๐ŸŽฏโญ INTERACTIVE LESSON

Gibbs Free Energy and Spontaneity

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Gibbs Free Energy and Spontaneity - Complete Interactive Lesson

Part 1: Introduction to Gibbs Free Energy

โšก Gibbs Free Energy and Spontaneity

Part 1 of 7 โ€” ฮ”G = ฮ”H โˆ’ Tฮ”S

Gibbs Free Energy (GG) is the single most important thermodynamic quantity for chemists. It combines enthalpy and entropy into one number that tells you whether a reaction is spontaneous โ€” without needing to calculate the entropy of the surroundings.

Defining Gibbs Free Energy

G=Hโˆ’TSG = H - TS

The change in Gibbs free energy at constant temperature:

ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta S

Where Does This Come From?

Recall: ฮ”Suniverse=ฮ”Ssystem+ฮ”Ssurroundings\Delta S_{\text{universe}} = \Delta S_{\text{system}} + \Delta S_{\text{surroundings}}

And: ฮ”Ssurroundings=โˆ’ฮ”Hsystem/T\Delta S_{\text{surroundings}} = -\Delta H_{\text{system}}/T

So: ฮ”Suniverse=ฮ”Ssysโˆ’ฮ”Hsys/T\Delta S_{\text{universe}} = \Delta S_{\text{sys}} - \Delta H_{\text{sys}}/T

Multiply by โˆ’T-T:

โˆ’Tฮ”Suniverse=ฮ”Hsysโˆ’Tฮ”Ssys=ฮ”G-T\Delta S_{\text{universe}} = \Delta H_{\text{sys}} - T\Delta S_{\text{sys}} = \Delta G

Since ฮ”Suniverse>0\Delta S_{\text{universe}} > 0 for spontaneous processes:

ฮ”G<0(spontaneous)\Delta G < 0 \quad \text{(spontaneous)}

The Spontaneity Criterion

ฮ”G\Delta GMeaning
ฮ”G<0\Delta G < 0Spontaneous (thermodynamically favorable)
ฮ”G=0\Delta G = 0At equilibrium
ฮ”G>0\Delta G > 0Nonspontaneous (reverse reaction is spontaneous)

Why Gibbs Free Energy Is So Useful

  • It accounts for both enthalpy and entropy
  • It is a property of the system only โ€” no need to calculate ฮ”Ssurroundings\Delta S_{\text{surroundings}}
  • It connects directly to equilibrium and electrochemistry

What "Free" Means

"Free energy" is the maximum amount of energy available to do useful work (non-PVPV work) in a reaction.

wmax=ฮ”Gw_{\text{max}} = \Delta G

If ฮ”G=โˆ’100\Delta G = -100 kJ, the reaction can do at most 100 kJ of useful work.

Temperature and Spontaneity

From ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta S, we see that temperature affects spontaneity through the Tฮ”ST\Delta S term:

  • At low temperatures: ฮ”H\Delta H dominates (Tฮ”ST\Delta S is small)
  • At high temperatures: Tฮ”ST\Delta S dominates (Tฮ”ST\Delta S is large)

The Crossover Temperature

When ฮ”G=0\Delta G = 0 (equilibrium):

T=ฮ”Hฮ”ST = \frac{\Delta H}{\Delta S}

This is the temperature at which the reaction switches between spontaneous and nonspontaneous.

Example

For ice melting: ฮ”H=+6.01\Delta H = +6.01 kJ/mol, ฮ”S=+22.0\Delta S = +22.0 J/(molยทK)

T=601022.0=273ย K=0ยฐCT = \frac{6010}{22.0} = 273 \text{ K} = 0ยฐ\text{C}

Above 273 K: melting is spontaneous (ฮ”G<0\Delta G < 0). Below 273 K: freezing is spontaneous.

Gibbs Free Energy Concept Quiz ๐ŸŽฏ

Gibbs Free Energy Calculations ๐Ÿงฎ

  1. ฮ”H=โˆ’100\Delta H = -100 kJ, ฮ”S=+50\Delta S = +50 J/K, T=298T = 298 K. Calculate ฮ”G\Delta G in kJ. (to 3 significant figures)

  2. ฮ”H=+200\Delta H = +200 kJ, ฮ”S=+500\Delta S = +500 J/K, T=500T = 500 K. Calculate ฮ”G\Delta G in kJ.

