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๐ŸŽฏโญ INTERACTIVE LESSON

Spontaneity and Free Energy Applications

Learn step-by-step with interactive practice!

Spontaneity and Free Energy Applications - 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


Topics in This Part

Section
โšก Defining Gibbs Free Energy
Where Does This Come From?
โšก The Spontaneity Criterion
Why Gibbs Free Energy Is So Useful
What "Free" Means

๐Ÿ”‘ Key Concept: Mastering this material will strengthen your foundation for both the AP Chemistry exam and more advanced chemistry topics.


What You'll Master in Part 1

  • Understanding the core concepts covered in Part 1
  • Applying these ideas to solve practice problems
  • Building toward AP exam readiness for this topic

โšก Defining Gibbs Free Energy

G=Hโˆ’TSG = H - TS

The change in Gibbs free energy at constant temperature:

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

๐Ÿ”‘ Key Equation: This is the master equation of Gibbs free energy โ€” it combines enthalpy and entropy into a single criterion for spontaneity.


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

โšก 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)

๐Ÿ”‘ Key Concept: Memorize this table โ€” it's the foundation for every Gibbs free energy problem on the AP exam.


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”G\boxed{w_{\text{max}} = \Delta G}

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

โšก 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)

โš ๏ธ Warning: Temperature must always be in Kelvin in thermodynamic equations. Also ensure ฮ”H\Delta H and Tฮ”ST\Delta S use the same units (both kJ or both J).


The Crossover Temperature

When ฮ”G=0\Delta G = 0 (equilibrium):

T=ฮ”Hฮ”S\boxed{T = \frac{\Delta H}{\Delta S}}

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


Example

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

Solution:

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


Topics in This Part

Section
๐Ÿ“Œ The Four Cases
Case 1: ฮ”H < 0, ฮ”S > 0 โ€” Always Spontaneous โœ…
Case 2: ฮ”H > 0, ฮ”S < 0 โ€” Never Spontaneous โŒ
Case 3: ฮ”H < 0, ฮ”S < 0 โ€” Spontaneous at Low T ๐Ÿฅถ
Case 4: ฮ”H > 0, ฮ”S > 0 โ€” Spontaneous at High T ๐Ÿ”ฅ

๐Ÿ”‘ Key Concept: Mastering this material will strengthen your foundation for both the AP Chemistry exam and more advanced chemistry topics.


What You'll Master in Part 2

  • Understanding the core concepts covered in Part 2
  • Applying these ideas to solve practice problems
  • Building toward AP exam readiness for this topic

๐Ÿ“Œ 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

๐Ÿ“‹ 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

๐Ÿ”‘ Key Concept: This table appears on nearly every AP Chemistry exam. Memorize all four cases and be ready to identify which case applies from ฮ”H/ฮ”S signs.


The Crossover Temperature

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

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

๐Ÿ’ก Tip: This equation only gives a physically meaningful (positive) temperature when ฮ”H\Delta H and ฮ”S\Delta S have the same sign (Cases 3 and 4).

๐Ÿงช 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


Topics in This Part

Section
โšก Standard Free Energy of Formation (ฮ”Gยฐf\Delta Gยฐ_f)
The Master Equation
Key Rule
Sample Values
๐Ÿงช Worked Example

๐Ÿ”‘ Key Concept: Mastering this material will strengthen your foundation for both the AP Chemistry exam and more advanced chemistry topics.


What You'll Master in Part 3

  • Understanding the core concepts covered in Part 3
  • Applying these ideas to solve practice problems
  • Building toward AP exam readiness for this topic

โšก 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)\boxed{\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\boxed{\Delta Gยฐ_f = 0 \text{ for all elements in their standard states}}

๐Ÿ”‘ Key Concept: Same convention as ฮ”Hยฐf\Delta Hยฐ_f โ€” elements in their standard states are the reference point.


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

๐Ÿงช Worked Example

Problem: 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

Solution: 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

Given:

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
C2H6(g)\text{C}_2\text{H}_6(g)โˆ’32.0-32.0
O2(g)\text{O}_2(g)00

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.

โš–๏ธ 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

โš ๏ธ Warning: 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


Topics in This Part

Section
๐Ÿ”‘ The Key Equation
What This Equation Tells Us
Important Nuance
๐Ÿ“Œ Solving for K from ฮ”Gยฐ
Worked Example

๐Ÿ”‘ Key Concept: Mastering this material will strengthen your foundation for both the AP Chemistry exam and more advanced chemistry topics.


What You'll Master in Part 4

  • Understanding the core concepts covered in Part 4
  • Applying these ideas to solve practice problems
  • Building toward AP exam readiness for this topic

๐Ÿ”‘ The Key Equation

ฮ”Gยฐ=โˆ’RTlnโกK\boxed{\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

๐Ÿ”‘ Key Concept: The sign of ฮ”Gยฐ\Delta Gยฐ tells you the position of equilibrium โ€” whether products (K>1K > 1) or reactants (K<1K < 1) are favored.


Important Nuance

โš ๏ธ Warning: 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.

