Liquids & Solids

General Chemistry I · Dr. Karmach

build Aug 09 · 11:10 · CC BY-NC-SA 4.0 · OpenStax Chemistry 2e where noted
Dr. Karmach

By the end of this unit, you can…

  • Identify the intermolecular forces present in a substance and rank their relative strength
  • Relate intermolecular-force strength to boiling point and other physical properties
  • Apply the heats of fusion and vaporization to compute the energy of a phase change
  • Read and construct a heating or cooling curve and compute the heat for each segment
Dr. Karmach

Today's route 🗺️

  1. Intermolecular Forces
  2. IMFs & Boiling Point
  3. Heat of a Phase Change
  4. Heating & Cooling Curves
  5. Phase Diagrams
  6. Types of Solids
Dr. Karmach

1 · Intermolecular Forces

Identify which intermolecular forces a substance has and name the strongest one present, keeping these attractions between molecules distinct from the bonds inside them.

Dr. Karmach

Why water beads and geckos climb

Water beads up on a waxed car. A gecko walks up a glass wall. Faint attractions between molecules, far weaker than the bonds inside them, hold and lift.

Dr. Karmach

Forces between molecules, not the bonds within

An intermolecular force is an attraction between separate molecules. It is always weaker than the covalent bond holding one molecule together. Melting and boiling loosen these forces; the bonds inside stay intact.

Dr. Karmach

The four kinds, weakest to strongest

Every substance has London dispersion. Polar molecules add dipole–dipole. An H on N, O, or F adds hydrogen bonding. Dissolved ions give ion–dipole, the strongest.

Dr. Karmach

Dispersion grows with size

London dispersion comes from the electron cloud shifting for an instant. A bigger, heavier cloud shifts more easily, so dispersion strengthens as molar mass rises. Among the nonpolar halogens, it climbs straight down the group.

F₂ · Cl₂ · Br₂ · I₂ — all nonpolar
molar mass 38.00 → 70.90 → 159.80 → 253.80 g/mol · dispersion rises with it
Dr. Karmach

The method

  1. Identify the pieces. Ions in a polar solvent, or molecules? Polar? Any H on N, O, or F?
  2. Name every force present. Dispersion always; dipole–dipole if polar; hydrogen bonding if H–N/O/F; ion–dipole for dissolved ions.
  3. Pick the strongest.
Dr. Karmach

Worked example 1 — methane

CH₄ — carbon bonded to four hydrogens
tetrahedral · four identical C–H bonds · wanted: forces present, and the strongest

Natural gas is mostly methane. Name every intermolecular force it has, then the strongest.

Dr. Karmach

Worked example 1 — solution

CH₄ — carbon bonded to four hydrogens
tetrahedral · four identical C–H bonds

Step 1 · Identify the pieces

Methane is a molecule, not ions in a solvent. Its four C–H bonds sit in a symmetric tetrahedron, so the molecule is nonpolar. No H is bonded to N, O, or F.

Dr. Karmach

Worked example 1 — solution

CH₄ — carbon bonded to four hydrogens
tetrahedral · four identical C–H bonds
Step 1 · Identify the pieces Step 2 · Name every force present
nonpolar · no ionic pieces London dispersion only

Dispersion is present in every substance. Nothing here adds dipole–dipole, hydrogen bonding, or ion–dipole.

Dr. Karmach

Worked example 1 — solution

CH₄ — carbon bonded to four hydrogens
tetrahedral · four identical C–H bonds
Step 1 · Identify the pieces Step 2 · Name every force present
nonpolar · no ionic pieces London dispersion only
Step 3 · Pick the strongest
CH₄ → strongest force: London dispersion
the only force present, so it is also the strongest
Dr. Karmach

Worked example 1 — solution

CH₄ — carbon bonded to four hydrogens
tetrahedral · four identical C–H bonds
Step 1 · Identify the pieces Step 2 · Name every force present
nonpolar · no ionic pieces London dispersion only
Step 3 · Pick the strongest
CH₄ → strongest force: London dispersion
the only force present, so it is also the strongest
A nonpolar molecule with no ions has just one option. Dispersion is the whole story for methane.
Dr. Karmach

Worked example 2 — methanol

CH₃OH — an O–H group on a carbon
polar molecule · wanted: forces present, and the strongest

Methanol is the alcohol in some racing fuels. It is polar, so it has dipole–dipole attraction.

A common first answer: polar, so dipole–dipole is the strongest. Test it against the method.

Dr. Karmach

Worked example 2 — forces present

CH₃OH — an O–H group on a carbon
polar molecule · the H sits directly on O

A common first answer

strongest force = dipole–dipole?
true for a polar molecule with no H on N, O, or F — but methanol has an O–H ✗

Methanol is polar, so dipole–dipole is real. It is not the strongest, because the H bonded to oxygen does more.

Dr. Karmach

Worked example 2 — forces present

CH₃OH — an O–H group on a carbon
polar molecule · the H sits directly on O
A common first answer
strongest force = dipole–dipole?
true for a polar molecule with no H on N, O, or F — but methanol has an O–H ✗
Step 1 · Identify the pieces

A molecule, not ions. Polar. And one H is bonded directly to O — the trigger for hydrogen bonding.

Dr. Karmach

Worked example 2 — forces present

CH₃OH — an O–H group on a carbon
polar molecule · the H sits directly on O
A common first answer
strongest force = dipole–dipole?
true for a polar molecule with no H on N, O, or F — but methanol has an O–H ✗
Step 1 · Identify the pieces Step 2 · Name every force present
dispersion · dipole–dipole · hydrogen bonding (H on O) three forces present
Every molecule has dispersion. Polar adds dipole–dipole; the O–H adds hydrogen bonding on top.
Dr. Karmach

Worked example 2 — the strongest force

CH₃OH — three forces present
dispersion · dipole–dipole · hydrogen bonding (H on O)

Step 3 · Pick the strongest

CH₃OH → strongest force: hydrogen bonding
H–O present · a strong special dipole–dipole, above ordinary dipole–dipole and dispersion
An H on N, O, or F lifts the strongest force from dipole–dipole up to hydrogen bonding.
Dr. Karmach

Take-home: hydrogen bonding needs H on N, O, or F

H₂O · NH₃ · HF — H bonded to O, N, F
hydrogen bonding present · the strongest force in each
H₂S · HCl · CH₄ — H bonded to S, Cl, C
no hydrogen bonding · the H sits on the wrong atom

Hydrogen bonding needs an H bonded directly to nitrogen, oxygen, or fluorine. An H on carbon, sulfur, or chlorine does not qualify, however many H atoms a molecule has.

Dr. Karmach

Your turn — hydrogen sulfide

H₂S — bent, two S–H bonds
polar molecule · sulfur is not N, O, or F
step H₂S
1 · identify the pieces a molecule · polar · H bonded to
2 · name every force dispersion, plus
3 · pick the strongest

Fill the three cells. Watch the atom the H sits on.

Dr. Karmach

Your turn — hydrogen sulfide

H₂S — bent, two S–H bonds
polar molecule · sulfur is not N, O, or F
step H₂S
1 · identify the pieces a molecule · polar · H bonded to
2 · name every force dispersion, plus
3 · pick the strongest

Fill the three cells. Watch the atom the H sits on.

