Chap19 Thermodynamics Ppt

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Chapter 19 Chemical Thermodynamics John D. Bookstaver St. Charles Community College St. Peters, MO 2006, Prentice Hall, Inc. Modified by S.A. Green, 2006 Modified by D. Amuso 2011

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Transcript of Chap19 Thermodynamics Ppt

  • Chapter 19Chemical ThermodynamicsJohn D. BookstaverSt. Charles Community CollegeSt. Peters, MO2006, Prentice Hall, Inc.Modified by S.A. Green, 2006Modified by D. Amuso 2011

  • ThermodynamicsThe study of the relationships between heat, work, and the energy of a system.

  • First Law of ThermodynamicsYou will recall from Chapter 5 that energy cannot be created nor destroyed.Therefore, the total energy of the universe is a constant.Energy can, however, be converted from one form to another or transferred from a system to the surroundings or vice versa.

  • Second Law of Thermodynamics

    The total Entropy of the universe increases in any spontaneous, irreversible process.

  • EntropyEntropy can be thought of as a measure of the randomness or disorder of a system.It is related to the various modes of motion in molecules (microstates). Vibrational Rotational Translational

  • EntropyMolecules have more entropy (disorder) when:Phase Changes from: S L G Example: Sublimation CO2(s) CO2(g) Dissolving occurs (solution forms): Example: NaCl(s) Na+(aq) + Cl-(aq)

  • Entropy3) Temperature increases Example: Fe(s) at 0 oC Fe(s) at 25 oC 4) For Gases ONLY, when Volume increases or Pressure decreases Examples: 2 Liters He(g) 4 Liters He(g) 3 atm He(g) 1 atm He(g)

  • Entropy5) Rx results in more molecules/moles of gas Examples: 2NH3(g) N2(g) + 3H2(g) CaCO3(s) CaO(s) + CO2(g)

    N2O4(g) 2 NO2(g) This one is difficult to predict: N2(g) + O2(g) 2 NO(g)

  • EntropyWhen there are more moles Example: 1 mole H2O(g) 2 moles H2O(g)

    7) When there are more atoms per molecule Examples: 1 mole Ar(g) 1 mole HCl(g)

    1 mole NO2(g) 1 mole N2O4(g)

  • Entropy8) When an atom has a bigger atomic number 1 mole He(g) 1 mole Ne (g)

  • Spontaneous ProcessesSpontaneous processes are those that can proceed without any outside intervention.The gas in vessel B will spontaneously effuse into vessel A, but once the gas is in both vessels, it will not spontaneously move to just one vessel.

  • Spontaneous ProcessesProcesses that are spontaneous at one temperature may be nonspontaneous at other temperatures.Above 0C it is spontaneous for ice to melt.Below 0C the reverse process is spontaneous.

  • Spontaneous ProcessesProcesses that are spontaneous in one direction are nonspontaneous in the reverse direction.Spontaneous processes are irreversible.

  • Second Law of ThermodynamicsA reversible process results in no overall change in Entropy while an irreversible, spontaneous process results in an overall increase in Entropy.Reversible:Irreversible (Spontaneous):

  • Third Law of Thermodynamics

    The Entropy of a pure crystalline substance at absolute zero is zero. why?

  • Third Law of Thermodynamics

  • Standard EntropiesStandard Conditions: 298 K, 1 atm, 1 Molar

    The values for Standard Entropies (So) are expressed in J/mol-K. Note: Increase with increasing molar mass.

  • Standard EntropiesLarger and more complex molecules have greater entropies.

  • Entropy ChangesDSo = S n Soproducts - S m SoreactantsBe careful: Sunits are in J/mol-K

    Note for pure elements:

  • Gibbs Free Energy Use G to decide if a process is spontaneous

    G = negative value = spontaneous G = zero = at equilibrium G = positive value = not spontaneous

    Note: equation can be used w/o the o too. DGo = DHo TDSo

  • Gibbs Free EnergyIf DG is negative DG = maximum amt of energy free to do work by the reaction

    2. If G is positive DG = minimum amt of work needed to make the reaction happen DGo = DHo TDSo

  • Gibbs Free Energy

    In our tables, units are: DGo = kJ/mol DHo = kJ/mol DSo = J/mol-K

    DGo = DHo TDSo

  • Free Energy and TemperatureThere are two parts to the free energy equation: H the enthalpy term TS the entropy term

    The temperature dependence of free energy comes from the entropy term.

  • What causes a reaction to be spontaneous?Think Humpty DumptySystem tend to seek: Minimum Enthalpy Exothermic Rx, DH = negative Maximum Entropy More disorder, DS = positiveBecause: DGo = DHo TDSo - = (-) - (+)

  • Free Energy and TemperatureBy knowing the sign (+ or -) of S and H, we can get the sign of G and determine if a reaction is spontaneous.

  • At Equilibrium

    DGo = zero Therefore: DHo = TDSo

    Or: DSo = DHo T

    Use this equation when asked to calculate enthalpy of vaporization or enthalpy of fusion.

    DGo = DHo TDSo

  • DGo = S n Gof products - S m Go f reactantsStandard Free Energy Changes

    Be careful: Values for Gf are in kJ/mol G can be looked up in tables or calculated from S and H. DGo = DHo TDSo

  • Free Energy and EquilibriumRemember from above:If DG is 0, the system is at equilibrium.So DG must be related to the equilibrium constant, K (chapter 15). The standard free energy, DG, is directly linked to Keq by:

    DGo = - RT ln K Where R = 8.314 J/mol-K

  • DGo = - RT ln K

    If the free energy change is a negative value,the reaction is spontaneous, ln K must be a positive value, and K will be a large number meaning the equilibrium mixture is mainly products.

    If the free energy change is zero, ln K = zero and K = one.

    Relationships

  • Free Energy and EquilibriumUnder non-standard conditions, we need to use DG instead of DG.

    Q is the reaction quotient from chapter 15.

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