crystalline substance at absolute zero = 0. • Entropy : time’s arrow • Absolutely MUST learn table in Chapter highlights!

  21. 20.4 Thermodynamics and K • ØUnderstand relationship between DGo, K, and product-favored reactions! • DGo<0 K>1 product-favored • DGo=0 K=1 • DGo>0 K<1 reactant-favored

  22. Spontaneity, Entropy & Free Energy • Relationship between DGo and Keq • DGo Keq • = 0 1 • < 0 >1 • > 0 < 1

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