๐ŸŽฏโญ INTERACTIVE LESSON

Entropy and the Second Law

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Entropy and the Second Law - Complete Interactive Lesson

Part 1: Introduction to Entropy

๐ŸŽฒ What Is Entropy?

Part 1 of 7 โ€” Disorder, Microstates, and S = k ln W

Why do ice cubes melt at room temperature but never spontaneously re-freeze? Why does gas expand to fill a container? The answer lies in entropy โ€” a measure of the number of ways energy and matter can be distributed in a system.

Entropy and "Disorder"

Entropy (SS) is often described as a measure of disorder or randomness. While this is a helpful starting point, the more precise definition involves microstates.

Everyday Examples of Increasing Entropy

ProcessLower EntropyHigher Entropy
Ice meltingSolid (ordered)Liquid (disordered)
Gas expandingCompressed gasExpanded gas
Dissolving saltCrystalline solidIons in solution
Shuffling cardsOrdered deckRandom arrangement

Key Insight

Systems naturally tend toward states of higher entropy. This is not because nature "prefers disorder" โ€” it is because there are vastly more disordered arrangements than ordered ones.

Microstates and the Boltzmann Equation

What Is a Microstate?

A microstate (WW) is a specific arrangement of particles and energy in a system. The more microstates available, the higher the entropy.

Boltzmann's Equation

S=kBlnโกWS = k_B \ln W

SymbolMeaningValue
SSEntropyJ/K
kBk_BBoltzmann constant1.38ร—10โˆ’231.38 \times 10^{-23} J/K
WWNumber of microstatesdimensionless
lnโก\lnNatural logarithmโ€”

Example: Two Coins

  • 2 coins have 22=42^2 = 4 microstates: HH, HT, TH, TT
  • The "disordered" state (one H, one T) has 2 microstates โ†’ most probable
  • The "ordered" states (both H or both T) have 1 microstate each

Scaling Up

For 102310^{23} particles (a mole), the number of microstates is astronomically large. The probability of all gas molecules spontaneously gathering in one corner is essentially zero โ€” not because it violates any law, but because the number of "spread out" microstates vastly outnumbers "concentrated" ones.

Entropy Is Extensive

Entropy depends on the amount of substance โ€” double the amount, double the entropy.

Units and Properties of Entropy

Units

Entropy is measured in J/K (joules per kelvin) or J/(molยทK) for molar entropy.

Note: Unlike enthalpy (kJ), entropy uses joules โ€” a common source of unit errors on the AP exam!

Key Properties

PropertyDescription
State functionDepends only on current state, not path
ExtensiveProportional to amount of substance
Always positiveS>0S > 0 for any real substance (at T>0T > 0 K)
Increases with THigher temperature = more microstates

Entropy Is NOT Conserved

Unlike energy, entropy can be created (in irreversible processes). The total entropy of the universe always increases for spontaneous processes.

Entropy Concept Quiz ๐ŸŽฏ

Microstate Counting ๐Ÿงฎ

  1. How many microstates does a system of 3 coins have? (W=2nW = 2^n)

  2. For 4 coins, what fraction of microstates have ALL heads? (express as a simplified fraction like 1/16)

  3. If system A has W=100W = 100 microstates and system B has W=200W = 200 microstates, which has higher entropy? (type A or B)

Entropy Basics ๐Ÿ”ฝ

Exit Quiz โ€” What Is Entropy? โœ…

Part 2: Microstates & Disorder

๐Ÿ“ˆ Predicting Entropy Changes

Part 2 of 7 โ€” More Gas = More Entropy

Before we calculate ฮ”S\Delta S numerically, we need to develop the ability to predict whether entropy increases or decreases in a process. This qualitative skill is tested heavily on the AP exam and relies on simple rules about phases, moles of gas, and molecular complexity.

Entropy and Phase

Entropy increases dramatically as matter moves from solid to liquid to gas:

Ssolid<Sliquidโ‰ชSgasS_{\text{solid}} < S_{\text{liquid}} \ll S_{\text{gas}}

Why?

PhaseMolecular FreedomRelative Entropy
SolidFixed positions, vibration onlyLowest
LiquidClose together but mobileMedium
GasFar apart, random motionHighest

The jump from liquid โ†’ gas is much larger than solid โ†’ liquid because gas molecules have vastly more accessible positions and velocities.