  3. A reaction has ฮ”H=+30\Delta H = +30 kJ and ฮ”S=+100\Delta S = +100 J/K. At what temperature (in K) is ฮ”G=0\Delta G = 0?

Gibbs Free Energy Concepts ๐Ÿ”ฝ

Exit Quiz โ€” Gibbs Free Energy โœ…

Part 2: ฮ”G = ฮ”H โˆ’ Tฮ”S

๐Ÿ”€ Four ฮ”H/ฮ”S Combinations

Part 2 of 7 โ€” Always, Never, or Temperature-Dependent

The equation ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta S has four possible sign combinations for ฮ”H\Delta H and ฮ”S\Delta S. Understanding these four cases is essential for AP Chemistry and lets you quickly assess spontaneity.

The Four Cases

Case 1: ฮ”H < 0, ฮ”S > 0 โ€” Always Spontaneous โœ…

ฮ”G=(negative)โˆ’T(positive)=alwaysย negative\Delta G = (\text{negative}) - T(\text{positive}) = \text{always negative}

  • Both terms favor spontaneity
  • Spontaneous at all temperatures
  • Example: combustion of hydrocarbons

Case 2: ฮ”H > 0, ฮ”S < 0 โ€” Never Spontaneous โŒ

ฮ”G=(positive)โˆ’T(negative)=alwaysย positive\Delta G = (\text{positive}) - T(\text{negative}) = \text{always positive}

  • Both terms oppose spontaneity
  • Never spontaneous (the reverse reaction is always spontaneous)
  • Example: the reverse of combustion

Case 3: ฮ”H < 0, ฮ”S < 0 โ€” Spontaneous at Low T ๐Ÿฅถ

ฮ”G=(negative)โˆ’T(negative)\Delta G = (\text{negative}) - T(\text{negative})

  • Exothermic but entropy-decreasing
  • At low T: โˆฃฮ”Hโˆฃ>โˆฃTฮ”Sโˆฃ|\Delta H| > |T\Delta S| โ†’ ฮ”G<0\Delta G < 0
  • At high T: โˆฃTฮ”Sโˆฃ>โˆฃฮ”Hโˆฃ|T\Delta S| > |\Delta H| โ†’ ฮ”G>0\Delta G > 0
  • Example: freezing of water

Case 4: ฮ”H > 0, ฮ”S > 0 โ€” Spontaneous at High T ๐Ÿ”ฅ

ฮ”G=(positive)โˆ’T(positive)\Delta G = (\text{positive}) - T(\text{positive})

  • Endothermic but entropy-increasing
  • At high T: โˆฃTฮ”Sโˆฃ>โˆฃฮ”Hโˆฃ|T\Delta S| > |\Delta H| โ†’ ฮ”G<0\Delta G < 0
  • At low T: โˆฃฮ”Hโˆฃ>โˆฃTฮ”Sโˆฃ|\Delta H| > |T\Delta S| โ†’ ฮ”G>0\Delta G > 0
  • Example: melting of ice, vaporization

Summary Table

ฮ”H\Delta Hฮ”S\Delta Sฮ”G\Delta GSpontaneous?
โˆ’+Always โˆ’Always โœ…
+โˆ’Always +Never โŒ
โˆ’โˆ’โˆ’ at low T, + at high TLow T only ๐Ÿฅถ
+++ at low T, โˆ’ at high THigh T only ๐Ÿ”ฅ

The Crossover Temperature

For Cases 3 and 4, the temperature where ฮ”G=0\Delta G = 0:

Tcrossover=ฮ”Hฮ”ST_{\text{crossover}} = \frac{\Delta H}{\Delta S}

(Both ฮ”H\Delta H and ฮ”S\Delta S must have the same sign for this temperature to be positive and physically meaningful.)