H₂S → strongest force: dipole–dipole
H on sulfur, not N/O/F → no hydrogen bonding · dispersion + dipole–dipole, strongest is dipole–dipole
Dr. Karmach

Where this goes wrong

Naming the covalent bond as the force between molecules. The bonds inside a molecule are intramolecular. They hold one molecule together and do not break when it melts or boils. Intermolecular forces act between molecules; melting and boiling loosen those.
Stopping at dipole–dipole when an H sits on N, O, or F. A polar molecule does have dipole–dipole. But an H bonded to nitrogen, oxygen, or fluorine upgrades the strongest force to hydrogen bonding, the stronger special case.
Defaulting to dispersion and missing the stronger force. Dispersion is in every molecule, but it is the weakest. Scan for an H on N, O, or F first, then for a dipole — the strongest present is the answer, not dispersion by default.
Ranking the forces in the wrong order. The order runs dispersion, dipole–dipole, hydrogen bonding, ion–dipole. Hydrogen bonding is not the strongest of all; ion–dipole outranks it.
Dr. Karmach

Practice 1

hydrogen fluoride, HF
a polar molecule · the single H is bonded to fluorine

What is the strongest intermolecular force present in HF?

  1. Hydrogen bonding — the H is bonded directly to fluorine, one of N, O, F
  2. Ordinary dipole–dipole — HF is polar, so dipole–dipole is as strong as it gets
  3. London dispersion — every molecule has it, so it must be the strongest
  4. The H–F covalent bond — that is the force holding the molecule to its neighbours
Dr. Karmach

Practice 1 — answer: A

HF → strongest force: hydrogen bonding — answer A
H bonded directly to F · a strong special dipole–dipole, the strongest force here

B stopped one rung early: HF is polar, but the H bonded to fluorine upgrades the strongest force to hydrogen bonding, above ordinary dipole–dipole. C defaulted to the weakest force; dispersion is in every molecule but never the strongest when a stronger one is present. D named the H–F bond inside the molecule, which is intramolecular and does not act between molecules.

Scan from the top: an H on F means hydrogen bonding, and the scan stops there.
Dr. Karmach

Worked example 3 — ranking three molecules

propane C₃H₈ · dimethyl ether CH₃OCH₃ · ethanol C₂H₅OH
molar mass ≈ 44, 46, 46 g/mol · wanted: rank by the strongest force each has

Three molecules of nearly equal molar mass. Rank them by the strength of the strongest intermolecular force in each, weakest first.

Dr. Karmach

Worked example 3 — forces present

propane C₃H₈ · dimethyl ether CH₃OCH₃ · ethanol C₂H₅OH
molar mass ≈ 44, 46, 46 g/mol · dispersion is comparable in all three

Step 1 · Identify the pieces

Propane is a nonpolar hydrocarbon. Dimethyl ether is polar, but every H sits on carbon. Ethanol is polar and has an O–H.

Dr. Karmach

Worked example 3 — forces present

propane C₃H₈ · dimethyl ether CH₃OCH₃ · ethanol C₂H₅OH
molar mass ≈ 44, 46, 46 g/mol · dispersion is comparable in all three
Step 1 · Identify the pieces Step 2 · Name every force present
propane → dispersion · ether → + dipole–dipole · ethanol → + hydrogen bonding
Each one has dispersion. The polar ether adds dipole–dipole; ethanol's O–H adds hydrogen bonding on top.
Dr. Karmach

Worked example 3 — the ranking

propane · dimethyl ether · ethanol — same mass range
strongest force: dispersion < dipole–dipole < hydrogen bonding

Step 3 · Pick the strongest

Similar masses, so the strongest-force type sets the order: propane < dimethyl ether < ethanol.
Dr. Karmach

Practice 2

argon (Ar) · hydrogen chloride (HCl) · water (H₂O)
rank by the strongest force in each, weakest first

Argon atoms, HCl molecules, and H₂O molecules. Which ranking orders them by the strength of their strongest intermolecular force, weakest first?

  1. Ar < HCl < H₂O — dispersion only, then dipole–dipole, then hydrogen bonding
  2. HCl < Ar < H₂O — a polar molecule must be weaker than a lone atom
  3. Ar < H₂O < HCl — HCl hydrogen bonds because it contains hydrogen, so it ranks above water
  4. They rank equally — all three attract their neighbours, so the strengths match
Dr. Karmach

Practice 2 — answer: A

Ar < HCl < H₂O — answer A
dispersion only · dipole–dipole · hydrogen bonding · strongest force rises left to right

B put the polar molecule below the lone atom; HCl has dipole–dipole on top of dispersion, so it outranks argon. C claimed HCl hydrogen bonds, but its H sits on chlorine, not on N, O, or F — HCl stops at dipole–dipole and stays below water. D treated one attraction as all the same strength; the type sets the strength, and the three types differ.

Argon has only dispersion, HCl adds dipole–dipole, water reaches hydrogen bonding. The strongest force climbs across the row.
Dr. Karmach

Check yourself

  1. Acetone (CH₃COCH₃) is a polar molecule with no O–H, N–H, or F–H bond. Name every intermolecular force it has, then the strongest.
  2. Two nonpolar gases differ only in size. Which has the stronger dispersion force, and why?

Stronger intermolecular forces hold a liquid together more tightly, so more heat is needed to boil it. Ranking these forces is the first step toward predicting which substance boils at the higher temperature.

Dr. Karmach

2 · IMFs & Boiling Point

Predict which substance boils higher from its intermolecular forces — the stronger the attraction between molecules, the more energy needed to pull them apart, so the higher the boiling point; among nonpolar molecules the bigger one disperses more.

Dr. Karmach

Three liquids off your skin

Rubbing alcohol dries in seconds. Water lingers for minutes. Cooking oil barely leaves at all. Stronger attractions between molecules hold a liquid together longer.

Dr. Karmach

Boiling pulls molecules apart

To boil, molecules must break free of their neighbors, and stronger attractions take more energy to overcome. The stronger the intermolecular forces, the higher the boiling point.

stronger intermolecular forces → higher boiling point
also raises melting point, surface tension, viscosity · lowers vapor pressure
Dr. Karmach

Ranking the forces at equal size

When molecules are about the same size, the type of force sets the order. Hydrogen bonding pulls hardest, ordinary dipole–dipole attraction is weaker, and dispersion is weakest of the three.

at ≈ 44–46 g/mol: ethanol (hydrogen bonding) 78 °C · dimethyl ether (dipole–dipole) −24 °C · propane (dispersion) −42 °C
nearly equal mass, so dispersion is nearly equal — the stronger force type boils higher
Dr. Karmach

Bigger nonpolar molecules boil higher

Nonpolar molecules have only dispersion forces. Dispersion comes from the electrons, so a bigger molecule with more electrons and more surface attracts more strongly. Among nonpolar molecules, the larger boils higher.

Dr. Karmach

The method

  1. Identify each substance's strongest force. Hydrogen bonding, dipole–dipole, or dispersion.
  2. The stronger force boils higher. Across types, rank them: hydrogen bonding > dipole–dipole > dispersion.
  3. For a tie, the bigger molecule attracts more. Same type: more electrons, more surface.
Dr. Karmach

Worked example 1 — same size, different force

dimethyl ether (CH₃OCH₃) vs ethanol (C₂H₅OH)
both C₂H₆O, molar mass 46.07 g/mol · wanted: which boils higher, and why

Two liquids built from the same atoms: the same molar mass, and nearly the same dispersion.

Name the higher-boiling liquid, and the force that explains it.

Dr. Karmach

Worked example 1 — solution

dimethyl ether (CH₃OCH₃) vs ethanol (C₂H₅OH)
both C₂H₆O, 46.07 g/mol

Step 1 · Identify each substance's strongest force

Ethanol has an O–H bond, so it hydrogen bonds. Dimethyl ether is polar but has no O–H, so its strongest force is ordinary dipole–dipole attraction.