Phase Change Entropy

Processฮ”S\Delta SReason
Melting (fusion)PositiveSolid โ†’ liquid (more freedom)
VaporizationPositive (large)Liquid โ†’ gas (much more freedom)
SublimationPositive (largest)Solid โ†’ gas
FreezingNegativeLiquid โ†’ solid (less freedom)
CondensationNegativeGas โ†’ liquid (less freedom)

Rules for Predicting ฮ”S\Delta S of Reactions

Rule 1: Count Moles of Gas

The most reliable predictor of ฮ”S\Delta S:

ฮ”ngas=molย gasย (products)โˆ’molย gasย (reactants)\Delta n_{\text{gas}} = \text{mol gas (products)} - \text{mol gas (reactants)}

  • If ฮ”ngas>0\Delta n_{\text{gas}} > 0: ฮ”S>0\Delta S > 0 (entropy increases)
  • If ฮ”ngas<0\Delta n_{\text{gas}} < 0: ฮ”S<0\Delta S < 0 (entropy decreases)
  • If ฮ”ngas=0\Delta n_{\text{gas}} = 0: need other information

Rule 2: Dissolving Usually Increases Entropy

When a solid dissolves in a solvent, entropy typically increases (solid โ†’ ions or molecules in solution).

Exception: Some ions become so heavily hydrated that they actually decrease the entropy of water molecules around them.

Rule 3: More Molecules = More Entropy

A reaction that produces more total molecules than it consumes generally has ฮ”S>0\Delta S > 0.

Rule 4: Temperature Increases Entropy

Higher temperature means more kinetic energy and more accessible microstates.

Rule 5: Molecular Complexity

More complex molecules (more atoms, more bonds, more ways to vibrate) have higher entropy than simpler ones.

Practice Examples

Reactionฮ”ngas\Delta n_{\text{gas}}Prediction
2H2(g)+O2(g)โ†’2H2O(g)2\text{H}_2(g) + \text{O}_2(g) \rightarrow 2\text{H}_2\text{O}(g)2โˆ’3=โˆ’12 - 3 = -1ฮ”S<0\Delta S < 0
CaCO3(s)โ†’CaO(s)+CO2(g)\text{CaCO}_3(s) \rightarrow \text{CaO}(s) + \text{CO}_2(g)1โˆ’0=+11 - 0 = +1ฮ”S>0\Delta S > 0
N2(g)+3H2(g)โ†’2NH3(g)\text{N}_2(g) + 3\text{H}_2(g) \rightarrow 2\text{NH}_3(g)2โˆ’4=โˆ’22 - 4 = -2ฮ”S<0\Delta S < 0
2KClO3(s)โ†’2KCl(s)+3O2(g)2\text{KClO}_3(s) \rightarrow 2\text{KCl}(s) + 3\text{O}_2(g)3โˆ’0=+33 - 0 = +3ฮ”S>0\Delta S > 0

Key Insight for AP

When asked to "predict the sign of ฮ”S\Delta S" โ€” always start by counting moles of gas. If ฮ”ngas=0\Delta n_{\text{gas}} = 0, then consider total moles and phases.

Predicting Entropy Quiz ๐ŸŽฏ

Predict ฮ”S Sign ๐Ÿงฎ

Type "positive" or "negative" for the sign of ฮ”S\Delta S:

  1. H2O(l)โ†’H2O(g)\text{H}_2\text{O}(l) \rightarrow \text{H}_2\text{O}(g)

  2. N2(g)+3H2(g)โ†’2NH3(g)\text{N}_2(g) + 3\text{H}_2(g) \rightarrow 2\text{NH}_3(g)

  3. 2NH4NO3(s)โ†’2N2(g)+O2(g)+4H2O(g)\text{2NH}_4\text{NO}_3(s) \rightarrow 2\text{N}_2(g) + \text{O}_2(g) + 4\text{H}_2\text{O}(g)

Entropy Predictions ๐Ÿ”ฝ

Exit Quiz โ€” Predicting Entropy โœ…

Part 3: Second Law of Thermodynamics

๐ŸŒ The Second Law of Thermodynamics

Part 3 of 7 โ€” ฮ”S_universe > 0 for Spontaneous Processes

The Second Law is one of the most profound principles in all of science. It tells us which direction processes naturally go and provides the ultimate criterion for spontaneity.

The Second Law

The entropy of the universe increases for every spontaneous process.

