Entropy, Entropy Changes, and Gibbs Free Energy Study Notes
Entropy and Energy Dispersal
Entropic factors: energy dispersal reduces the likelihood that energy flows drive changes in the system; more dispersed energy → greater thermodynamic stability.
Energy is dispersed over sub-microscopic particle motions: translations, rotations, vibrations.
As the number of particles increases and interactions diversify, energy can be dispersed across more pathways.
Entropy (S) and Standard Molar Entropy (S°)
Entropy describes the extent to which energy can be dispersed across the sub-microscopic particles of a system.
Standard molar entropy S° for a substance represents the energy-dispersal extent in one mole of substance at 25°C (298 K) and 1 bar.
Units: S°\text{ (units)} = \mathrm{J\,mol^{-1}\,K^{-1}}
Standard state definitions (examples):
1 M solution
1 bar gas
liquid
pure liquid
solid
pure solid element
most stable allotrope at 1 bar and 25°C (e.g., \mathrm{O2(g)} is more stable than \mathrm{O(g)} or \mathrm{O3(g)})
Change in Entropy for Reactions
The change in entropy for a reaction (∆rS°) can be calculated from tabulated standard molar entropies:
\Deltar S^{\circ} = \left(\sumi ni^{\text{products}} Si^{\circ}\right) - \left(\sumj nj^{\text{reactants}} S_j^{\circ}\right)Like enthalpy, ∆rS° is obtained by summing product S° values minus reactant S° values using stoichiometric coefficients.
Third Law of Thermodynamics
A perfect crystal of a pure substance at 0 K has zero entropy: S = 0\quad \text{at } T = 0\ \text{K}
Entropy values are measured relative to a perfect crystal at 0 K.
Predicting Entropy: Largest Entropy and Trends
Which substance has the largest entropy? (given S° values)
A. \mathrm{H_2O(s)}
B. \mathrm{H_2O(l)}
C. \mathrm{H_2O(g)}
Given: S^{\circ}(\mathrm{H2O(s)}) = 41.0\ \mathrm{J\,mol^{-1}\,K^{-1}}, S^{\circ}(\mathrm{H2O(l)}) = 70.0\ \mathrm{J\,mol^{-1}\,K^{-1}}, S^{\circ}(\mathrm{H_2O(g)}) = 188.8\ \mathrm{J\,mol^{-1}\,K^{-1}}
Entropy increases with increasing temperature and with phase changes solid → liquid → gas.
Example data:
Gas phase generally has higher S° than liquid; liquid higher than solid.
Trends with mass and complexity: atoms/molecules with greater mass and more complex structures tend to have higher entropies.
Example trends (molar mass vs S°):
He(g): M\approx 4\ \mathrm{g\,mol^{-1}},\ S^{\circ}=126\ \mathrm{J\,mol^{-1}\,K^{-1}}
Ne(g): M\approx 20\ \mathrm{g\,mol^{-1}},\ S^{\circ}=146.2\ \mathrm{J\,mol^{-1}\,K^{-1}}
Ar(g): M\approx 40\ \mathrm{g\,mol^{-1}},\ S^{\circ}=154.8\ \mathrm{J\,mol^{-1}\,K^{-1}}
Kr(g): M\approx 84\ \mathrm{g\,mol^{-1}},\ S^{\circ}=164.0\ \mathrm{J\,mol^{-1}\,K^{-1}}
C3H8(g): M\approx 44\ \mathrm{g\,mol^{-1}},\ S^{\circ}=269.9\ \mathrm{J\,mol^{-1}\,K^{-1}}
C6H14(g): M\approx 86\ \mathrm{g\,mol^{-1}},\ S^{\circ}=388.82\ \mathrm{J\,mol^{-1}\,K^{-1}}
Takeaway: Greater mass, greater molecular complexity → higher entropy.
Entropy Changes in Chemical Reactions
Entropy changes can be predicted for reactions using changes in moles of gas and phase changes:
Example: 6 moles of gas on the reactant side vs 7 moles on the product side increases disorder.
