Second Law of Thermodynamics
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www.physics.sfsu.edu/~lwilliam/ 111/thermo/sld008.htm The second law of thermodynamics states that the universe (i.e. all systems) tend to the greatest degree of randomization. This concept is defined by the term entropy, S. S = k lnW Eqn. 12 where k = Boltzmann constant (the gas constant, R, divided by Avagadros' number) and W = the number of substrates. For an isothermal reversible reaction the change in entropy can be reduced to the term: DS = DH/T Eqn. 13
Whereas, enthalpy is a term whose value is
largely dependent upon electronic internal energies, entropy values are
dependent upon translational, vibrational and rotational internal
energies. Entropy also differs from enthalpy in that the values of
enthalpy that indicate favored reactions are negative and the values of
entropy are positive. Together the terms enthalpy and entropy demonstrate
that a system tends toward the highest entropy and the lowest enthalpy.
DG = DH - TDS Eqn. 14 Free energy is a valuable concept because it allows one to determine whether a reaction will proceed and allows one to calculate the equilibrium constant of the reaction which defines the extent to which a reaction can proceed. The discussion above indicated that a decrease in energy, a negative DH, and an increase in entropy, a positive DS, are indicative of favorable reactions. These terms would, therefore, make DG a negative value. Reactions with negative DG values are termed exergonic and those with positive DG values endergonic. However, when a system is at equilibrium: DG = 0 Eqn. 15 Gibb's free energy calculations allow one to determine whether a given reaction will be thermodynamically favorable. The sign of DG states that a reaction as written or its reverse process is the favorable step. If DG is negative then the forward reaction is favored and visa versa for DG values that are calculated to be positive.
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