ฮ”Suniverse=ฮ”Ssystem+ฮ”Ssurroundings>0\Delta S_{\text{universe}} = \Delta S_{\text{system}} + \Delta S_{\text{surroundings}} > 0

Three Cases

ConditionProcess Type
ฮ”Suniverse>0\Delta S_{\text{universe}} > 0Spontaneous (irreversible)
ฮ”Suniverse=0\Delta S_{\text{universe}} = 0At equilibrium (reversible)
ฮ”Suniverse<0\Delta S_{\text{universe}} < 0Nonspontaneous (reverse is spontaneous)

What Does "Spontaneous" Mean?

A spontaneous process occurs without continuous outside intervention. It does NOT mean:

  • Fast (diamond โ†’ graphite is spontaneous but infinitely slow)
  • Without any initial input (a match needs a spark, but then burning is spontaneous)

It DOES mean:

  • The process is thermodynamically favorable
  • The reverse process will not happen on its own

Entropy of the Surroundings

The entropy change of the surroundings depends on the heat flow and temperature:

ฮ”Ssurroundings=โˆ’qsystemT=โˆ’ฮ”HsystemT\Delta S_{\text{surroundings}} = -\frac{q_{\text{system}}}{T} = -\frac{\Delta H_{\text{system}}}{T}

(at constant pressure and temperature)

Why the Negative Sign?

Heat released by the system (โˆ’q-q) is absorbed by the surroundings (+q+q), and vice versa.

Why Divide by Temperature?

The same amount of heat has a greater impact on entropy at lower temperature:

  • Adding 100 J of heat to a cold system (200 K) creates a larger entropy change than adding 100 J to a hot system (1000 K)
  • This is like adding 10tosomeonewith10 to someone with 100 vs. someone with $10,000

Combining System and Surroundings

ฮ”Suniverse=ฮ”Ssystem+(โˆ’ฮ”HsystemT)\Delta S_{\text{universe}} = \Delta S_{\text{system}} + \left(-\frac{\Delta H_{\text{system}}}{T}\right)

This equation connects entropy, enthalpy, and spontaneity โ€” leading directly to Gibbs Free Energy (covered in Topic 3).

How Spontaneous Processes Work

Exothermic Reactions at Room Temperature

For combustion of methane: ฮ”Hsys<0\Delta H_{\text{sys}} < 0

  • ฮ”Ssurr=โˆ’ฮ”H/T>0\Delta S_{\text{surr}} = -\Delta H/T > 0 (large positive)
  • Even if ฮ”Ssys<0\Delta S_{\text{sys}} < 0, ฮ”Suniv\Delta S_{\text{univ}} can still be positive
  • The large heat release drives spontaneity

Endothermic Spontaneous Processes

Ice melting above 0ยฐC: ฮ”Hsys>0\Delta H_{\text{sys}} > 0

  • ฮ”Ssurr=โˆ’ฮ”H/T<0\Delta S_{\text{surr}} = -\Delta H/T < 0 (negative)
  • But ฮ”Ssys>0\Delta S_{\text{sys}} > 0 (solid โ†’ liquid, large increase)
  • If ฮ”Ssys\Delta S_{\text{sys}} outweighs โˆฃฮ”Ssurrโˆฃ|\Delta S_{\text{surr}}|, the process is spontaneous

Temperature Dependence

At the melting point (0ยฐC for water): ฮ”Suniverse=0(equilibrium)\Delta S_{\text{universe}} = 0 \quad \text{(equilibrium)}

Above 0ยฐC: melting is spontaneous. Below 0ยฐC: freezing is spontaneous.

Second Law Concept Quiz ๐ŸŽฏ

Second Law Calculations ๐Ÿงฎ

  1. A reaction has ฮ”H=โˆ’100\Delta H = -100 kJ and ฮ”Ssys=โˆ’50\Delta S_{\text{sys}} = -50 J/K at T=400T = 400 K. What is ฮ”Ssurr\Delta S_{\text{surr}}? (in J/K)

  2. Using your answer from (1), what is ฮ”Suniverse\Delta S_{\text{universe}}? (in J/K)

  3. Is the reaction spontaneous? (type "yes" or "no")

Second Law Concepts ๐Ÿ”ฝ

Exit Quiz โ€” Second Law โœ…

Part 4: Standard Entropy Changes

โ„๏ธ The Third Law and Standard Molar Entropy

Part 4 of 7 โ€” S = 0 at Absolute Zero

The Third Law of Thermodynamics provides a reference point for entropy. Unlike enthalpy, where we can only measure changes, entropy has an absolute scale โ€” and it starts at zero.

The Third Law of Thermodynamics

The entropy of a perfect crystal at absolute zero (0 K) is exactly zero.

S=0atย T=0ย Kย (perfectย crystal)S = 0 \quad \text{at } T = 0 \text{ K (perfect crystal)}

Why Zero?