Dr. Karmach

Worked example 1 — solution

dimethyl ether (CH₃OCH₃) vs ethanol (C₂H₅OH)
both C₂H₆O, 46.07 g/mol
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher

Equal molar mass means dispersion is the same for both, so only the force type differs. Hydrogen bonding is stronger than dipole–dipole, so ethanol boils higher.

ethanol 78 °C · dimethyl ether −24 °C
hydrogen bonding vs dipole–dipole · same 46.07 g/mol
Dr. Karmach

Worked example 1 — solution

dimethyl ether (CH₃OCH₃) vs ethanol (C₂H₅OH)
both C₂H₆O, 46.07 g/mol
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher
ethanol 78 °C · dimethyl ether −24 °C
hydrogen bonding vs dipole–dipole · same 46.07 g/mol
Identical mass, and hydrogen bonding lifts ethanol's boiling point 102 °C above dimethyl ether's. The force type, not the size, made the difference. ✓
Dr. Karmach

Worked example 2 — two halogens

chlorine (Cl₂) vs iodine (I₂)
Cl₂ 70.90 g/mol · I₂ 253.80 g/mol · both nonpolar · wanted: which boils higher, and why

A common first answer: both are nonpolar molecules with only dispersion forces, so they should boil at about the same temperature.

Name the higher-boiling halogen, and the reason.

Dr. Karmach

Worked example 2 — solution

chlorine (Cl₂) vs iodine (I₂)
Cl₂ 70.90 g/mol · I₂ 253.80 g/mol · both nonpolar

Step 1 · Identify each substance's strongest force

Both are nonpolar, so dispersion is the only force acting in each.

Dr. Karmach

Worked example 2 — solution

chlorine (Cl₂) vs iodine (I₂)
Cl₂ 70.90 g/mol · I₂ 253.80 g/mol · both nonpolar
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher

Same force type does not mean same strength. The molecule held by stronger dispersion boils higher.

Dr. Karmach

Worked example 2 — solution

chlorine (Cl₂) vs iodine (I₂)
Cl₂ 70.90 g/mol · I₂ 253.80 g/mol · both nonpolar
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher Step 3 · For a tie, the bigger molecule attracts more

Iodine is far larger than chlorine, with many more electrons, so its dispersion is much stronger. Iodine boils higher.

iodine 184 °C · chlorine −34 °C
253.80 g/mol vs 70.90 g/mol · dispersion grows with size
Dr. Karmach

Worked example 2 — solution

chlorine (Cl₂) vs iodine (I₂)
Cl₂ 70.90 g/mol · I₂ 253.80 g/mol · both nonpolar
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher Step 3 · For a tie, the bigger molecule attracts more
iodine 184 °C · chlorine −34 °C
253.80 g/mol vs 70.90 g/mol · dispersion grows with size
Iodine boils 218 °C above chlorine, and at room temperature iodine is a solid while chlorine is a gas. Same force type, very different strength. ✓
Dr. Karmach

Take-home: type outranks mass

Size decides only among one force type. Across types, the stronger force wins against a far heavier molecule. Tin hydride is nearly seven times water's mass, yet water boils higher because water hydrogen bonds.

Dr. Karmach

Your turn — methanol and ethane

methanol (CH₃OH) 32.04 g/mol · ethane (C₂H₆) 30.07 g/mol
nearly equal mass, so dispersion is nearly equal
methanol: strongest force = · ethane: strongest force = · higher boiling point:

Fill each strongest force, then name the higher-boiling liquid.

Dr. Karmach

Your turn — methanol and ethane

methanol (CH₃OH) 32.04 g/mol · ethane (C₂H₆) 30.07 g/mol
nearly equal mass, so dispersion is nearly equal
methanol: strongest force = · ethane: strongest force = · higher boiling point:

Fill each strongest force, then name the higher-boiling liquid.

methanol: hydrogen bonding (O–H) · ethane: dispersion (nonpolar) · higher boiling point: methanol
Equal mass, so dispersion ties. Methanol's O–H adds hydrogen bonding, and it boils at 65 °C against ethane's −89 °C, 154 °C higher. ✓
Dr. Karmach

Where this goes wrong

Heavier always boils higher. Mass alone does not decide. Water, 18.02 g/mol, boils at 100 °C, above butane at 58.12 g/mol (−0.5 °C), because water hydrogen bonds while butane has only dispersion. Rank by force first; size counts only within one type.
Reversing the trend. "Lighter molecules move faster, so they need a higher temperature to boil." Weakly held molecules escape more easily, not less. Weak forces mean a low boiling point; strong forces mean a high one.
Confusing forces with bonds. "The bigger molecule boils higher because its covalent bonds are stronger." Boiling never breaks the covalent bonds inside a molecule. It overcomes the attractions between whole molecules, which are far weaker than bonds.
Same type, same boiling point. Two nonpolar molecules share the dispersion force but not its strength. Dispersion grows with size, so iodine (253.80 g/mol) boils far above chlorine (70.90 g/mol).
Dr. Karmach

Practice 1

pentane (C₅H₁₂) vs heptane (C₇H₁₆)
pentane 72.15 g/mol · heptane 100.20 g/mol · both nonpolar

Pentane and heptane are both nonpolar. Which boils at the higher temperature, and why?

  1. Heptane — it is the larger molecule, so its dispersion forces are stronger and take more energy to overcome.
  2. Heptane — its covalent bonds are stronger and must be broken for it to boil.
  3. Pentane — lighter molecules move faster, so a higher temperature is needed to boil them off.
  4. They boil at nearly the same temperature, since both are nonpolar and rely on the same force.
Dr. Karmach

Practice 1 — answer: A

pentane (C₅H₁₂) vs heptane (C₇H₁₆)
pentane 72.15 g/mol · heptane 100.20 g/mol · both nonpolar — dispersion only

Both are nonpolar, so dispersion is the only force. Heptane is the larger molecule, so its dispersion is stronger and it boils higher — answer A.

B confused forces with bonds: boiling overcomes the attractions between molecules, never the covalent bonds inside them. C reversed the trend: weakly held light molecules escape more easily and boil lower, not higher. D forgot that the same force type can differ in strength, and dispersion grows with size.

Heptane boils at 98 °C, pentane at 36 °C, 62 °C higher for the larger molecule. ✓
Dr. Karmach

Worked example 3 — rank three by boiling point

butane (C₄H₁₀) · acetone (C₃H₆O) · 1-propanol (C₃H₈O)
58.12 · 58.08 · 60.09 g/mol · nearly equal mass · wanted: order the boiling points

Three liquids of nearly equal molar mass, so dispersion is about the same for all three.

Rank the three boiling points from lowest to highest.

Dr. Karmach

Worked example 3 — solution

butane (C₄H₁₀) · acetone (C₃H₆O) · 1-propanol (C₃H₈O)
58.12 · 58.08 · 60.09 g/mol · nearly equal mass

Step 1 · Identify each substance's strongest force

Butane is nonpolar: dispersion only. Acetone is polar with no O–H: dipole–dipole. 1-Propanol has an O–H: hydrogen bonding.

Dr. Karmach

Worked example 3 — solution

butane (C₄H₁₀) · acetone (C₃H₆O) · 1-propanol (C₃H₈O)
58.12 · 58.08 · 60.09 g/mol · nearly equal mass
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher

Mass is nearly equal, so dispersion ties and the force type sets the order. Hydrogen bonding beats dipole–dipole beats dispersion, so 1-propanol > acetone > butane.

butane −0.5 °C · acetone 56 °C · 1-propanol 97 °C
dispersion < dipole–dipole < hydrogen bonding · masses within 2 g/mol
Dr. Karmach

Worked example 3 — solution

butane (C₄H₁₀) · acetone (C₃H₆O) · 1-propanol (C₃H₈O)
58.12 · 58.08 · 60.09 g/mol · nearly equal mass
Step 1 · Identify each substance's strongest force Step 2 · The stronger force boils higher
butane −0.5 °C · acetone 56 °C · 1-propanol 97 °C
dispersion < dipole–dipole < hydrogen bonding · masses within 2 g/mol
Lowest to highest: butane −0.5 °C, acetone 56 °C, 1-propanol 97 °C. Propanol boils 41 °C above acetone on hydrogen bonding alone, at nearly the same mass. ✓
Dr. Karmach

Practice 2

water (H₂O) vs hydrogen sulfide (H₂S)
H₂O 18.02 g/mol · H₂S 34.08 g/mol · both bent, polar molecules

Water and hydrogen sulfide are both bent and polar, and hydrogen sulfide is the heavier molecule. Which boils at the higher temperature, and why?

