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Enthalpy
ΔH = ΔE + PΔV For constant pressure processes only At a constant pressure, ΔHsys = energy flow as heat (and work).
Enthalpy Equation
ΔH°rxn = ΣnΔH°f (products) - ΣnΔH°f (reactants) Standard molar enthalpy (1 mol formed) ΔH°rxn = Σ bond energies (reactants) - Σ bond energies (products) Gas phase reactions only
Hess' Law
Enthalpic change (ΔH) for a process is a constant whether the process occurs in one step OR a series of steps. ΔH°rxn = ΔH°1+ ΔH°2
ΔH properties
If ΔH = negative, process is exothermic. If ΔH = positive, process is endothermic. Sign of ΔH does not necessarily predict spontaneity of a reaction.
Entropy
Measure of disorder/randomness of a system 2nd Law of Thermodynamics dictates that ΔSuniv = ΔSsys + ΔSsurr At equilibrium, ΔSuniv = 0. ΔSgas >> ΔSliquid > ΔSsolid
Entropy Equations
ΔS° = ΣnΔS° (products) - ΣnΔS° (reactants) ΔSsurr = (-ΔHsys) / T Entropy of a pure crystal = 0
Gibbs Free Energy (ΔG)
ΔG = ΔHsys - T(ΔSsys) When ΔG = negative, processes are spontaneous; when ΔG = positive, processes are spontaneous in the reverse direction. When ΔG = 0, processes are at equilibrium.
ΔG° (ΔG at standard conditions)
ΔG°rxn = ΣnΔG°f (products) - ΣnΔG°f (reactants) ΔG°rxn = ΔH°rxn - TΔS°rxn
ΔG at non-standard conditions
ΔG = ΔG° + RTln(Q) where R = 8.3145 J/K mol T = temperature in K (C + 273.25) Q = ratio of products/reactants
How to determine boiling point
ΔHvap = TΔSvap T = ΔHvap / ΔSvap
Interpreting K Values
K > 1: large, ΔGf is negative, spontaneous K < 1: small, ΔGf is positive, non-spontaneous K = 0: slope is 0, ΔGf is 0, reaction at equilibrium
Equilibrium
Point at which opposing processes (forward and reverse reactions) occur at the same rate. Reversible processes only Dynamic
Kc
[A]a[B]b/[C]c[D]d
Kp
Kp = Kc(RT)Δn Where R = .08206, T = temperature in K, Δn = change in # moles of gas
Reversing an Equation
Knew = 1/Kold

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