Free Energy and Equilibrium

Free Energy and Equilibrium

  • This lecture connects thermodynamics and kinetics.

Standard vs. Non-Standard States

  • Reactants and products are only in their standard states for an instant during a reaction.
  • Standard states for reactions in solution are 1 mol/L concentrations.
  • For gases, standard state is 1 atmosphere of pressure.
  • ΔG\Delta G in standard states predicts the direction of reaction at equilibrium.
  • ΔG\Delta G in non-standard states predicts the direction of reaction given specific reaction conditions.

Equation for Non-Standard Gibbs Free Energy

  • ΔG=ΔG+RTlogQ\Delta G = \Delta G^{\circ} + RT \log Q
    • ΔG\Delta G: Gibbs free energy under non-standard conditions.
    • ΔG\Delta G^{\circ}: Gibbs free energy under standard conditions.
    • R: Ideal gas constant (8.314 J/mol*K).
    • T: Temperature in Kelvin.
    • Q: Reaction quotient (proportional to product concentrations over reactant concentrations, each raised to their stoichiometric powers).

Equilibrium Conditions

  • At equilibrium, Q becomes K (equilibrium constant).
  • At equilibrium, ΔG=0\Delta G = 0, meaning the change in entropy of the universe is zero.
  • Therefore, ΔG=RTlogK\Delta G^{\circ} = -RT \log K
    • This equation links thermodynamics (ΔG\Delta G) and kinetics (K).

Relationship Between K and ΔG\Delta G

  • K approaches 1: Significant amounts of both reactants and products are present at equilibrium.
  • K = 1: ΔG=0\Delta G = 0. Products and reactants are equally favored at equilibrium.
  • K > 1: ΔG\Delta G is negative. Products are favored (forward reaction is spontaneous).
  • K < 1: ΔG\Delta G is positive. Reactants are favored (reverse reaction is spontaneous).

Calculating K from Calorimetry

  • Sometimes it's experimentally impossible to make the kinetics measurements to get K, but easy to measure ΔG\Delta G with thermodynamic experiments.
  • Conversely, if kinetics experiments give K, ΔG\Delta G can be back-calculated.

Interpreting ΔG\Delta G and K

  • K is proportional to product concentrations at equilibrium over reactant concentrations at equilibrium.
  • K > 1 means the numerator (products) is much bigger than the denominator (reactants).
  • K < 1 means the denominator (reactants) is bigger than the numerator (products), favoring the reverse reaction.

Free Energy and Reaction Direction

  • A negative ΔG\Delta G indicates a forward reaction.
  • The value of Q can place the system on either side of ΔG\Delta G^\circ on a free energy diagram, influencing the initial reaction direction until equilibrium is reached.

Example Problem 1: Calculating ΔG\Delta G^\circ and Kp

  • Reaction: PCl<em>5(g)PCl</em>3(g)+Cl2(g)PCl<em>5(g) \rightleftharpoons PCl</em>3(g) + Cl_2(g)
  • Given: ΔGf\Delta G_f^\circ values for reactants and products at 25°C.
  • Steps:
    • Calculate ΔG\Delta G^\circ for the reaction using the formula:
      ΔG<em>rxn=ΣΔG</em>f(products)ΣΔGf(reactants)\Delta G^\circ<em>{rxn} = \Sigma \Delta G</em>f^\circ (products) - \Sigma \Delta G_f^\circ (reactants)
    • Use ΔG=RTlogK\Delta G^\circ = -RT \log K to solve for Kp.
      • logK=ΔGRTlog K = - \frac{\Delta G^\circ}{RT}
      • K=eΔGRTK = e^{-\frac{\Delta G^\circ}{RT}}
  • Solution:
    • ΔG=+39 kJ\Delta G^\circ = +39 \text{ kJ}
    • Kp=1.5×107Kp = 1.5 \times 10^{-7}
  • Interpretation:
    • Reaction lies strongly in the reverse direction at equilibrium because ΔG\Delta G^\circ is positive and Kp << 1.

Example Problem 2: Calculating ΔG\Delta G under Non-Standard Conditions

  • Using the same reaction as above, calculate ΔG\Delta G given initial partial pressures.
  • Use the equation: ΔG=ΔG+RTlogQ\Delta G = \Delta G^\circ + RT \log Q
  • Calculate Q using initial partial pressures:
    • Q=P<em>PCl</em>3×P<em>Cl</em>2P<em>PCl</em>5Q = \frac{P<em>{PCl</em>3} \times P<em>{Cl</em>2}}{P<em>{PCl</em>5}}
  • Solution:
    • Q=37Q = 37
    • ΔG=+48 kJ\Delta G = +48 \text{ kJ}
  • Interpretation:
    • The reaction will proceed in reverse under these conditions because Q > K and ΔG\Delta G is positive.

Example Problem 3: Ozone Depletion

  • Reaction: NO(g)+O<em>3(g)NO</em>2(g)+O2(g)NO(g) + O<em>3(g) \rightarrow NO</em>2(g) + O_2(g)
  • Use data from appendix three to calculate ΔG\Delta G^{\circ} and K at 298 K.
  • ΔG<em>rxn=ΣΔG</em>f(products)ΣΔGf(reactants)\Delta G^\circ<em>{rxn} = \Sigma \Delta G</em>f^\circ (products) - \Sigma \Delta G_f^\circ (reactants)
  • Solution:
    • ΔG=198.3 kJ\Delta G^\circ = -198.3 \text{ kJ}
    • K=5.76×1034K = 5.76 \times 10^{34}
  • Interpretation:
    • The forward reaction is highly favored because ΔG\Delta G^{\circ} is large and negative, and K is very large.

Example Problem 4: Autoionization of Water

  • Reaction: H2O(l)H+(aq)+OH(aq)H_2O(l) \rightleftharpoons H^+(aq) + OH^-(aq)
  • K = 1×10141 \times 10^{-14} at 25°C.
  • Calculate ΔG\Delta G^{\circ} using ΔG=RTlogK\Delta G^\circ = -RT \log K
  • Solution:
    • ΔG=+79.9 kJ/mol\Delta G^\circ = +79.9 \text{ kJ/mol}
  • Interpretation:
    • The autoionization of water is not favored forward because ΔG\Delta G^{\circ} is large and positive and K is very small.
  • At 40°C, ΔG\Delta G^{\circ} = +81.1 kJ/mol, showing the reaction remains unfavorable forward.

Predicting Signs of Thermodynamic Quantities Without Math

  • For the reaction: H2(g)2H(g)H_2(g) \rightarrow 2H(g)
  • Predict the signs of ΔH\Delta H and ΔS\Delta S and spontaneity at high or low temperatures.
  • ΔS\Delta S is positive because one mole of gas goes to two moles of gas, increasing disorder.
  • ΔH\Delta H is endothermic (positive) because it takes energy to break stable H-H bonds.
    • High temperatures would favor spontaneity.

Rubber Band Entropy

  • Relaxed rubber has higher entropy, stretched rubber has lower entropy because polymer chains align.
  • Contraction is spontaneous.

Nursery Rhyme and Second Law of Thermodynamics

  • Humpty Dumpty illustrates the second law. It is easy to break an egg (increase entropy) but impossible to perfectly restore it (decrease entropy).

Environmental Studies Excerpt

  • Discusses the misconceptions the general public has about energy.
  • The first law of thermodynamics, says that energy is conserved.
  • The second law says that energy changes from a more useful to a less useful form every time it's converted with the first law.
  • The second law is really why we have an energy crisis.