Real-World Examples

Case 1 (Always Spontaneous): Combustion

CH4(g)+2O2(g)โ†’CO2(g)+2H2O(g)\text{CH}_4(g) + 2\text{O}_2(g) \rightarrow \text{CO}_2(g) + 2\text{H}_2\text{O}(g)

  • ฮ”H<0\Delta H < 0 (releases heat)
  • ฮ”S>0\Delta S > 0 (ฮ”ngas=3โˆ’3=0\Delta n_{\text{gas}} = 3 - 3 = 0, but products are more complex โ€” actually ฮ”S\Delta S can be slightly negative for this specific reaction at standard conditions)

Case 3 (Low T): Freezing Water

H2O(l)โ†’H2O(s)\text{H}_2\text{O}(l) \rightarrow \text{H}_2\text{O}(s)

  • ฮ”H<0\Delta H < 0 (releases heat โ€” exothermic)
  • ฮ”S<0\Delta S < 0 (liquid โ†’ solid, more ordered)
  • Spontaneous only below 273 K

Case 4 (High T): Melting Ice

H2O(s)โ†’H2O(l)\text{H}_2\text{O}(s) \rightarrow \text{H}_2\text{O}(l)

  • ฮ”H>0\Delta H > 0 (absorbs heat โ€” endothermic)
  • ฮ”S>0\Delta S > 0 (solid โ†’ liquid, more disordered)
  • Spontaneous only above 273 K

Four Cases Quiz ๐ŸŽฏ

Classify the Reaction ๐Ÿงฎ

For each combination, type "always", "never", "low T", or "high T" for when the reaction is spontaneous:

  1. ฮ”H<0\Delta H < 0, ฮ”S>0\Delta S > 0

  2. ฮ”H>0\Delta H > 0, ฮ”S>0\Delta S > 0

  3. ฮ”H>0\Delta H > 0, ฮ”S<0\Delta S < 0

Spontaneity and Temperature ๐Ÿ”ฝ

Exit Quiz โ€” Four Cases โœ…

Part 3: Spontaneity & Temperature

๐Ÿ—๏ธ Standard Free Energy of Formation

Part 3 of 7 โ€” Calculating ฮ”Gยฐ from Tables

Just as we used ฮ”Hยฐf\Delta Hยฐ_f to calculate ฮ”Hยฐrxn\Delta Hยฐ_{\text{rxn}}, we can use standard free energies of formation (ฮ”Gยฐf\Delta Gยฐ_f) to calculate ฮ”Gยฐrxn\Delta Gยฐ_{\text{rxn}}. The formula is identical in structure.

Standard Free Energy of Formation (ฮ”Gยฐf\Delta Gยฐ_f)

The free energy change when one mole of a compound is formed from its elements in their standard states at standard conditions.

The Master Equation

ฮ”Gยฐrxn=โˆ‘nโ‹…ฮ”Gยฐf(products)โˆ’โˆ‘mโ‹…ฮ”Gยฐf(reactants)\Delta Gยฐ_{\text{rxn}} = \sum n \cdot \Delta Gยฐ_f(\text{products}) - \sum m \cdot \Delta Gยฐ_f(\text{reactants})

Key Rule

ฮ”Gยฐf=0ย forย allย elementsย inย theirย standardย states\Delta Gยฐ_f = 0 \text{ for all elements in their standard states}

(Same convention as ฮ”Hยฐf\Delta Hยฐ_f)

Sample Values

Substanceฮ”Gยฐf\Delta Gยฐ_f (kJ/mol)
CO2(g)\text{CO}_2(g)โˆ’394.4-394.4
H2O(l)\text{H}_2\text{O}(l)โˆ’237.1-237.1
H2O(g)\text{H}_2\text{O}(g)โˆ’228.6-228.6
NH3(g)\text{NH}_3(g)โˆ’16.4-16.4
NO2(g)\text{NO}_2(g)+51.3+51.3
C2H6(g)\text{C}_2\text{H}_6(g)โˆ’32.0-32.0
O2(g)\text{O}_2(g)00
N2(g)\text{N}_2(g)00

Worked Example

Calculate ฮ”Gยฐ\Delta Gยฐ for: CH4(g)+2O2(g)โ†’CO2(g)+2H2O(l)\text{CH}_4(g) + 2\text{O}_2(g) \rightarrow \text{CO}_2(g) + 2\text{H}_2\text{O}(l)

Substanceฮ”Gยฐf\Delta Gยฐ_f (kJ/mol)
CH4(g)\text{CH}_4(g)โˆ’50.7-50.7
O2(g)\text{O}_2(g)00
CO2(g)\text{CO}_2(g)โˆ’394.4-394.4
H2O(l)\text{H}_2\text{O}(l)โˆ’237.1-237.1

ฮ”Gยฐ=[(โˆ’394.4)+2(โˆ’237.1)]โˆ’[(โˆ’50.7)+2(0)]\Delta Gยฐ = [(-394.4) + 2(-237.1)] - [(-50.7) + 2(0)] =[โˆ’394.4โˆ’474.2]โˆ’[โˆ’50.7]= [-394.4 - 474.2] - [-50.7] =โˆ’868.6+50.7=โˆ’817.9ย kJ= -868.6 + 50.7 = -817.9 \text{ kJ}

The large negative ฮ”Gยฐ\Delta Gยฐ confirms that combustion of methane is very spontaneous.

