Entropy
Spontaneous vs. Non-Spontaneous Processes
- Thermodynamics deals with spontaneous and non-spontaneous changes.
- Spontaneous processes occur naturally (e.g., a skier going downhill).
- Non-spontaneous processes require external intervention (e.g., a skier going uphill without assistance).
- Examples of spontaneous processes:
- Diffusion of a gas.
- Flow of heat from hot to cold.
- Marbles thrown in the air spreading apart.
- Heating a liquid until it boils.
- Reverse processes are non-spontaneous (marbles reforming into a package, heat flowing from cold to hot).
- Dynamite pieces will never reform into the original stick after explosion.
Entropy (S)
- Spontaneous processes are accompanied by an increase in the disorder of the universe, which is entropy.
- Entropy is represented by the capital letter S, indicating it's a state function.
- Entropy is a measure of disorder.
- Example: Dynamite stick is more ordered than its fragmented pieces after explosion.
- Living organisms are highly ordered, but nature tends to increase disorder (entropy) in the universe.
Processes with Decreasing Entropy
- Condensation: Gas to liquid conversion decreases entropy (decrease in disorder).
- Other examples: crystallization, precipitation, freezing.
- Relating entropy directly to spontaneity is complex.
Entropy and States of Matter
- Entropy of a solid < entropy of a liquid << entropy of a gas.
- Gases have the highest disorder and kinetic energy.
- Solids and liquids are condensed phases.
Units and Absolute Entropy Values
- Entropy is a thermodynamic quantity measured in joules per Kelvin mole ( J/K⋅mol ).
- Enthalpic contributions to energy changes are generally larger than entropic contributions (by about three orders of magnitude).
- Unlike enthalpy (ΔH) values, entropy values are absolute and positive, according to the third law of thermodynamics.
- The standard state for gases is one atmosphere, but for thermodynamics, the standard state is 25 degrees Celsius.
Third Law of Thermodynamics
- Classical physics: At 0 Kelvin, a perfect crystalline solid with no molecular motion has zero entropy.
- All other entropy values are relative to this benchmark.
- Quantum mechanics suggests that complete cessation of molecular motion is impossible due to the Heisenberg uncertainty principle.
Statistical Nature of Entropy
- Statistical mechanics: Highest entropy corresponds to the system with the most microstates (individual statistical states).
- Example: Gas molecules in a container with a valve separating an empty side. Opening the valve leads to diffusion and an increase in entropy.
- Although uniform gas distribution may seem more ordered, each gas molecule has more available locations (microstates), making it more disordered.
- Entropy drives processes like gas laws, heat flow, and diffusion.
- Molecules on the hot side have higher kinetic energy; heat flow to the cold side increases microstates for every molecule.
Entropy Diagram
- Processes increasing entropy:
- Solid melting to liquid.
- Liquid boiling/evaporating to vapor.
- Dissolving a compound in a solvent to form a solution.
- Heating a system (T1 to T2) increases kinetic energy and microstates (even in solids, promoting molecular vibration/rotation).
Entropy Change in Chemical Reactions
- ΔS<em>reaction=S</em>products−Sreactants
- \Delta S > 0 if the moles of gas increase.
- \Delta S < 0 if the moles of gas decrease.
- ΔS is negligible if there's no net change in gas molecules.
- Gases being evolved or consumed significantly affect ΔS.
Precipitation Reaction Exception
- Precipitation reactions often show \Delta S < 0 (products more ordered than reactants).
- Example: Silver ions reacting with chloride ions to form silver chloride precipitate.
- Despite decreasing entropy, these reactions can be spontaneous.
Example Problems: Predicting the Sign of ΔS
- General rule: Compare gas moles on reactant vs. product sides, except for precipitation.
- A superscripted zero means ΔS is at standard conditions.
Example 1
- N<em>2(g)+2H</em>2(g)→NH3(g)
- 3 moles of gas become 1 mole: \Delta S < 0
Example 2
- 2CO(g)+O<em>2(g)→2CO</em>2(g)
- 2 moles of gas going to 2 moles of gas: ΔS≈0
Example 3
- 2N<em>2O</em>5(g)→4NO<em>2(g)+O</em>2(g)
- 5 moles of gas become 6 moles: \Delta S > 0
Example 4
- C(s)+O<em>2(g)→CO</em>2(g)
- 1 mole of gas yields 2 moles: \Delta S > 0
Example 5
- Ag+(aq)+Cl−(aq)→AgCl(s)
- Precipitation reaction: \Delta S < 0
More Examples
- Two-chamber experiment: gas molecules distributed evenly has higher entropy. \Delta S < 0. Unfavorable process
- Salt dissolving: reverse precipitation, \Delta S > 0, favorable process
- Gas reactants to liquid products: \Delta S < 0, not favorable
Calculating Delta S for Chemical Reactions
- If absolute entropy values are known:
- ΔS<em>reaction=∑S</em>products−∑Sreactants
- ΔS Formula for a Reaction:
- For aA+bB→cC+dD
- ΔS=[c⋅S(C)+d⋅S(D)]−[a⋅S(A)+b⋅S(B)]
- Standard conditions: one atmosphere, 25 degrees Celsius.
Example: Calculate Delta S
- Reaction: CH<em>4(g)+2O</em>2(g)→CO<em>2(g)+2H</em>2O(l)
- Using Appendix III, look up entropy values for each compound (all positive due to the third law).
- ΔS=[1⋅S(CO<em>2)+2⋅S(H</em>2O)]−[1⋅S(CH<em>4)+2⋅S(O</em>2)]
- ΔS=[1⋅(213.6)+2⋅(69.9)]−[1⋅(186.3)+2⋅(205.0)]=−242.8KJ
Spontaneity and Entropy Contradiction
- Statements: Entropy must increase for spontaneous processes, yet many spontaneous processes have decreasing entropy.
- Examples: Freezing, condensation, crystallization.
- The second law of thermodynamics resolves this. In the next video.