Spontaneity Entropy and Free Energy Spontaneous Processes and

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Spontaneity, Entropy and Free Energy

Spontaneity, Entropy and Free Energy

Spontaneous Processes and Entropy q. First Law • “Energy can neither be created nor

Spontaneous Processes and Entropy q. First Law • “Energy can neither be created nor destroyed" • The energy of the universe is constant q. Spontaneous Processes • Processes that occur without outside intervention • Spontaneous processes may be fast or slow – Many forms of combustion are fast – Conversion of diamond to graphite is slow

Entropy (S) Ø A measure of the randomness or disorder Ø The driving force

Entropy (S) Ø A measure of the randomness or disorder Ø The driving force for a spontaneous process is an increase in the entropy of the universe Ø Entropy is a thermodynamic function describing the number of arrangements that are available to a system Ø Nature proceeds toward the states that have the highest probabilities of existing

Positional Entropy § The probability of occurrence of a particular state depends on the

Positional Entropy § The probability of occurrence of a particular state depends on the number of ways (microstates) in which that arrangement can be achieved Ssolid < Sliquid << Sgas

Second Law of Thermodynamics § § § "In any spontaneous process there is always

Second Law of Thermodynamics § § § "In any spontaneous process there is always an increase in the entropy of the universe" "The entropy of the universe is increasing" For a given change to be spontaneous, Suniverse must be positive Suniv = Ssys + Ssurr

 H, S, G and Spontaneity G = H - T S H is

H, S, G and Spontaneity G = H - T S H is enthalpy, T is Kelvin temperature Value of H Value of T S Value of Spontaneity G Negative Positive Negative Spontaneous Negative Positive Nonspontaneous Negative ? ? ? Spontaneous if the absolute value of H is greater than the absolute value of T S (low temperature) Positive ? ? ? Spontaneous if the absolute value of T S is greater than the absolute value of H (high temperature)

Calculating Entropy Change in a Reaction v Entropy is an extensive property (a function

Calculating Entropy Change in a Reaction v Entropy is an extensive property (a function of the number of moles) v Generally, the more complex the molecule, the higher the standard entropy value

Standard Free Energy Change v G 0 is the change in free energy that

Standard Free Energy Change v G 0 is the change in free energy that will occur if the reactants in their standard states are converted to the products in their standard states v G 0 cannot be measured directly v The more negative the value for G 0, the farther to the right the reaction will proceed in order to achieve equilibrium v Equilibrium is the lowest possible free energy position for a reaction

Calculating Free Energy Method #1 For reactions at constant temperature: 0 G = 0

Calculating Free Energy Method #1 For reactions at constant temperature: 0 G = 0 H - 0 T S

Calculating Free Energy: Method #2 An adaptation of Hess's Law: Cdiamond(s) + O 2(g)

Calculating Free Energy: Method #2 An adaptation of Hess's Law: Cdiamond(s) + O 2(g) CO 2(g) G 0 = -397 k. J Cgraphite(s) + O 2(g) CO 2(g) G 0 = -394 k. J Cdiamond(s) + O 2(g) CO 2(g) G 0 = -397 k. J CO 2(g) Cgraphite(s) + O 2(g) G 0 = +394 k. J Cdiamond(s) Cgraphite(s) G 0 = -3 k. J

Calculating Free Energy Method #3 Using standard free energy of formation ( Gf 0):

Calculating Free Energy Method #3 Using standard free energy of formation ( Gf 0): Gf 0 of an element in its standard state is zero

The Dependence of Free Energy on Pressure q Enthalpy, H, is not pressure dependent

The Dependence of Free Energy on Pressure q Enthalpy, H, is not pressure dependent q Entropy, S Ø entropy depends on volume, so it also depends on pressure Slarge volume > Ssmall volume Slow pressure > Shigh pressure

Free Energy and Equilibrium q Equilibrium point occurs at the lowest value of free

Free Energy and Equilibrium q Equilibrium point occurs at the lowest value of free energy available to the reaction system q At equilibrium, G = 0 and Q = K G 0 = 0 G 0 < 0 G 0 > 0 K K = 1 K > 1 K < 1

Temperature Dependence of K So, ln(K) 1/T

Temperature Dependence of K So, ln(K) 1/T

Free Energy and Work q The maximum possible useful work obtainable from a process

Free Energy and Work q The maximum possible useful work obtainable from a process at constant temperature and pressure is equal to the change in free energy q The amount of work obtained is always less than the maximum q Henry Bent's First Two Laws of Thermodynamics q First law: You can't win, you can only break even q Second law: You can't break even