๐Ÿ“Œ Solving for K from ฮ”Gยฐ

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


Worked Example

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

Solution:

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

โš ๏ธ Warning: When using ฮ”Gยฐ=โˆ’RTlnโกK\Delta Gยฐ = -RT\ln K, RR must be 8.3148.314 J/(molยทK) and ฮ”Gยฐ\Delta Gยฐ must be in J/mol (not kJ). Convert kJ to J before plugging in!

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


Topics in This Part

Section
โšก The Non-Standard Free Energy Equation
Recall: Q vs K
๐Ÿ“Œ Interpreting ฮ”G, Q, and K
Key Insight
The Big Picture

๐Ÿ”‘ Key Concept: Mastering this material will strengthen your foundation for both the AP Chemistry exam and more advanced chemistry topics.


What You'll Master in Part 5

  • Understanding the core concepts covered in Part 5
  • Applying these ideas to solve practice problems
  • Building toward AP exam readiness for this topic

โšก The Non-Standard Free Energy Equation

ฮ”G=ฮ”Gยฐ+RTlnโกQ\boxed{\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)

๐Ÿ“Œ 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

๐Ÿ”‘ Key Concept: The relationship between QQ and KK determines the direction of spontaneous change โ€” always toward equilibrium.


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

โš ๏ธ Warning: Don't confuse ฮ”Gยฐ\Delta Gยฐ and ฮ”G\Delta G โ€” they answer different questions:

  • 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

๐Ÿงช Worked Example โ€” Non-Standard ฮ”G

Problem: 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), with 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.

Given

QuantityValue
ฮ”Gยฐ\Delta Gยฐโˆ’33.0-33.0 kJ/mol = โˆ’33,000-33{,}000 J/mol
TT298 K
RR8.314 J/(molยทK)
PN2P_{\text{N}_2}1.0 atm
PH2P_{\text{H}_2}3.0 atm
PNH3P_{\text{NH}_3}0.50 atm

Step-by-Step Solution

StepActionCalculationResult
1Calculate QQ(0.50)2(1.0)(3.0)3=0.2527\frac{(0.50)^2}{(1.0)(3.0)^3} = \frac{0.25}{27}Q=0.00926Q = 0.00926
2Calculate RTRT(8.314)(298)(8.314)(298)2478ย J/mol2478 \text{ J/mol}
3Calculate RTlnโกQRT\ln Q(2478)(lnโก0.00926)=(2478)(โˆ’4.682)(2478)(\ln 0.00926) = (2478)(-4.682)โˆ’11,602ย J-11{,}602 \text{ J}
4Calculate ฮ”G\Delta Gโˆ’33,000+(โˆ’11,602)-33{,}000 + (-11{,}602)ฮ”G=โˆ’44.6ย kJ\Delta G = -44.6 \text{ kJ}

๐Ÿ”‘ Interpretation: Since ฮ”G<0\Delta G < 0 and Q<KQ < K, the forward reaction is spontaneous โ€” more NH3\text{NH}_3 will form until the system reaches equilibrium.

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


Practice Makes Perfect

This workshop features multi-step problems that mirror the AP Chemistry exam format. Each problem requires you to combine concepts from previous parts and show your work clearly.

๐Ÿ”‘ Why this matters: The AP Chemistry exam rewards students who can apply concepts to unfamiliar problems โ€” structured practice is the best preparation.


What You'll Master in Part 6

  • Working through complete multi-step problems from start to finish
  • Building problem-solving strategies you can apply on the AP exam
  • Identifying which concepts to apply and in what order

๐Ÿ› ๏ธ Problem-Solving Flowchart

๐Ÿ’ก Tip: On the AP exam, identify what you're given first, then choose the correct equation.

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

โš ๏ธ Warning: Unit mismatches are the #1 source of errors in Gibbs free energy calculations!

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


Bringing It All Together

This comprehensive review connects every concept from Parts 1โ€“6 with AP-style problems. The questions are designed to mirror what you'll see on the actual exam โ€” multi-step, multi-concept, and requiring clear written explanations.

๐Ÿ”‘ Why this matters: AP Chemistry exam questions rarely test one concept in isolation โ€” success requires connecting ideas across topics.


What You'll Master in Part 7

  • Solving AP-style questions that integrate multiple concepts from this unit
  • Writing clear, concise explanations using proper chemistry terminology
  • Identifying and avoiding common AP exam traps and mistakes

๐ŸŒก๏ธ The Web of Thermodynamic Equations

Core Equations

๐Ÿ”‘ Key Concept: These five equations form the complete Gibbs free energy toolkit for AP Chemistry. | Equation | When to Use | |----------|-------------| | ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta S | Calculate 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 K | Connect free energy to equilibrium | | ฮ”G=ฮ”Gยฐ+RTlnโกQ\Delta G = \Delta Gยฐ + RT\ln Q | Non-standard conditions | | ฮ”Gยฐ=โˆ’nFEยฐ\Delta Gยฐ = -nFEยฐ | Connect 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

โš ๏ธ Warning: Notice the distinction โ€” ฮ”Gยฐ\Delta Gยฐ (with ยฐ) predicts equilibrium position, while ฮ”G\Delta G (without ยฐ) predicts reaction direction.

  • 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