Two Methods to Calculate ฮ”Gยฐ

  1. From ฮ”Gยฐf\Delta Gยฐ_f values (this method) โ€” direct lookup
  2. From ฮ”Hยฐ\Delta Hยฐ and ฮ”Sยฐ\Delta Sยฐ: ฮ”Gยฐ=ฮ”Hยฐโˆ’Tฮ”Sยฐ\Delta Gยฐ = \Delta Hยฐ - T\Delta Sยฐ

Both methods give the same answer at 25ยฐC.

Standard Free Energy Quiz ๐ŸŽฏ

ฮ”Gยฐ Calculations ๐Ÿงฎ

Use these ฮ”Gยฐf\Delta Gยฐ_f values (kJ/mol): CO2(g)=โˆ’394.4\text{CO}_2(g) = -394.4, H2O(l)=โˆ’237.1\text{H}_2\text{O}(l) = -237.1, C2H6(g)=โˆ’32.0\text{C}_2\text{H}_6(g) = -32.0, O2(g)=0\text{O}_2(g) = 0

  1. Calculate ฮ”Gยฐ\Delta Gยฐ for: C2H6(g)+72O2(g)โ†’2CO2(g)+3H2O(l)\text{C}_2\text{H}_6(g) + \frac{7}{2}\text{O}_2(g) \rightarrow 2\text{CO}_2(g) + 3\text{H}_2\text{O}(l) (in kJ, to 1 decimal)

  2. Is this reaction spontaneous under standard conditions? (type "yes" or "no")

Round all answers to 3 significant figures.

Comparing the Three Formation Quantities

QuantitySymbolElementsUnitsWhat It Tells You
Formation enthalpyฮ”Hยฐf\Delta Hยฐ_f= 0kJ/molHeat flow
Standard entropySยฐSยฐโ‰  0 (positive!)J/(molยทK)Disorder
Formation free energyฮ”Gยฐf\Delta Gยฐ_f= 0kJ/molSpontaneity

Common AP Mistake

Students often confuse these three quantities. Remember:

  • ฮ”Hยฐf\Delta Hยฐ_f and ฮ”Gยฐf\Delta Gยฐ_f are zero for elements in standard states
  • SยฐSยฐ is NOT zero โ€” it is always positive at T>0T > 0 K

Formation Free Energy Concepts ๐Ÿ”ฝ

Exit Quiz โ€” Standard Free Energy โœ…

Part 4: Standard Free Energy of Formation

โš–๏ธ ฮ”G and Equilibrium

Part 4 of 7 โ€” ฮ”Gยฐ = โˆ’RT ln K

One of the most powerful relationships in all of chemistry connects Gibbs free energy to the equilibrium constant. This equation bridges thermodynamics and equilibrium โ€” two pillars of AP Chemistry.

The Key Equation

ฮ”Gยฐ=โˆ’RTlnโกK\Delta Gยฐ = -RT\ln K

SymbolMeaningValue/Units
ฮ”Gยฐ\Delta GยฐStandard free energy changeJ/mol (or kJ/mol)
RRGas constant8.3148.314 J/(molยทK)
TTTemperatureK
KKEquilibrium constantdimensionless

What This Equation Tells Us

If ฮ”Gยฐ\Delta GยฐThen KKMeaning
ฮ”Gยฐ<0\Delta Gยฐ < 0K>1K > 1Products favored at equilibrium
ฮ”Gยฐ=0\Delta Gยฐ = 0K=1K = 1Neither favored
ฮ”Gยฐ>0\Delta Gยฐ > 0K<1K < 1Reactants favored at equilibrium

Important Nuance

ฮ”Gยฐ<0\Delta Gยฐ < 0 does NOT mean the reaction goes to completion. It means K>1K > 1, so products are favored, but reactants are still present at equilibrium.

Solving for K from ฮ”Gยฐ

Rearranging: K=eโˆ’ฮ”Gยฐ/(RT)K = e^{-\Delta Gยฐ/(RT)}

Worked Example

Find KK at 25ยฐC for a reaction with ฮ”Gยฐ=โˆ’5.40\Delta Gยฐ = -5.40 kJ/mol.