Reaction example (gas): \mathrm{C3H8(g) + 5\,O2(g) \rightarrow 3\,CO2(g) + 4\,H_2O(g)}
Example (aqueous+solid): \mathrm{AgNO3(aq) + NaCl(aq) \rightarrow NaNO3(aq) + AgCl(s)}
Predicting positive ΔS°: certain reactions increase gas-phase moles or produce more dispersed species.
Positive ΔS° Reactions (Practice Question)
Which reactions would have a positive change in entropy, ΔrS°?
1) \mathrm{CaCO3(s) + 2\,HCl(aq) \rightarrow CaCl2(aq) + CO2(g) + H2O(l)}
2) \mathrm{2\ NO(g) + O2(g) \rightarrow 2\ NO2(g)}
3) \mathrm{2\ KClO3(s) \rightarrow 2\ KCl(s) + 3\ O2(g)}Answer: 1 and 3 (increase in gas moles or production of gas from solids). (Reason: 2 decreases gas moles; 1 and 3 increase disorder by producing gas or increasing gas-phase species.)
Spontaneity, Equilibrium, and the Reaction Quotient
Spontaneous vs. nonspontaneous: a process is spontaneous if its composition evolves toward equilibrium (lower free energy) without external driving forces.
A process can be spontaneous or nonspontaneous depending on conditions (e.g., temperature, pressure).
Example concept: K < 1 implies reactant-favored equilibrium.
A numeric example: K = 0.0313; for a given reaction, Q can be compared to K to assess spontaneity.
At Q = 1 (standard state), the standard Gibbs free energy change ΔrG° is defined and relates to K (see below).
Standard state reference: 0 atm vs 1 bar; 1 M solutions; these standards set the baseline for ΔrG°, ΔrG°, and K.
Gibbs Free Energy and Spontaneity
Gibbs free energy is at a minimum at equilibrium.
On a plot of Gibbs free energy G versus composition (Q), ΔrG is the slope of the curve at that Q:
\Delta_r G = \text{(slope of G vs Q at that composition)}For a given reaction, if ΔrG is positive, the system evolves to increase reactants; if negative, it evolves to increase products. In either case, G decreases as equilibrium is approached.
Example interpretation: If the forward process is condensation of water (liquid to solid, etc.), ΔrG is positive; if evaporation (liquid to gas) is favored, ΔrG is negative.
At equilibrium, ΔrG = 0.
Relating ΔrG to Enthalpy and Entropy
The relationship between ΔrG, ΔrH, and ΔrS:
\Deltar G = \Deltar H - T\Delta_r SΔrG° and the equilibrium constant K are related by:
\Delta_r G^{\circ} = -RT\ln KΔrG° is typically tabulated for standard composition (Q = 1).
Units: ΔrH° in kJ/mol; ΔrS° in J/mol·K; ΔrG° and ΔrG are in kJ/mol (consistent with R and T units in J, K).
For any composition, the Gibbs energy is given by:
\Deltar G = \Deltar G^{\circ} + RT\ln QWhere:
R = 8.3145\ \mathrm{J\,mol^{-1}\,K^{-1}}
T in kelvin, Q is the reaction quotient.
Standard State and Vaporization Example (Water)
When Q = 1 for the process \mathrm{H2O(l) \rightleftharpoons H2O(g)} (at 298 K):
The slide lists: \Delta_r G^{\circ} = 8.59\ \mathrm{kJ\,mol^{-1}}
This implies the forward process (liquid → gas) has a positive ΔrG° at standard state, so the reverse process (gas → liquid, condensation) would be favored at standard state.
Note: Real values for water vaporization give a ΔG° that is positive at 298 K, reflecting non-spontaneity of vaporization at room temperature; the exact value can depend on the data source and reference state.
Another slide repeats: at 298 K, for the same process, ΔrG° ≈ +8.59 kJ/mol and Q = P_H2O, with the interpretation that the forward process has positive ΔrG°.
ΔrG° and Temperature/Composition (Q) Examples
When Q = 5.00 × 10^−3 (298 K) for the liquid↔gas water process, ΔrG° is still given as 8.59 kJ/mol in the slide, and ΔrG is determined by including RT ln Q:
\Deltar G = \Deltar G^{\circ} + RT\ln QWhen Q = 0.0313 (298 K) for the same process, ΔrG° remains 8.59 kJ/mol; ΔrG depends on Q, demonstrating how nonstandard composition shifts spontaneity.
