Free Energy & Thermodynamics Notes

Thermodynamics & The First Law

  • The energy of the universe is constant.
  • ΔE=w+q\Delta E = w + q
    • w=PΔVw = -P\Delta V (+ if work done to system, - if work done by system).
    • Constant pressure: qP=ΔEw=ΔE+PΔV=ΔHq_P = \Delta E - w = \Delta E + P\Delta V = \Delta H
    • q (+) if heat enters the system (endothermic), q (-) if heat leaves the system (exothermic).

Spontaneous Reactions

  • Proceeds on its own without continuous external influence.
  • Non-spontaneous reactions require continuous external influence (energy).
  • Combustion is a spontaneous, exothermic reaction.
  • Cold pack reactions are spontaneous and endothermic.
  • Enthalpy change ΔH\Delta H alone doesn't indicate spontaneity.

Gibbs Free Energy and Spontaneity

  • Spontaneity is determined by the free energy change of the system.
  • Thermodynamically favorable: \Delta G < 0 (negative).
  • Thermodynamically unfavorable: \Delta G > 0 (positive).
  • ΔG=ΔHTΔS\Delta G = \Delta H - T\Delta S
    • ΔG\Delta G: Gibbs Free Energy change (kJ/mol).
    • ΔH\Delta H: Enthalpy change (kJ/mol).
    • ΔS\Delta S: Entropy change (J/K).
    • T: Temperature (K).

Entropy

  • Measure of disorder or energy dispersal in a system (J/K or J/(mol·K)).
  • S=k<em>BlnWS = k<em>B \cdot \ln W (k</em>Bk</em>B is Boltzmann constant, W is # of energetically equivalent arrangements).
  • Third Law: Entropy of a perfectly ordered crystalline substance at 0 K is zero.
  • Absolute entropy (S) increases with increasing temperature.
  • Standard Molar Entropy (SS^\circ): Absolute entropy of one mole of a pure substance at 1 atm and a specified temperature (usually 25 °C).
  • In general: SS^\circ (gas) > SS^\circ (liquid) > SS^\circ (solid).

Entropy Change

  • \Delta S > 0: Entropy increases (greater energy dispersal).
  • \Delta S < 0: Entropy decreases (less energy dispersal).
  • ΔS=S<em>finalS</em>initial\Delta S = S<em>{\text{final}} - S</em>{\text{initial}}
  • Entropy increases with temperature, volume, and number of independent particles.
  • Phase changes: fusion/melting, vaporization, and sublimation increase entropy (\Delta S > 0); freezing, condensation, and deposition decrease entropy (\Delta S < 0).

Standard Entropy of Reaction

  • ΔSrxn=[cS(C)+dS(D)][aS(A)+bS(B)]\Delta S^\circ_{rxn} = [cS^\circ(C) + dS^\circ(D)] − [aS^\circ(A) + bS^\circ(B)] for the reaction: aA + bB → cC + dD

The Laws of Thermodynamics

  • 1st Law: Energy of the universe is constant.
  • 3rd Law: Entropy of a perfectly ordered crystalline substance at 0 K is zero.
  • 2nd Law: For a spontaneous process, the total entropy of the universe always increases (\Delta S_{universe} > 0).
  • \Delta S{universe} = \Delta S{system} + \Delta S_{surroundings} > 0

Entropy of Surroundings

  • ΔS<em>surrq</em>sysΔHrx\Delta S<em>{surr} \propto -q</em>{sys} \propto \Delta H_{rx}
  • Exothermic: ΔH<em>rx<0\Delta H<em>{rx} < 0, \Delta S{surroundings} > 0
  • Endothermic: ΔH<em>rx>0\Delta H<em>{rx} > 0, \Delta S{surroundings} < 0

Gibbs Free Energy and the Universe

  • TΔSuniverse=ΔG=ΔHTΔS-T\Delta S_{universe} = \Delta G = \Delta H - T\Delta S
  • If \Delta S_{universe} > 0, then \Delta G < 0 (thermodynamically favorable/spontaneous).
  • If ΔSuniverse<0\Delta S_{universe} < 0, then ΔG>0\Delta G > 0 (thermodynamically unfavorable/non-spontaneous).

Gibbs Free Energy and Equilibrium

  • \Delta G < 0: Reaction is thermodynamically favorable.
  • \Delta G > 0: Reaction is thermodynamically unfavorable.
  • ΔG=0\Delta G = 0: Reaction is at equilibrium.
  • ΔG+TΔS=ΔH\Delta G + T\Delta S = \Delta H

Spontaneity and Temperature

  • ΔG=ΔHTΔS\Delta G = \Delta H - T\Delta S
  • ΔH<0\Delta H < 0 and ΔS>0\Delta S > 0: ΔG\Delta G always negative (spontaneous at all temperatures).
  • \Delta H > 0 and \Delta S < 0: ΔG\Delta G always positive (non-spontaneous at all temperatures).
  • \Delta H < 0 and \Delta S < 0: ΔG\Delta G temperature-dependent (spontaneous at low temperatures).
  • \Delta H > 0 and \Delta S > 0: ΔG\Delta G temperature-dependent (spontaneous at high temperatures).

Calculating Standard Free Energy Changes (ΔGrx\Delta G^\circ_{rx})

  • ΔG<em>rx=ΔH</em>rxTΔSrx\Delta G^\circ<em>{rx} = \Delta H^\circ</em>{rx} - T\Delta S^\circ_{rx}
  • ΔH<em>rx=n</em>pΔH<em>f(products)n</em>rΔHf(reactants)\Delta H^\circ<em>{rx} = \sum n</em>p \Delta H^\circ<em>f (products) - \sum n</em>r \Delta H^\circ_f (reactants)
  • ΔS<em>rx=n</em>pS(products)nrS(reactants)\Delta S^\circ<em>{rx} = \sum n</em>p S^\circ(products) - \sum n_r S^\circ(reactants)

Using Tabulated Values of ΔGf\Delta G^\circ_f

  • ΔGf\Delta G^\circ_f: Standard free energy of formation of 1 mole of a compound from its elements in their standard states.
  • For an element in its most stable form at 25 °C, ΔH<em>f=0\Delta H^\circ<em>f = 0 and ΔG</em>f=0\Delta G^\circ</em>f = 0
  • A substance with a negative ΔGf\Delta G^\circ_f is thermodynamically stable.
  • A substance with a positive ΔGf\Delta G^\circ_f is thermodynamically unstable.

Hess’s Law

  • If ΔG<em>rx\Delta G^\circ<em>{rx} is known for a series of stepwise reactions, ΔG</em>rx\Delta G^\circ</em>{rx} can be determined.

Non-Standard Conditions

  • ΔG<em>rx=ΔG</em>rx+RTlnQ\Delta G<em>{rx} = \Delta G^\circ</em>{rx} + RT \cdot \ln Q
    • R: gas constant 8.314 J/(mol·K)
    • T: absolute temperature, K