At absolute zero:

  • All molecular motion ceases (except zero-point energy)
  • A perfect crystal has only one microstate (W=1W = 1)
  • S=klnโก1=0S = k \ln 1 = 0

Consequences

  1. Absolute entropy values can be determined (unlike enthalpy)
  2. All substances at T>0T > 0 K have S>0S > 0
  3. Absolute zero can never actually be reached (it would require an infinite number of cooling steps)

Standard Molar Entropy (SยฐSยฐ)

The entropy of one mole of a substance at standard conditions (1 atm, usually 25ยฐC).

Key Values to Know

SubstanceSยฐSยฐ [J/(molยทK)]
C(s,graphite)\text{C}(s, \text{graphite})5.7
C(s,diamond)\text{C}(s, \text{diamond})2.4
H2(g)\text{H}_2(g)130.7
N2(g)\text{N}_2(g)191.6
O2(g)\text{O}_2(g)205.1
H2O(l)\text{H}_2\text{O}(l)69.9
H2O(g)\text{H}_2\text{O}(g)188.8
CO2(g)\text{CO}_2(g)213.7
NH3(g)\text{NH}_3(g)192.5

Patterns in Standard Entropy

  1. Gases > liquids > solids โ€” always!
  2. More complex molecules have higher SยฐSยฐ
  3. Heavier atoms tend to have higher SยฐSยฐ (more accessible energy levels)
  4. Allotropes differ: diamond (2.4) < graphite (5.7) โ€” more ordered crystal

Important: Sยฐ>0Sยฐ > 0 for ALL substances at 298 K

Unlike ฮ”Hยฐf\Delta Hยฐ_f, which is zero for elements, SยฐSยฐ is never zero at room temperature. Every substance has entropy at temperatures above 0 K.

How Entropy Varies with Temperature

As temperature increases from 0 K, entropy increases through several stages:

Heating a Substance

  1. Solid phase: SS increases gradually as vibrations intensify
  2. At melting point: sudden jump in SS (phase change โ€” fusion)
  3. Liquid phase: SS continues to increase
  4. At boiling point: large jump in SS (phase change โ€” vaporization)
  5. Gas phase: SS continues to increase

Key Feature

The jump at the boiling point is much larger than at the melting point, because the liquid โ†’ gas transition involves a much greater increase in molecular freedom.

Phase Transition Entropy

ฮ”Stransition=ฮ”HtransitionTtransition\Delta S_{\text{transition}} = \frac{\Delta H_{\text{transition}}}{T_{\text{transition}}}

This formula applies at the equilibrium transition temperature, where the process is reversible.

Third Law Concept Quiz ๐ŸŽฏ

Compare Standard Entropies ๐Ÿงฎ

Which substance has the HIGHER standard molar entropy? Type the chemical formula.

  1. H2O(l)\text{H}_2\text{O}(l) or H2O(g)\text{H}_2\text{O}(g)?

  2. C(s,diamond)\text{C}(s, \text{diamond}) or C(s,graphite)\text{C}(s, \text{graphite})?

  3. O2(g)\text{O}_2(g) or O3(g)\text{O}_3(g)?

Third Law and Standard Entropy ๐Ÿ”ฝ

Exit Quiz โ€” Third Law & Standard Entropy โœ…

Part 5: Predicting Entropy Changes

๐Ÿ”ข Calculating ฮ”Sยฐ_rxn from Standard Entropies

Part 5 of 7 โ€” The Entropy Version of the Master Equation

Just as we calculated ฮ”Hยฐrxn\Delta Hยฐ_{\text{rxn}} from formation enthalpies, we can calculate ฮ”Sยฐrxn\Delta Sยฐ_{\text{rxn}} from standard molar entropies. The formula is very similar โ€” products minus reactants.

The Entropy Master Equation

ฮ”Sยฐrxn=โˆ‘nโ‹…Sยฐ(products)โˆ’โˆ‘mโ‹…Sยฐ(reactants)\Delta Sยฐ_{\text{rxn}} = \sum n \cdot Sยฐ(\text{products}) - \sum m \cdot Sยฐ(\text{reactants})

where nn and mm are stoichiometric coefficients.

