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adiabatic process
no heat is exchanged between the system and the environment
thermal energy of the system is constant throughout the process
isothermal process
system’s temperature remains constant
total energy of the system (U) is constant throughout the process
isobaric process
pressure of the system is constant
isovolumetric (isochoric) process
no change in volume
no work is performed; ΔU = Q
Hess’s Law
enthalpy changes of reactions are additive
second law of thermodynamics (entropy)
energy spontaneously disperses from being localized to becoming spread out if it is not hindered from doing so
ΔS = Qrev/T
Qrev = heat that is gained or loss in a reversible process
ΔSuniverse = ΔSsystem + ΔSsurroundings > 0
Gibbs free energy
ΔG = ΔH - TΔS
endergonic = system releases energy (ΔG < 0) and is spontaneous
exergonic = system gains energy (ΔG > 0) and is nonspontaneous
effect of ΔH and ΔS on ΔG
ΔH | ΔS | outcome |
|---|---|---|
+ | + | spontaneous at high T |
+ | - | nonspontaneous at all T |
- | + | spontaneous at all T |
- | - | spontaneous at low T |
standard Gibbs free energy
ΔGrxno = ΣΔGf,productso - ΣΔGi,reactantso
Free energy, Keq, and Q
ΔGrxno = -RT ln(Keq)
ΔGrxn = ΔGrxno + RT ln(Q) = RT ln(Q/Keq)