K=eโˆ’ฮ”Gยฐ/(RT)=eโˆ’(โˆ’5400)/(8.314ร—298)K = e^{-\Delta Gยฐ/(RT)} = e^{-(-5400)/(8.314 \times 298)}

K=e5400/2477.6=e2.180=8.85K = e^{5400/2477.6} = e^{2.180} = 8.85

Solving for ฮ”Gยฐ from K

If K=1.0ร—1010K = 1.0 \times 10^{10} at 298 K:

ฮ”Gยฐ=โˆ’RTlnโกK=โˆ’(8.314)(298)lnโก(1.0ร—1010)\Delta Gยฐ = -RT\ln K = -(8.314)(298)\ln(1.0 \times 10^{10})

ฮ”Gยฐ=โˆ’(2477.6)(23.03)=โˆ’57,050ย J=โˆ’57.1ย kJ\Delta Gยฐ = -(2477.6)(23.03) = -57{,}050 \text{ J} = -57.1 \text{ kJ}

Converting Between ln and log

lnโกK=2.303logโกK\ln K = 2.303 \log K

So: ฮ”Gยฐ=โˆ’2.303RTlogโกK\Delta Gยฐ = -2.303 RT \log K

ฮ”Gยฐ and K Concept Quiz ๐ŸŽฏ

ฮ”Gยฐ and K Calculations ๐Ÿงฎ

Use R=8.314R = 8.314 J/(molยทK), T=298T = 298 K

  1. If ฮ”Gยฐ=โˆ’17.1\Delta Gยฐ = -17.1 kJ/mol, what is KK? (round to nearest whole number)

  2. If K=1.0ร—105K = 1.0 \times 10^{5} at 298 K, what is ฮ”Gยฐ\Delta Gยฐ? (in kJ/mol, to 1 decimal)

  3. If ฮ”Gยฐ=+10.0\Delta Gยฐ = +10.0 kJ/mol, is KK greater than or less than 1? (type "greater" or "less")

ฮ”Gยฐ and Equilibrium ๐Ÿ”ฝ

Exit Quiz โ€” ฮ”Gยฐ and K โœ…

Part 5: ฮ”G and Equilibrium

๐Ÿ“Š Non-Standard Conditions โ€” ฮ”G = ฮ”Gยฐ + RT ln Q

Part 5 of 7 โ€” Real-World Free Energy

ฮ”Gยฐ\Delta Gยฐ tells us about equilibrium, but real reactions rarely start at standard conditions. To determine spontaneity at any concentration, pressure, or composition, we need ฮ”G\Delta G (without the ยฐ), which uses the reaction quotient QQ.

The Non-Standard Free Energy Equation

ฮ”G=ฮ”Gยฐ+RTlnโกQ\Delta G = \Delta Gยฐ + RT\ln Q

SymbolMeaning
ฮ”G\Delta GFree energy change at current conditions
ฮ”Gยฐ\Delta GยฐFree energy change at standard conditions
RR8.314 J/(molยทK)
TTTemperature in K
QQReaction quotient (current concentrations)

Recall: Q vs K

  • QQ = reaction quotient (calculated from current concentrations)
  • KK = equilibrium constant (concentrations at equilibrium)

Q=[products]n[reactants]mQ = \frac{[\text{products}]^n}{[\text{reactants}]^m} (same form as K, but not at equilibrium)

Interpreting ฮ”G, Q, and K

ConditionQQ vs KKฮ”G\Delta GDirection
Q<KQ < KBelow equilibriumฮ”G<0\Delta G < 0Forward reaction spontaneous
Q=KQ = KAt equilibriumฮ”G=0\Delta G = 0No net change
Q>KQ > KAbove equilibriumฮ”G>0\Delta G > 0Reverse reaction spontaneous

Key Insight

At equilibrium, Q=KQ = K and ฮ”G=0\Delta G = 0:

0=ฮ”Gยฐ+RTlnโกK0 = \Delta Gยฐ + RT\ln K ฮ”Gยฐ=โˆ’RTlnโกK\Delta Gยฐ = -RT\ln K

This is how we derived the ฮ”Gยฐ\Delta Gยฐโ€“KK relationship!