Key Differences from the Enthalpy Version

FeatureEnthalpyEntropy
Formulaฮ”Hยฐ=โˆ‘ฮ”Hยฐf(prod)โˆ’โˆ‘ฮ”Hยฐf(react)\Delta Hยฐ = \sum \Delta Hยฐ_f(\text{prod}) - \sum \Delta Hยฐ_f(\text{react})ฮ”Sยฐ=โˆ‘Sยฐ(prod)โˆ’โˆ‘Sยฐ(react)\Delta Sยฐ = \sum Sยฐ(\text{prod}) - \sum Sยฐ(\text{react})
Usesฮ”Hยฐf\Delta Hยฐ_f (formation enthalpies)SยฐSยฐ (absolute entropies)
Elementsฮ”Hยฐf=0\Delta Hยฐ_f = 0Sยฐโ‰ 0Sยฐ \neq 0 (always positive!)
UnitskJJ/K

Critical Warning โš ๏ธ

SยฐSยฐ for elements is NOT zero! This is the #1 mistake students make. Absolute entropies are always positive at temperatures above 0 K.

Worked Example

Calculate ฮ”Sยฐ\Delta Sยฐ for: N2(g)+3H2(g)โ†’2NH3(g)\text{N}_2(g) + 3\text{H}_2(g) \rightarrow 2\text{NH}_3(g)

SubstanceSยฐSยฐ [J/(molยทK)]
N2(g)\text{N}_2(g)191.6
H2(g)\text{H}_2(g)130.7
NH3(g)\text{NH}_3(g)192.5

Solution:

ฮ”Sยฐ=โˆ‘Sยฐ(products)โˆ’โˆ‘Sยฐ(reactants)\Delta Sยฐ = \sum Sยฐ(\text{products}) - \sum Sยฐ(\text{reactants})

ฮ”Sยฐ=[2(192.5)]โˆ’[1(191.6)+3(130.7)]\Delta Sยฐ = [2(192.5)] - [1(191.6) + 3(130.7)]

ฮ”Sยฐ=385.0โˆ’[191.6+392.1]\Delta Sยฐ = 385.0 - [191.6 + 392.1]

ฮ”Sยฐ=385.0โˆ’583.7=โˆ’198.7ย J/K\Delta Sยฐ = 385.0 - 583.7 = -198.7 \text{ J/K}

Check: Does the Sign Make Sense?

ฮ”ngas=2โˆ’4=โˆ’2\Delta n_{\text{gas}} = 2 - 4 = -2 (fewer moles of gas in products)

ฮ”S<0\Delta S < 0 โœ“ โ€” consistent with our prediction!

ฮ”Sยฐ Calculation Concept Quiz ๐ŸŽฏ

ฮ”Sยฐ Calculations ๐Ÿงฎ

Use these SยฐSยฐ values [J/(molยทK)]: CO2(g)=213.7\text{CO}_2(g) = 213.7, H2O(g)=188.8\text{H}_2\text{O}(g) = 188.8, H2O(l)=69.9\text{H}_2\text{O}(l) = 69.9, CH4(g)=186.3\text{CH}_4(g) = 186.3, O2(g)=205.1\text{O}_2(g) = 205.1, C(s)=5.7\text{C}(s) = 5.7, H2(g)=130.7\text{H}_2(g) = 130.7

  1. Calculate ฮ”Sยฐ\Delta Sยฐ for: C(s)+O2(g)โ†’CO2(g)\text{C}(s) + \text{O}_2(g) \rightarrow \text{CO}_2(g) [J/K, to 3 significant figures]

  2. Calculate ฮ”Sยฐ\Delta Sยฐ for: 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) [J/K, to 3 significant figures]

ฮ”Sยฐ Concepts ๐Ÿ”ฝ

Exit Quiz โ€” Calculating ฮ”Sยฐ โœ…

Part 6: Problem-Solving Workshop

๐Ÿ› ๏ธ Problem-Solving Workshop โ€” Entropy

Part 6 of 7 โ€” Practice and Strategies

This workshop focuses on the types of entropy problems you will encounter on the AP exam. We will practice predicting signs, calculating ฮ”Sยฐ\Delta Sยฐ, and connecting entropy to spontaneity.

Problem-Solving Strategies

Strategy 1: Predict the Sign of ฮ”S

  1. Count moles of gas: ฮ”ngas=molย gasย (products)โˆ’molย gasย (reactants)\Delta n_{\text{gas}} = \text{mol gas (products)} - \text{mol gas (reactants)}
  2. If ฮ”ngas>0\Delta n_{\text{gas}} > 0: ฮ”S>0\Delta S > 0
  3. If ฮ”ngas<0\Delta n_{\text{gas}} < 0: ฮ”S<0\Delta S < 0
  4. If ฮ”ngas=0\Delta n_{\text{gas}} = 0: consider phase changes, complexity, and total moles

Strategy 2: Calculate ฮ”Sยฐ

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

Remember: SยฐSยฐ for elements is NOT zero!