Key point: ΔrG° relates to K via \Delta_r G^{\circ} = -RT\ln K\,.
Spontaneity and Temperature Dependence
Spontaneity can depend on temperature. A process may be spontaneous at one temperature and not at another.
Visual note (conceptual): some processes are spontaneous for T > 0 °C and others for T < 0 °C depending on the balance between enthalpy and entropy contributions.
Practical implication: cooling a hot substance, gas expansion into a vacuum, or phase changes can shift spontaneity with temperature.
Real-World and Conceptual Examples of Spontaneity
Spontaneous for T > 0 °C vs spontaneous for T < 0 °C: temperature can flip whether a process is spontaneous.
Coffee cooling down: generally spontaneous (exothermic flow of heat to surroundings with increasing entropy of the surroundings).
Expansion of a gas into a vacuum: spontaneous (increase in entropy due to more available microstates).
Melting of ice: spontaneous above 0 °C, non-spontaneous below 0 °C; depends on temperature relative to the phase boundary.
Gibbs Free Energy Minima and Equilibrium Slopes
At equilibrium, Gibbs free energy is at its minimum with respect to composition.
The slope of the G vs composition curve at a given Q equals ΔrG for the reaction: a direct link between thermodynamics and reaction progress.
For a process like H2O(l) ⇄ H2O(g) at a given T, the sign of ΔrG indicates whether the system moves toward more liquid (positive ΔrG would favor reactants) or more gas (negative ΔrG would favor products).
A representative value on the slide: ΔrG = 2.85 kJ mol^−1 at a specified Q, illustrating a nonzero driving force away from equilibrium.
Standard vs General Formulations and Units
ΔrG° is commonly tabulated for the standard composition (Q = 1) and relates to K via \Delta_r G^{\circ} = -RT\ln K.
For any composition (Q ≠ 1), the general relation is \Deltar G = \Deltar G^{\circ} + RT\ln Q.
Remember: to compare to standard states, ensure units are consistent: ΔH° in kJ/mol and ΔS° in J/mol·K, so ΔG° will be in kJ/mol when using R in J·mol^−1·K^−1 with T in K.
Quick Concept Checks and Reminders
Spontaneous does not imply fast: a reaction can be thermodynamically spontaneous but kinetically slow.
The standard composition (Q = 1) provides a baseline reference point for comparing spontaneity under standard conditions.
The concept of energy dispersal (entropy) works together with enthalpy to determine spontaneity via ΔG.
Homework and Study Reminders (From the Transcript)
By Saturday, 9/20 at 8:30 AM: Complete and Upload Week 3 Discussion packet (topics you worked on this week).
By Monday, 9/22 at 8:30 AM: Complete and Upload Homework 5-5; will review in class Tuesday.
Notes on Data and References from the Transcript
Standard molar entropy (S°) and its units: \text{S° (J mol^{-1} K^{-1})}
Example S° values (for illustration):
\mathrm{H_2O(s)\;:\;S^{\circ}=41.0}
\mathrm{H_2O(l)\;:\;S^{\circ}=70.0}
\mathrm{H_2O(g)\;:\;S^{\circ}=188.8}
Example data for noble gases and small molecules (S° values in J/mol·K):
He(g): 126
Ne(g): 146.2
Ar(g): 154.8
Kr(g): 164.0
C3H8(g): 269.9
C6H14(g): 388.82
Example reactions cited:
Gas-producing combustion/oxidation example: \mathrm{C3H8(g) + 5 O2(g) \rightarrow 3 CO2(g) + 4 H_2O(g)}
Aqueous + solid formation: \mathrm{AgNO3(aq) + NaCl(aq) \rightarrow NaNO3(aq) + AgCl(s)}$$
Final Remarks
Entropy captures how energy becomes distributed among many microstates; Gibbs free energy combines entropy with enthalpy to determine spontaneity and equilibrium.
Always relate ΔrG to K (thermodynamic equilibrium) and Q (current composition) to decide whether a process will proceed toward products or reactants under given conditions.