  1. Water — its O–H bonds let it hydrogen bond, a stronger attraction than the dipole–dipole forces in hydrogen sulfide.
  2. Hydrogen sulfide — it is the heavier molecule, so it boils at the higher temperature.
  3. Water — its covalent O–H bonds are stronger and take more energy to break.
  4. They boil at nearly the same temperature, since both are bent, polar molecules.
Dr. Karmach

Practice 2 — answer: A

water (H₂O) vs hydrogen sulfide (H₂S)
H₂O 18.02 g/mol · H₂S 34.08 g/mol · both polar

Water's O–H bonds let it hydrogen bond. Hydrogen sulfide has no H on a small, strongly electron-attracting atom, so it is held only by weaker dipole–dipole forces. Water boils higher — answer A.

B ranked by mass alone: hydrogen sulfide is heavier, but its forces are weaker, so it boils lower. C confused forces with bonds: boiling overcomes the attractions between molecules, not the covalent O–H bonds inside them. D treated the same force type as the same strength, when hydrogen bonding is a much stronger special case.

Water boils at 100 °C, hydrogen sulfide at −60 °C — a 160 °C gap in favor of the lighter, hydrogen-bonding molecule. ✓
Dr. Karmach

Check yourself

  1. Neon and argon are both nonpolar. Which boils at the higher temperature, and which force decides it?
  2. Dimethyl ether and ethanol have the same molar mass. Which boils higher, and why?

Reaching the boiling point is only the start. Turning a liquid into vapor at that temperature takes a fixed amount of energy for every gram: the heat of vaporization.

Dr. Karmach

3 · Heat of a Phase Change

Find the heat of a phase change with q = mass × ΔH, choosing the heat of fusion for melting or freezing and the heat of vaporization for boiling or condensing, while the temperature holds constant.

Dr. Karmach

Heat flows, the temperature holds

A glass of ice water stays at 0 °C until the last cube melts. Sweat cools your skin. Heat moves in or out; the temperature holds.

Dr. Karmach

Temperature holds during a phase change

A phase change runs at one temperature. The heat does not warm the sample; it pulls the molecules apart. Ice water holds at 0 °C until the last cube melts.

Dr. Karmach

Heat of fusion and heat of vaporization

for water — ΔHfus = 335 J/g · ΔHvap = 2259 J/g
melt or freeze: 335 J per gram · boil or condense: 2259 J per gram

Melting is called fusion. The heat of fusion, ΔHfus, melts one gram; the heat of vaporization, ΔHvap, boils one gram. Freezing and condensing release the same amounts, reversed.

Dr. Karmach

Vaporizing costs more than melting

ΔHvap is far larger than ΔHfus. Melting only loosens the packing; the molecules still touch. Vaporizing pulls them fully apart, which takes about seven times the energy.

Dr. Karmach

The phase-change heat equation

q = mass × ΔH
g × (J/g) = J · absorbed (+) to melt or boil · released (−) to freeze or condense

Each heat is a conversion factor in joules per gram. Multiply by the mass and grams cancel. Melting and boiling absorb heat; freezing and condensing release it, so q turns negative.

Dr. Karmach

The method

  1. Name the phase change.
  2. Pick its ΔH: fusion to melt or freeze, vaporization to boil or condense.
  3. Multiply: q = mass × ΔH. Grams cancel.
  4. Set the direction: melting and boiling absorb; freezing and condensing release.
Dr. Karmach

Worked example 1 — melt ice

q = mass × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q

A tray holds 60.0 g of ice at 0 °C. How much heat melts it completely? (ΔHfus of water: 335 J/g)

Name the change of state, then pick its heat.

Dr. Karmach

Worked example 1 — solution

q = mass × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q

Step 1 · Name the phase change

The ice is melting: solid water turns to liquid, all at 0 °C.

Dr. Karmach

Worked example 1 — solution

q = mass × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q
Step 1 · Name the phase change Step 2 · Pick its ΔH

Melting uses the heat of fusion, ΔHfus = 335 J/g.

Dr. Karmach

Worked example 1 — solution

q = mass × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q
Step 1 · Name the phase change Step 2 · Pick its ΔH Step 3 · Multiply

Write the factor so grams cancel. Only one orientation does:

335 J1 g cancels grams ✓    1 g335 J cancels nothing ✗
60.0 g × 335 J1 g = 20,100 J
Dr. Karmach

Worked example 1 — solution

q = mass × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q
Step 1 · Name the phase change Step 2 · Pick its ΔH Step 3 · Multiply
60.0 g × 335 J1 g = 20,100 J
Step 4 · Set the direction
Melting absorbs heat, so q is positive: 20,100 J (20.1 kJ) go in, and the temperature never leaves 0 °C. ✓
Dr. Karmach

Worked example 2 — boil water to steam

q = mass × ΔHvap
given: 20.0 g water at 100 °C · ΔHvap = 2259 J/g · wanted: q

20.0 g of water at 100 °C boils away to steam. How much heat does it take? (ΔHvap of water: 2259 J/g)

Same route as melting, with the vaporization heat.

Dr. Karmach

Worked example 2 — solution

q = mass × ΔHvap
given: 20.0 g water at 100 °C · ΔHvap = 2259 J/g · wanted: q

Step 1 · Name the phase change

The water is boiling: liquid turns to gas, all at 100 °C.

Dr. Karmach

Worked example 2 — solution

q = mass × ΔHvap
given: 20.0 g water at 100 °C · ΔHvap = 2259 J/g · wanted: q
Step 1 · Name the phase change Step 2 · Pick its ΔH

Boiling uses the heat of vaporization, ΔHvap = 2259 J/g.

Dr. Karmach

Worked example 2 — solution

q = mass × ΔHvap
given: 20.0 g water at 100 °C · ΔHvap = 2259 J/g · wanted: q
Step 1 · Name the phase change Step 2 · Pick its ΔH Step 3 · Multiply
20.0 g × 2259 J1 g = 45,180 J

Grams cancel; joules remain.

Dr. Karmach

Worked example 2 — solution

q = mass × ΔHvap
given: 20.0 g water at 100 °C · ΔHvap = 2259 J/g · wanted: q
Step 1 · Name the phase change Step 2 · Pick its ΔH Step 3 · Multiply
20.0 g × 2259 J1 g = 45,180 J
Step 4 · Set the direction
Boiling absorbs heat: q = +45,180 J (45.2 kJ). Same 20.0 g would take only 6,700 J to melt — vaporizing costs far more. ✓
Dr. Karmach

Your turn — melt more ice

q = mass × ΔHfus
given: 40.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q

40.0 g of ice at 0 °C melts to water. Fill in the heat of fusion, then compute.

40.0 g × J1 g = J
Dr. Karmach

Your turn — melt more ice

q = mass × ΔHfus
given: 40.0 g ice at 0 °C · ΔHfus = 335 J/g · wanted: q

40.0 g of ice at 0 °C melts to water. Fill in the heat of fusion, then compute.

