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CHAPTER 14 Thermodynamics: Spontaneous Processes, , and Free

A tiny fraction of the 's energy is used to produce complicated, ordered, high- Useful energy is being "degraded" in energy systems such as life the form of unusable , light, etc.

• Our observation is that natural processes proceed from ordered, high-energy systems to disordered, lower energy states. • In addition, once the energy has been "degraded", it is no longer available to perform useful work. • It may not appear to be so locally (earth), but globally it is true (sun, universe as a whole).

1 Thermodynamics - quantitative description of the factors that drive chemical reactions, i.e. temperature, , entropy, free energy.

Answers questions such as-

• will two or more substances react when they are mixed under specified conditions? • if a reaction occurs, what energy changes are associated with it? • to what extent does a reaction occur to?

Thermodynamics does NOT tell us the RATE of a reaction

Spontaneous Processes A spontaneous process is one that is capable of proceeding in a given direction without an external driving force • A waterfall runs downhill • A lump of sugar dissolves in a cup of coffee • At 1 atm, water freezes below 0 0C and ice melts above 0 0C • Heat flows from a hotter object to a colder object • A expands in an evacuated bulb • Iron exposed to oxygen and water forms rust

2 Spontaneous chemical and physical changes are frequently accompanied by a release of heat (exothermic H < 0) -

o C3H8(g) + 5 O2(g)  3 CO2(g) + 4 H2O(l) H = -2200 kJ

Although many spontaneous processes are exothermic (e.g., the previous combustion reaction), not true for all spontaneous reactions:

Endothermic (ΔH > 0), but reaction is spontaneous.

3 Some processes are accompanied by no change in enthalpy at all (Ho = 0.0), as is the case for an ideal gas spontaneously expanding:

spontaneous

nonspontaneous

There's another factor promoting spontaneity in these processes, and that's the increasing randomness or disorder of the system:

1. propane combustion:

o C3H8(g) + 5 O2(g)  3 CO2(g) + 4 H2O(l) H = -2200 kJ

2. water : o H2O(s)  H2O(l) H = 6.01 kJ

3. gas expansion:

4 Thermodynamics: Entropy

. Second Law of Thermodynamics: • The total entropy of the universe increases in any spontaneous process . Entropy (S): • A measure of the amount of disorder (qualitative), or unusable energy in a system at a specific temperature (quantitative). • Entropy is affected by molecular motion, or disorder from volume changes (e.g. the previous gas expansion example).

Types of Molecular Motion

. Three types of motion: • Translational—movement through space. • Rotational—spinning motion around axis  to bond. • Vibrational—movement of toward/away from each other. . As temperature increases, the amount of motion increases.

5 Trends in

Ssolid < Sliquid < Sgas

Entropy is expected to INCREASE for these types of processes (S > 0) :

6 Changes in Entropy

order S disorder S

S = Sf - Si

S > 0

S < 0

Suniverse

Example - Predict whether the entropy change is greater than or less than zero for each of the following processes:

(a) freezing ethanol (b) evaporating a beaker of liquid bromine at room temperature (c) dissolving sucrose in water (d) cooling nitrogen gas from 80 oC to 20 oC.

7 Entropy Changes in the System (Ssys) 0 The standard entropy of reaction (Srxn ) is the entropy change for a reaction carried out at 1 atm and 250C.

aA + bB cC + dD from Appendix

0 0 0 0 0 Srxn = [c S (C) + dS (D) ] - [a S (A) + bS (B) ]

0 0 0 Srxn = S nS (products) - S mS (reactants)

The Second Law of Thermodynamics: The total entropy of the universe increases in any spontaneous process

Spontaneous process: Suniv = Ssys + Ssurr > 0

sys = system One can be negative but the surr = surroundings other will be even more positive

Equilibrium process: Suniv = Ssys + Ssurr = 0

At equilibrium the forward and reverse rates are equal, e.g vapor pressure

(l) = (g) So there is no net change in entropy

8 Entropy Changes in the Surroundings (Ssurr)

Exothermic Process Endothermic Process

Ssurr > 0 Ssurr < 0

The change in entropy of the surroundings can be calculated:

if Hsys < 0 (exothermic), then Ssurr > 0 (entropy of the surroundings increases) Ssurr  -Hsys if Hsys > 0 (endothermic), then Ssurr < 0 (entropy of the surroundings decreases)

If the temperature of the surroundings is already high, Ssurr  1 then pumping heat in or out Tsurr causes less change in disorder than at lower temperatures

9 Combining the two:

Ssurr  -Hsys and Ssurr  1 so Ssurr = -Hsys Tsurr T

(Tsurr usually = Tsys)

e.g. N2(g) + 3H2(g)  2NH3(g) Ssys = -198.3 J/K * Hsys = -92.6 kJ The two main driving forces are in opposition to each other - the release of heat favors a spontaneous reaction while the

decrease in entropy does not. Calculating Suniv will decide the issue (next slide). Remember: for a spontaneous reaction the entropy of the universe increases.

0 0 0 *from Ch 5: Hrxn = S nH f (products) - S mHf (reactants)

Is the reaction spontaneous at 25 oC?

Suniv = Ssys + Ssurr

10 The previous example with ammonia illustrated that maybe entropy will decrease in the system, but this will always be accompanied by a greater increase in

the entropy of the surroundings such that Suniv > 0.

Suniv = Ssys + Ssurr > 0

Another way of stating the 2nd Law is that "You Can't Win!"

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