The Big Picture

  • ฮ”Gยฐ\Delta Gยฐ tells you WHERE equilibrium lies (the value of KK)
  • ฮ”G\Delta G tells you WHICH DIRECTION the reaction will go from current conditions
  • A reaction with ฮ”Gยฐ>0\Delta Gยฐ > 0 can still proceed forward if QQ is small enough

Worked Example

For the reaction N2(g)+3H2(g)โ‡Œ2NH3(g)\text{N}_2(g) + 3\text{H}_2(g) \rightleftharpoons 2\text{NH}_3(g)

ฮ”Gยฐ=โˆ’33.0\Delta Gยฐ = -33.0 kJ/mol at 298 K

Calculate ฮ”G\Delta G when PN2=1.0P_{\text{N}_2} = 1.0 atm, PH2=3.0P_{\text{H}_2} = 3.0 atm, PNH3=0.50P_{\text{NH}_3} = 0.50 atm.

Step 1: Calculate Q

Q=(PNH3)2(PN2)(PH2)3=(0.50)2(1.0)(3.0)3=0.2527=0.00926Q = \frac{(P_{\text{NH}_3})^2}{(P_{\text{N}_2})(P_{\text{H}_2})^3} = \frac{(0.50)^2}{(1.0)(3.0)^3} = \frac{0.25}{27} = 0.00926

Step 2: Calculate ฮ”G

ฮ”G=ฮ”Gยฐ+RTlnโกQ\Delta G = \Delta Gยฐ + RT\ln Q =โˆ’33,000+(8.314)(298)lnโก(0.00926)= -33{,}000 + (8.314)(298)\ln(0.00926) =โˆ’33,000+(2478)(โˆ’4.682)= -33{,}000 + (2478)(-4.682) =โˆ’33,000+(โˆ’11,602)= -33{,}000 + (-11{,}602) =โˆ’44,602ย J=โˆ’44.6ย kJ= -44{,}602 \text{ J} = -44.6 \text{ kJ}

Since ฮ”G<0\Delta G < 0 and Q<KQ < K, the forward reaction is spontaneous โ€” more NH3\text{NH}_3 will form.

Non-Standard ฮ”G Quiz ๐ŸŽฏ

Non-Standard ฮ”G Calculations ๐Ÿงฎ

For a reaction with ฮ”Gยฐ=โˆ’10.0\Delta Gยฐ = -10.0 kJ/mol at T=298T = 298 K:

  1. What is ฮ”G\Delta G when Q=1Q = 1? (in kJ/mol)

  2. What is ฮ”G\Delta G when Q=KQ = K (at equilibrium)? (in kJ/mol)

  3. If Q>KQ > K, is ฮ”G\Delta G positive or negative? (type "positive" or "negative")

Round all answers to 3 significant figures.

Q, K, and ฮ”G ๐Ÿ”ฝ

Exit Quiz โ€” Non-Standard ฮ”G โœ…

Part 6: Problem-Solving Workshop

๐Ÿ› ๏ธ Problem-Solving Workshop โ€” Gibbs Free Energy

Part 6 of 7 โ€” Practice and Integration

This workshop brings together all the Gibbs free energy tools: calculating ฮ”G from ฮ”H and ฮ”S, using formation values, the four sign cases, ฮ”Gยฐ-K relationships, and non-standard conditions.

Problem-Solving Flowchart

What Are You Given? โ†’ What Method to Use?

GivenMethod
ฮ”H\Delta H and ฮ”S\Delta S (or SยฐSยฐ)ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta S
ฮ”Gยฐf\Delta Gยฐ_f valuesฮ”Gยฐ=โˆ‘ฮ”Gยฐf(prod)โˆ’โˆ‘ฮ”Gยฐf(react)\Delta Gยฐ = \sum \Delta Gยฐ_f(\text{prod}) - \sum \Delta Gยฐ_f(\text{react})
KK (equilibrium constant)ฮ”Gยฐ=โˆ’RTlnโกK\Delta Gยฐ = -RT\ln K
ฮ”Gยฐ\Delta Gยฐ and QQฮ”G=ฮ”Gยฐ+RTlnโกQ\Delta G = \Delta Gยฐ + RT\ln Q

Common Unit Traps

QuantityCommon UnitsWatch Out
ฮ”H\Delta HkJConvert to J if using R=8.314R = 8.314 J/(molยทK)
ฮ”S\Delta SJ/KConvert to kJ/K if combining with ฮ”H in kJ
ฮ”G\Delta GkJ or JMatch with RR
TTKNever use ยฐC in these equations!