40.0 g × J1 g = J
40.0 g × 335 J1 g = 13,400 J
335 J melts one gram, so 40.0 g take 40.0 × 335 = 13,400 J (13.4 kJ), all at 0 °C. ✓
Dr. Karmach

Where this goes wrong

q = mass × ΔHfus
60.0 g ice at 0 °C · ΔHfus = 335 J/g · correct q = 20,100 J
Leaving out the mass. 335 J melts a single gram. The sample has 60.0 of them. Scale it up: 60.0 g × 335 J/g = 20,100 J.
Dividing by the heat of fusion. 60.0 ÷ 335 = 0.179, in units of g²/J. Nothing cancels. Write the factor so grams cancel: 60.0 g × (335 J / 1 g).
Reporting kilojoules as joules. 60.0 × 335 = 20,100, then sliding the decimal gives 20.1. That is the value in kilojoules. In joules it is 20,100 J.
Using the vaporization heat to melt. Melting uses ΔHfus = 335 J/g, not ΔHvap = 2259 J/g. 60.0 × 2259 = 135,540 J is the heat to boil the water, not melt the ice.
Dr. Karmach

Practice 1

q = mass × ΔHvap
given: 18.0 g water at 100 °C · ΔHvap = 2259 J/g · wanted: q

18.0 g of water at 100 °C boils to steam. How much heat does it take? (ΔHvap of water: 2259 J/g)

  1. 6030 J
  2. 40662 J
  3. 2259 J
  4. 40.7 J
Dr. Karmach

Practice 1 — answer: B

q = mass × ΔHvap
given: 18.0 g water at 100 °C · ΔHvap = 2259 J/g
18.0 g × 2259 J1 g = 40,662 J — answer B

A used the heat of fusion by mistake: 18.0 × 335 = 6,030 J is the heat to melt, not boil. C left out the mass: 2,259 J boils one gram only. D slid the decimal: 18.0 × 2259 = 40,662, then divided by 1000 to get 40.7 and mislabeled it joules.

Boiling 18.0 g takes about 40,000 J, roughly seven times what melting the same mass would cost. ✓
Dr. Karmach

Worked example 3 — a steam burn

q = mass × ΔHvap
given: 8.00 g steam at 100 °C → water at 100 °C · ΔHvap = 2259 J/g · wanted: heat released

8.00 g of steam at 100 °C condenses on skin and releases heat. This is why a steam burn is so severe. How much heat comes out?

A common first attempt: add a q = mass × c × ΔT term for the temperature. Test it.

Dr. Karmach

Worked example 3 — solution

q = mass × ΔHvap
8.00 g steam · condenses at 100 °C → water at 100 °C · wanted: heat released

A common first attempt

m·c·ΔT = 8.00 g × 4.184 J/g·°C × (100 − 100) °C = 0 J

The steam condenses at 100 °C into water at 100 °C. ΔT = 0, so the m·c·ΔT term adds nothing.

Dr. Karmach

Worked example 3 — solution

q = mass × ΔHvap
8.00 g steam · condenses at 100 °C → water at 100 °C · wanted: heat released

A common first attempt

m·c·ΔT = 8.00 g × 4.184 J/g·°C × (100 − 100) °C = 0 J

The steam condenses at 100 °C into water at 100 °C. ΔT = 0, so the m·c·ΔT term adds nothing.
Step 1 · Name the phase change

The steam is condensing: gas turns to liquid, all at 100 °C.

Dr. Karmach

Worked example 3 — solution

q = mass × ΔHvap
8.00 g steam · condenses at 100 °C → water at 100 °C · wanted: heat released

A common first attempt

m·c·ΔT = 8.00 g × 4.184 J/g·°C × (100 − 100) °C = 0 J

The steam condenses at 100 °C into water at 100 °C. ΔT = 0, so the m·c·ΔT term adds nothing.
Step 1 · Name the phase change
Step 2 · Pick its ΔH

Condensing uses the heat of vaporization, ΔHvap = 2259 J/g, the same value as boiling.

No temperature change means no m·c·ΔT term. The phase-change heat is the whole answer. ✓
Dr. Karmach

Worked example 3 — heat released

q = mass × ΔHvap
8.00 g steam condensing at 100 °C · ΔHvap = 2259 J/g

Step 3 · Multiply

8.00 g × 2259 J1 g = 18,072 J
Dr. Karmach

Worked example 3 — heat released

q = mass × ΔHvap
8.00 g steam condensing at 100 °C · ΔHvap = 2259 J/g
Step 3 · Multiply
8.00 g × 2259 J1 g = 18,072 J
Step 4 · Set the direction

Heat leaves the steam as it condenses, so q is negative: q = −18,072 J.

Condensing just 8.00 g of steam dumps 18,072 J (18.1 kJ) into the skin, all at 100 °C before the water even starts to cool. That is why steam burns are severe. ✓
Dr. Karmach

Take-home: a phase change has no ΔT

temperature changes, one phase: q = m · c · ΔT
warming or cooling within a solid, liquid, or gas
temperature constant, changing phase: q = mass × ΔH
melting, freezing, boiling, condensing. ΔT = 0, so no m·c·ΔT term

During a phase change the temperature holds, so ΔT = 0 and the m·c·ΔT term is zero. Use ΔH alone. The two never combine within one phase change.

Dr. Karmach

Practice 2

q = mass × ΔHfus
given: 30.0 g water at 0 °C freezes to ice · ΔHfus = 335 J/g · wanted: q

30.0 g of water at 0 °C freezes to ice. What is q for the water? (ΔHfus of water: 335 J/g)

  1. 67770 J
  2. -10050 J
  3. 10050 J
  4. 335 J
Dr. Karmach

Practice 2 — answer: B

q = mass × ΔHfus
given: 30.0 g water freezing at 0 °C · ΔHfus = 335 J/g
q = − 30.0 g × 335 J1 g = −10,050 J — answer B

A used the heat of vaporization: 30.0 × 2259 = 67,770 J is the heat to condense steam, not freeze water. C has the right size but the wrong sign: freezing releases heat, so q is negative. D left out the mass: 335 J freezes one gram only.

Freezing is the reverse of melting. It releases the same 335 J per gram that melting absorbs, so q is negative. ✓
Dr. Karmach

Check yourself

  1. A block of ice at 0 °C melts to water at 0 °C. What happens to the temperature while it melts, and where does the heat go?
  2. Which is larger for water, the heat of fusion or the heat of vaporization, and why?

Melting and boiling are the flat steps of a heating curve. Between those steps the temperature climbs, and there q = m·c·ΔT takes over. The full curve chains both kinds of heat, segment by segment.

Dr. Karmach

4 · Heating & Cooling Curves

Break a heating path into segments, use q = m·c·ΔT for each slope and the phase-change energy for each plateau, and add them for the total heat.

Dr. Karmach

From the freezer to a rolling boil

Heat a block of ice steadily. Temperature climbs, holds at 0 °C while it melts, climbs, then holds at 100 °C while it boils.

Dr. Karmach

Warming and phase changes alternate

Heating a substance alternates between warming one phase (a sloped step, q = m·c·ΔT) and changing the phase (a flat step, phase-change energy). The total heat is the sum of every step.

Dr. Karmach

Two kinds of segment, two equations

sloped segment — one phase warming
q = m · c · ΔT · uses that phase's specific heat c
flat plateau — a phase change at constant T
q = m · ΔH · the temperature does not move, so there is no ΔT

Read the graph one segment at a time. A slope warms a single phase. A plateau holds the temperature fixed while the phase changes. Each segment needs its own equation.

Dr. Karmach

Water's constants for each segment

slopes — q = m · c · ΔT
c(ice) = 2.09 · c(liquid water) = 4.184 · c(steam) = 2.03 J/g·°C
plateaus — q = m · ΔH
ΔHfus = 335 J/g at 0 °C · ΔHvap = 2259 J/g at 100 °C

Each phase carries its own specific heat. Each phase change carries its own energy. Liquid water's 4.184 J/g·°C does not apply to ice or steam.