Strategy 3: Unit Conversion

  • ฮ”H\Delta H is typically in kJ
  • ฮ”S\Delta S is typically in J/K
  • For ฮ”G=ฮ”Hโˆ’Tฮ”S\Delta G = \Delta H - T\Delta S: convert ฮ”S\Delta S to kJ/K by dividing by 1000

Strategy 4: Entropy of Surroundings

ฮ”Ssurr=โˆ’ฮ”HsysT\Delta S_{\text{surr}} = -\frac{\Delta H_{\text{sys}}}{T}

Mixed Entropy Problems ๐ŸŽฏ

Entropy Calculation Workshop ๐Ÿงฎ

  1. A reaction has ฮ”H=โˆ’150\Delta H = -150 kJ and occurs at T=300T = 300 K. What is ฮ”Ssurroundings\Delta S_{\text{surroundings}}? (in J/K)

  2. The melting of ice at 0ยฐC (273 K) has ฮ”Hfus=6.01\Delta H_{\text{fus}} = 6.01 kJ/mol. What is ฮ”Sfus\Delta S_{\text{fus}}? (in J/(molยทK), to 3 significant figures)

  3. A reaction has ฮ”Ssys=โˆ’100\Delta S_{\text{sys}} = -100 J/K and ฮ”Ssurr=+350\Delta S_{\text{surr}} = +350 J/K. What is ฮ”Suniverse\Delta S_{\text{universe}}? (in J/K)

Entropy Problem Strategies ๐Ÿ”ฝ

Challenge Problem ๐Ÿ†

Exit Quiz โ€” Entropy Workshop โœ…

Part 7: Synthesis & AP Review

๐ŸŽฏ Synthesis & AP Review โ€” Entropy

Part 7 of 7 โ€” Bringing It All Together

This review integrates all entropy concepts: microstates, predicting signs, the Second and Third Laws, calculating ฮ”Sยฐ\Delta Sยฐ, and connecting entropy to spontaneity.

Complete Concept Map

Entropy Fundamentals

ConceptKey Equation/Idea
Boltzmann equationS=kBlnโกWS = k_B \ln W
More microstatesHigher entropy
Phase orderSsolid<Sliquidโ‰ชSgasS_{\text{solid}} < S_{\text{liquid}} \ll S_{\text{gas}}
Third LawS=0S = 0 for perfect crystal at 0 K

Predicting and Calculating ฮ”S

MethodApproach
QualitativeCount ฮ”ngas\Delta n_{\text{gas}}; more gas โ†’ higher S
Quantitativeฮ”Sยฐ=โˆ‘nSยฐ(prod)โˆ’โˆ‘mSยฐ(react)\Delta Sยฐ = \sum n Sยฐ(\text{prod}) - \sum m Sยฐ(\text{react})
Phase transitionฮ”S=ฮ”Htrans/Ttrans\Delta S = \Delta H_{\text{trans}}/T_{\text{trans}}
Surroundingsฮ”Ssurr=โˆ’ฮ”Hsys/T\Delta S_{\text{surr}} = -\Delta H_{\text{sys}}/T

Spontaneity

ฮ”H\Delta Hฮ”S\Delta SSpontaneity
โˆ’+Always spontaneous
+โˆ’Never spontaneous
โˆ’โˆ’Spontaneous at low T
++Spontaneous at high T

Critical Unit Reminder

ฮ”H\Delta H โ†’ kJ, ฮ”S\Delta S โ†’ J/K. Convert before combining!

Comprehensive AP Review Quiz ๐ŸŽฏ

Integration Problems ๐Ÿงฎ

  1. At what temperature does a reaction with ฮ”H=โˆ’90\Delta H = -90 kJ and ฮ”S=โˆ’300\Delta S = -300 J/K become nonspontaneous? (in K)

  2. Calculate ฮ”Suniverse\Delta S_{\text{universe}} for an exothermic reaction with ฮ”H=โˆ’200\Delta H = -200 kJ, ฮ”Ssys=โˆ’50\Delta S_{\text{sys}} = -50 J/K, at T=298T = 298 K. (in J/K, round to nearest whole number)

  3. Is the process in (2) spontaneous? (type "yes" or "no")

Final Concept Review ๐Ÿ”ฝ

Final Exit Quiz โ€” Entropy Mastery โœ