Mixed ฮ”G Problems ๐ŸŽฏ

Multi-Step Calculation Workshop ๐Ÿงฎ

  1. A reaction has ฮ”Hยฐ=+50\Delta Hยฐ = +50 kJ and ฮ”Sยฐ=+150\Delta Sยฐ = +150 J/K. What is ฮ”Gยฐ\Delta Gยฐ at 400 K? (in kJ)

  2. For the reaction in (1), what is KK at 400 K? (round to nearest whole number; use e3.01โ‰ˆ20e^{3.01} \approx 20)

  3. A reaction has ฮ”Gยฐ=โˆ’20\Delta Gยฐ = -20 kJ/mol. What is KK at 298 K? (round to nearest thousand; use e8.07โ‰ˆ3200e^{8.07} \approx 3200)

Problem Strategy Selection ๐Ÿ”ฝ

Exit Quiz โ€” Problem-Solving Workshop โœ…

Part 7: Synthesis & AP Review

๐ŸŽฏ Synthesis & AP Review โ€” Gibbs Free Energy

Part 7 of 7 โ€” Mastering the Connections

Gibbs free energy ties together enthalpy, entropy, equilibrium, and electrochemistry. This final review ensures you can navigate all the relationships and solve any AP-level problem.

The Web of Thermodynamic Equations

Core Equations

EquationWhen to Use
ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta SCalculate ฮ”G from enthalpy and entropy
ฮ”Gยฐ=โˆ‘ฮ”Gยฐf(prod)โˆ’โˆ‘ฮ”Gยฐf(react)\Delta Gยฐ = \sum \Delta Gยฐ_f(\text{prod}) - \sum \Delta Gยฐ_f(\text{react})Calculate from tables
ฮ”Gยฐ=โˆ’RTlnโกK\Delta Gยฐ = -RT\ln KConnect free energy to equilibrium
ฮ”G=ฮ”Gยฐ+RTlnโกQ\Delta G = \Delta Gยฐ + RT\ln QNon-standard conditions
ฮ”Gยฐ=โˆ’nFEยฐ\Delta Gยฐ = -nFEยฐConnect to electrochemistry (Topic 4)

The Four Sign Cases

ฮ”H\Delta Hฮ”S\Delta SSpontaneous?Crossover T
โˆ’+AlwaysNone
+โˆ’NeverNone
โˆ’โˆ’Low TT=ฮ”H/ฮ”ST = \Delta H/\Delta S
++High TT=ฮ”H/ฮ”ST = \Delta H/\Delta S

Critical Relationships

  • ฮ”Gยฐ<0โ‡”K>1\Delta Gยฐ < 0 \Leftrightarrow K > 1 (products favored)
  • ฮ”Gยฐ=0โ‡”K=1\Delta Gยฐ = 0 \Leftrightarrow K = 1
  • ฮ”Gยฐ>0โ‡”K<1\Delta Gยฐ > 0 \Leftrightarrow K < 1 (reactants favored)
  • ฮ”G<0\Delta G < 0: forward reaction proceeds
  • ฮ”G=0\Delta G = 0: at equilibrium
  • ฮ”G>0\Delta G > 0: reverse reaction proceeds

Comprehensive AP Review ๐ŸŽฏ

Integration Problems ๐Ÿงฎ

  1. ฮ”Hยฐ=โˆ’180\Delta Hยฐ = -180 kJ, ฮ”Sยฐ=โˆ’250\Delta Sยฐ = -250 J/K. What is the crossover temperature? (in K)

  2. At 298 K, ฮ”Gยฐ=โˆ’57.1\Delta Gยฐ = -57.1 kJ/mol. What is KK? (use e23.0โ‰ˆ1010e^{23.0} \approx 10^{10}; express as a power of 10)

  3. A reaction has ฮ”Gยฐ=+5.0\Delta Gยฐ = +5.0 kJ/mol. At what value of QQ does ฮ”G=0\Delta G = 0 at 298 K? (i.e., what is KK? Round to nearest tenth; use eโˆ’2.02โ‰ˆ0.1e^{-2.02} \approx 0.1)

Final Concept Review ๐Ÿ”ฝ

Final Exit Quiz โ€” Gibbs Free Energy Mastery โœ