Dr. Karmach

The method

  1. Identify each segment. Each slope and each plateau is one piece.
  2. Compute each piece. A slope uses q = m·c·ΔT with that phase's c. A plateau uses the phase-change energy, ΔHfus or ΔHvap.
  3. Add every piece for the total.
Dr. Karmach

Worked example 1 — ice at 0 °C to warm water

total q = melt + warm
given: 30 g ice at 0 °C → liquid water at 25 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C · wanted: q

A 30 g block of ice, already at 0 °C, is heated until it becomes liquid water at 25 °C. How much heat does it take?

Identify each segment, then add the pieces.

Dr. Karmach

Worked example 1 — solution

total q = melt + warm
given: 30 g ice at 0 °C → liquid water at 25 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C

Step 1 · Identify each segment

The ice sits at its melting point. Two pieces follow: melt at a constant 0 °C, then warm the liquid to 25 °C.

Dr. Karmach

Worked example 1 — solution

total q = melt + warm
given: 30 g ice at 0 °C → liquid water at 25 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
Step 1 · Identify each segment Step 2 · Compute each piece
melt: 30 g × 335 J1 g = 10,050 J · warm: 30 g × 4.184 J1 g·°C × 25 °C = 3138 J
Dr. Karmach

Worked example 1 — solution

total q = melt + warm
given: 30 g ice at 0 °C → liquid water at 25 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
Step 1 · Identify each segment Step 2 · Compute each piece
melt: 30 g × 335 J1 g = 10,050 J · warm: 30 g × 4.184 J1 g·°C × 25 °C = 3138 J
Step 3 · Add every piece
q = 10,050 J + 3138 J = 13,188 J
Melting alone costs 10,050 J, more than warming the liquid 25 °C. The flat step costs more. ✓
Dr. Karmach

Worked example 2 — melt, then warm to 40 °C

total q = melt + warm
given: 45 g ice at 0 °C → liquid water at 40 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C · wanted: q

A 45 g block of ice at 0 °C is melted and then warmed to 40 °C.

A common first attempt: the sample ends 40 °C warmer, so multiply the melting heat by 40 as well. Test it.

Dr. Karmach

Worked example 2 — the melting step

total q = melt + warm
given: 45 g ice at 0 °C → liquid water at 40 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C

A common first attempt

melt: 45 g × 335 J1 g × 40 °C = 603,000 J ✗

Melting happens at a constant 0 °C. There is no temperature change to multiply, so ΔHfus already gives the whole melting heat.

Dr. Karmach

Worked example 2 — the melting step

total q = melt + warm
given: 45 g ice at 0 °C → liquid water at 40 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
A common first attempt
melt: 45 g × 335 J1 g × 40 °C = 603,000 J ✗
Step 1 · Identify each segment

Two pieces: melt at 0 °C, then warm the liquid from 0 °C to 40 °C. Only the warming piece has a ΔT.

The melting step holds at 0 °C, so it carries no temperature change. Only the warming step does. ✓
Dr. Karmach

Worked example 2 — the two pieces

total q = melt + warm
given: 45 g ice at 0 °C → liquid water at 40 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C

Step 2 · Compute each piece

melt: 45 g × 335 J1 g = 15,075 J · warm: 45 g × 4.184 J1 g·°C × 40 °C = 7531.2 J
Dr. Karmach

Worked example 2 — the two pieces

total q = melt + warm
given: 45 g ice at 0 °C → liquid water at 40 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
Step 2 · Compute each piece
melt: 45 g × 335 J1 g = 15,075 J · warm: 45 g × 4.184 J1 g·°C × 40 °C = 7531.2 J
Step 3 · Add every piece
q = 15,075 J + 7531.2 J = 22,606 J
The two pieces add to 22,606 J. The signless shortcut, 603,000 J, was nearly thirty times too large. ✓
Dr. Karmach

Take-home: a plateau is not q = m·c·ΔT

melt at 0 °C — correct
q = m · ΔHfus = 45 g × 335 J/g = 15,075 J · temperature stays 0 °C
treating the plateau as q = m·c·ΔT — wrong
45 g × 335 J/g × 40 °C = 603,000 J ✗ · there is no ΔT on a plateau

On a flat plateau the temperature is constant, so ΔT is zero. The heat comes from ΔHfus or ΔHvap. A phase-change energy is never multiplied by a temperature change.

Dr. Karmach

Worked example 3 — ice at −20 °C to steam at 120 °C

total q = warm ice + melt + warm water + boil + warm steam
given: 20 g · −20 °C → 120 °C · c(ice) 2.09 · c(water) 4.184 · c(steam) 2.03 J/g·°C · ΔHfus 335 · ΔHvap 2259 J/g · wanted: q

A 20 g sample starts as ice at −20 °C and ends as steam at 120 °C.

Count the segments between the start and end, then compute and add each one.

Dr. Karmach

Worked example 3 — warming and melting

total q = warm ice + melt + warm water + boil + warm steam
20 g · −20 °C → 120 °C · five segments to cross

Step 1 · Identify each segment

Five pieces: warm ice (−20 → 0), melt at 0 °C, warm water (0 → 100), boil at 100 °C, warm steam (100 → 120). Three slopes and two plateaus.

Dr. Karmach

Worked example 3 — warming and melting

total q = warm ice + melt + warm water + boil + warm steam
20 g · −20 °C → 120 °C · five segments to cross
Step 1 · Identify each segment Step 2 · Compute each piece
warm ice: 20 g × 2.09 J1 g·°C × 20 °C = 836 J · melt: 20 g × 335 J1 g = 6700 J
warm water: 20 g × 4.184 J1 g·°C × 100 °C = 8368 J
Each slope uses its own phase's c: ice 2.09, water 4.184. The plateaus still to come cost more. ✓
Dr. Karmach

Worked example 3 — boiling, then the total

total q = warm ice + melt + warm water + boil + warm steam
warm ice 836 · melt 6700 · warm water 8368 J so far

Step 2 · Compute each piece

boil: 20 g × 2259 J1 g = 45,180 J · warm steam: 20 g × 2.03 J1 g·°C × 20 °C = 812 J
Dr. Karmach

Worked example 3 — boiling, then the total

total q = warm ice + melt + warm water + boil + warm steam
warm ice 836 · melt 6700 · warm water 8368 J so far
Step 2 · Compute each piece
boil: 20 g × 2259 J1 g = 45,180 J · warm steam: 20 g × 2.03 J1 g·°C × 20 °C = 812 J
Step 3 · Add every piece
q = 836 + 6700 + 8368 + 45,180 + 812 = 61,896 J
Boiling alone is 45,180 J, about three-quarters of the total. Vaporizing water takes the most heat. ✓
Dr. Karmach

Your turn — 15 g of ice to warm water

total q = melt + warm
given: 15 g ice at 0 °C → liquid water at 50 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
melt: 15 g × ( J / 1 g) = J · warm: 15 g × 4.184 J/(g·°C) × °C = 3138 J

Fill in ΔHfus, the melt heat, and the temperature change, then add the two pieces.

Dr. Karmach

Your turn — 15 g of ice to warm water

total q = melt + warm
given: 15 g ice at 0 °C → liquid water at 50 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
melt: 15 g × ( J / 1 g) = J · warm: 15 g × 4.184 J/(g·°C) × °C = 3138 J

Fill in ΔHfus, the melt heat, and the temperature change, then add the two pieces.

melt: 15 g × (335 J / 1 g) = 5025 J · warm: 15 g × 4.184 J/(g·°C) × 50 °C = 3138 J
total = 5025 J + 3138 J = 8163 J
The melt costs 5025 J, more than warming the liquid all the way to 50 °C. Melting is the larger step. ✓
Dr. Karmach

Where this goes wrong

reference: 30 g ice at 0 °C → liquid water at 25 °C
melt 10,050 J + warm 3138 J = 13,188 J · ΔHfus 335 · c(ice) 2.09 · c(water) 4.184 J/g·°C
Treating a plateau as q = m·c·ΔT. Multiplying the fusion heat by a ΔT, 45 g × 335 J/g × 40 °C = 603,000 J, invents heat. Melting holds at 0 °C, so 45 g × 335 J/g = 15,075 J, no ΔT.
Skipping the melting plateau. Warming the liquid only, 30 g × 4.184 J/g·°C × 25 °C = 3138 J, leaves the ice unmelted. Melting first costs another 10,050 J.
Stopping at the melting point. 30 g × 335 J/g = 10,050 J melts the ice but leaves it at 0 °C. Warming to 25 °C adds 3138 J.
Using the wrong phase's specific heat. Warming ice with water's 4.184, 20 g × 4.184 × 20 °C = 1673.6 J, overcharges it. Ice's c is 2.09: 20 g × 2.09 × 20 °C = 836 J.
Dr. Karmach

Practice 1

total q = melt + warm
given: 20 g ice at 0 °C → liquid water at 30 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C · wanted: q

A 20 g block of ice at 0 °C is melted and warmed to 30 °C. How much heat does it take?

  1. 2510 J
  2. 6700 J
  3. 9210 J
  4. 201000 J
Dr. Karmach

Practice 1 — answer: C

total q = melt + warm
given: 20 g ice at 0 °C → liquid water at 30 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
melt: 20 g × (335 J / 1 g) = 6700 J · warm: 20 g × 4.184 J/(g·°C) × 30 °C = 2510 J
q = 6700 J + 2510 J = 9210 J — answer C

A skipped the melting plateau: 20 × 4.184 × 30 = 2510 J warms the liquid but never melts the ice. B stopped at the melting point: 20 × 335 = 6700 J leaves the water at 0 °C. D treated fusion like a specific heat: 20 × 335 × 30 = 201,000 J, multiplying a plateau by a ΔT it does not have.

Melting the ice and warming the water are two separate costs. Add both: 6700 J + 2510 J = 9210 J. ✓
Dr. Karmach

Practice 2

total q = warm ice + melt + warm water
given: 25 g ice at −16 °C → liquid water at 20 °C · c(ice) 2.09 · c(water) 4.184 J/g·°C · ΔHfus 335 J/g · wanted: q

A 25 g block of ice at −16 °C is heated to liquid water at 20 °C. How much heat does it take? Three segments: warm the ice, melt it, warm the water.

  1. 2928 J
  2. 9211 J
  3. 11303 J
  4. 12141 J
Dr. Karmach

Practice 2 — answer: C

total q = warm ice + melt + warm water
given: 25 g · −16 °C → 20 °C · c(ice) 2.09 · c(water) 4.184 J/g·°C · ΔHfus 335 J/g
warm ice: 25 g × 2.09 × 16 °C = 836 J · melt: 25 g × 335 J/g = 8375 J · warm water: 25 g × 4.184 × 20 °C = 2092 J
q = 836 J + 8375 J + 2092 J = 11,303 J — answer C

A skipped the melting plateau: 836 + 2092 = 2928 J never melts the ice. B stopped at the melting point: 836 + 8375 = 9211 J leaves the water at 0 °C. D used water's c for the ice: 25 × 4.184 × 16 = 1674 J for the ice leg gives 12,141 J.

Each phase warms with its own c, and the melt at 0 °C is its own step. Three costs, added: 11,303 J. ✓
Dr. Karmach

Check yourself

  1. A path crosses a flat plateau, then a rising slope. Which equation does each part use? Why does the plateau carry no ΔT?
  2. Water at 100 °C and steam at 100 °C are the same temperature. Why does boiling the water still take heat?

Dissolving moves heat too. When a solute dissolves, heat flows in or out, and that heat of solution is read the same way: q = m·c·ΔT from the temperature change of the surrounding water.

Dr. Karmach

5 · Phase Diagrams

Read a pressure–temperature phase diagram — name the stable phase at any P,T, follow a constant-pressure or constant-temperature path and list the phase changes, and locate the triple point, critical point, and the normal melting and boiling points on the 1-atm line.

Dr. Karmach

One map for all three states

Water can be ice, liquid, or steam. A phase diagram is the single map that says which one you get — for any pressure and temperature you choose.

Dr. Karmach

A phase diagram maps pressure vs temperature

A phase diagram plots pressure (y) against temperature (x) for one pure substance. Every point on the map is a P,T pair, and the diagram tells you which phase — solid, liquid, or gas — is stable there.

pick a pressure and a temperature → read off the stable phase
x-axis = Temperature · y-axis = Pressure · each point names one phase of one pure substance

To use it, find your temperature along the bottom and your pressure up the side, then see which region that point lands in.

Dr. Karmach

Three regions, three dividing curves

The map has three regions — solid, liquid, gas — separated by three curves. Each curve is a boundary where two phases are in balance, so crossing a curve is a phase change: the fusion (melting) curve splits solid from liquid, the vaporization curve splits liquid from gas, and the sublimation curve splits solid from gas.

Dr. Karmach

Two special points

triple point — the one P,T where solid, liquid, and gas all coexist
the single spot where all three curves meet
critical point (Tc, Pc) — the top end of the vaporization curve
beyond it the liquid–gas boundary disappears → a supercritical fluid, neither true liquid nor gas

Past the critical temperature you cannot condense a gas into a liquid by squeezing, no matter how hard — the distinction is simply gone.

Dr. Karmach

The 1-atm line gives the normal points

Draw a horizontal line at 1 atm (constant pressure) and slide across it. Where it crosses the fusion curve is the normal melting point; where it crosses the vaporization curve is the normal boiling point — the everyday melting and boiling points measured in open air.

a horizontal path = constant pressure · a vertical path = constant temperature
follow the path and list every curve you cross — each crossing is one phase change

For water at 1 atm that is 0 °C and 100 °C.

Dr. Karmach

The solid–liquid slope: water breaks the rule

Usually the fusion curve slopes up-and-right (solid denser than liquid). Water leans up-and-left (negative slope) — ice is less dense than water. CO₂'s triple point is 5.1 atm, above 1 atm, so at 1 atm it never melts: dry ice sublimes.

Dr. Karmach

Reading a phase diagram

  1. Find the point. Locate the temperature on the x-axis and the pressure on the y-axis; the region it lands in names the stable phase.
  2. Choose the path. A constant-pressure change is horizontal; a constant-temperature change is vertical.
  3. Cross the curves. Each curve your path crosses is one phase change — name it from the two regions on either side.
  4. Check the specials. The triple point is where all three meet; past the critical point there is no liquid–gas line to cross.
Dr. Karmach

Worked example — heat a solid at constant pressure

start: solid, at a pressure just above the triple-point pressure
given: a pure substance with a normal (positive-slope) fusion curve · path: heat at constant pressure, left to right · wanted: the phases crossed

Point A sits in the solid region at low temperature, at a pressure a little above the triple point. Heat it at constant pressure until it is well past its boiling point. List the phases it passes through.

Dr. Karmach

Worked example — solution

Step 1 · Start phase and path

A is in the solid region, so it begins solid. Heating at constant pressure is a horizontal path to the right.

Dr. Karmach

Worked example — solution

Step 1 · Start phase and path
Step 2 · Cross the curves in order

Above the triple point, the path crosses the fusion curve (solid → liquid, melting), then the vaporization curve (liquid → gas, boiling).

solid → (cross fusion) → liquid → (cross vaporization) → gas
two curves crossed = two phase changes: melts, then boils
Dr. Karmach

Worked example — solution

Step 1 · Start phase and path
Step 2 · Cross the curves in order

solid → (cross fusion) → liquid → (cross vaporization) → gas
two curves crossed = two phase changes: melts, then boils
Had the pressure been below the triple point, the same rightward path would cross only the sublimation curve — solid straight to gas, no liquid — which is exactly how dry ice behaves at 1 atm.
Dr. Karmach

Where this goes wrong

Swapping the axes. Temperature is the horizontal axis, pressure the vertical — read T across the bottom, P up the side, not the reverse.
Confusing the two special points. The triple point is where all three phases coexist; the critical point is where the liquid–gas distinction ends. They are different spots.
Assuming everything melts at 1 atm. If the triple point is above 1 atm (CO₂, 5.1 atm), the 1-atm line never reaches the fusion curve — the solid sublimes instead of melting.
Treating water's fusion line as normal. Water's solid–liquid line slopes up-to-the-left; ice is less dense than water, so raising the pressure on ice can melt it.
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Practice

A pure substance has its triple point at 5.1 atm and −57 °C (like CO₂). A block of its solid is warmed at a constant 1 atm from very cold to very hot. What does it do?

  1. Melts to a liquid, then boils to a gas.
  2. Sublimes — turns directly from solid to gas.
  3. Melts to a liquid and stays liquid.
  4. Nothing; it stays solid the whole way.
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Practice — answer: B

1 atm is BELOW the triple-point pressure of 5.1 atm
so the 1-atm line lies under the triple point and crosses only the sublimation curve

Because 1 atm is below the triple point, the constant-pressure path never touches the fusion or vaporization curves — it meets only the sublimation curve, so the solid goes straight to gas (B). A describes a normal substance whose triple point is below 1 atm. C and D ignore that a heated solid must change phase once it crosses that curve.

This is dry ice: solid CO₂ at 1 atm sublimes at about −78 °C rather than melting. ✓
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Check yourself

  1. On a generic phase diagram, which curve does a constant-pressure heating path cross first if the pressure is above the triple point — and what phase change is it?
  2. Why can raising the pressure on ice at 0 °C melt it, when raising the pressure on most solids does the opposite?

A phase diagram ties together everything about a pure substance's states — melting, boiling, sublimation, and the limits set by the triple and critical points — all on one pressure-versus-temperature map.

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6 · Types of Solids

Classify a solid as crystalline or amorphous and, for a crystal, sort it into one of the four types (ionic, metallic, covalent-network, molecular) from the particle at its lattice points and the force holding them — then predict its melting point, hardness, and conductivity, and count the atoms in a simple, body-centered, or face-centered cubic unit cell.

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Four ways to build a crystal

Salt, copper, diamond, and ice are all crystalline solids, yet their melting points run from below room temperature to over 3500 °C. The whole difference lies in what sits at the lattice points — and what force holds it there.

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Crystalline vs amorphous

There are two ways for particles to lock into a solid. A crystalline solid has a regular, repeating lattice — long-range order — so it melts sharply at a single temperature. An amorphous solid has no long-range order; heated, it softens gradually over a range instead.

crystalline = ordered, repeating lattice → sharp melting point
amorphous = no long-range order → softens over a range · glass, rubber, most plastics
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Two questions sort every crystal

Classifying a crystalline solid comes down to two answers: what particle sits at each lattice point, and what force holds those particles together. The two answers give four families — and the family fixes the properties.

particle + force → type → properties
the force is the throughline: stronger force means higher melting point and greater hardness
  • Ionic — ions, held by ionic bonds
  • Metallic — metal atoms, held by metallic bonding
  • Covalent network — atoms, held by a continuous network of covalent bonds
  • Molecular — molecules, held by intermolecular forces
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Ionic & metallic solids

Ionic — positive & negative ions · electrostatic ionic bonds
high mp, hard but brittle; conducts only when molten or dissolved · NaCl, MgO
Metallic — metal cations in a sea of shared electrons · metallic bonding
melting point varies, malleable & ductile; conducts as a solid · Cu, Fe, Au

That mobile sea of electrons is what lets a metal both bend without shattering and carry a current.

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Covalent-network & molecular solids

Covalent network — atoms joined in one continuous covalent network
very high mp, very hard, usually nonconducting · diamond, SiO₂ (quartz), SiC
Molecular — whole molecules held by intermolecular forces
low mp, soft, nonconducting · ice, dry ice (CO₂), sugar

Graphite is the exception among network solids: its sheets slide past one another (soft, a lubricant), and its delocalized electrons let it conduct.

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The whole picture

Read any row across — the particle sets the force, and the force sets every property.

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Counting atoms in a cubic unit cell

A unit cell is the smallest repeating box of the lattice. Atoms are shared with neighboring cells, so each contributes only a fraction: a corner atom ⅛, a face atom ½, a body-center atom a full 1.

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Classify a solid in three steps

  1. Name the particle at the lattice points — ions, a metal, network atoms, or discrete molecules?
  2. Name the force that holds them — ionic, metallic, covalent-network, or intermolecular?
  3. Predict the properties — melting point, hardness, and whether it conducts all follow from that force.
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Worked example — identify and predict

A shiny solid melts at 1085 °C, bends without breaking, and conducts electricity as a solid.
Classify it, then explain the electrical behavior — and contrast it with table salt, NaCl.

Work the three steps: name the particle, name the force, then read off the properties.

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Worked example — solution

Step 1 · the particle & force

Shiny, bends without breaking, and conducts as a solid — these are the signatures of a metal. The lattice points hold metal cations bathed in a sea of shared electrons.

metallic solid — e.g. copper (mp 1085 °C)
it conducts as a solid because the delocalized electrons are free to move
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Worked example — solution

Step 1 · the particle & force

metallic solid — e.g. copper (mp 1085 °C)
it conducts as a solid because the delocalized electrons are free to move
Step 2 · contrast with NaCl

In table salt the charges are ions locked rigidly in the lattice — no free carriers. It stays an insulator until you melt or dissolve it and set the ions loose.

NaCl — ionic solid: conducts ONLY when molten or dissolved
same "does it conduct?" question, opposite answer — the holding force is what differs
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Where this goes wrong

Ionic solids conduct as solids. They don't — the ions are locked in place. Conduction needs mobile charges, so an ionic solid conducts only once molten or dissolved.
Dry ice is a network solid like SiO₂. No — CO₂ freezes as a molecular solid (discrete molecules, weak IMFs, sublimes at −78 °C). SiO₂ is a covalent network (mp ≈ 1700 °C).
A wide melting range means it's crystalline. Backwards — a sharp melting point marks a crystal; softening over a range marks an amorphous solid.
Counting every drawn atom as a whole. Corner atoms are shared by 8 cells (⅛ each), face atoms by 2 (½). An fcc cell holds 8×⅛ + 6×½ = 4 atoms, not 14.
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Check yourself

  1. Diamond and dry ice are both built only from nonmetal atoms, yet diamond melts near 3500 °C while dry ice sublimes at −78 °C. Which is covalent-network and which is molecular — and what force explains the enormous gap?
  2. How many atoms belong to a body-centered cubic unit cell? Show the ⅛ and whole-atom counting.

Name the particle and its holding force, and every property follows — the same logic runs forward into bonding, phase changes, and materials design.

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Can you…?

  • ☐ identify the intermolecular forces present in a substance and rank their relative strength?
  • ☐ relate intermolecular-force strength to boiling point and other physical properties?
  • ☐ apply the heats of fusion and vaporization to compute the energy of a phase change?
  • ☐ read and construct a heating or cooling curve and compute the heat for each segment?

If any box stays empty, the practice site has a drill for it. 🧪

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