Thermochemistry

General Chemistry · Dr. Karmach

Dr. Karmach

By the end of this unit, you can…

  • Distinguish heat from work and convert among joules, calories, and Calories
  • Identify exothermic and endothermic processes from equations, energy diagrams, and the sign of ΔH
  • Apply q = m·c·ΔT to find heat, mass, specific heat, or temperature change
  • Compare how specific heats set different substances' temperature response to the same heat
  • Use calorimetry data to determine the heat of a process or reaction
  • Reverse and scale thermochemical equations and use ΔH as a conversion factor
  • Combine reversed and scaled equations with Hess's law to find an overall reaction's enthalpy
  • Write formation equations and use standard formation enthalpies to find any reaction's enthalpy
  • Compute heat for melting, vaporizing, or a full heating curve
Dr. Karmach

Today's route 🗺️

  1. Energy & Its Units
  2. Internal Energy & the First Law
  3. Exothermic & Endothermic
  4. Specific Heat & q = mcΔT
  5. Comparing Specific Heats
  6. Heat of a Phase Change
  7. Heating & Cooling Curves
  8. Calorimetry
  9. Thermochemical Equations
  10. Hess's Law
  11. Standard Enthalpies of Formation
Dr. Karmach

1 · Energy & Its Units

Tell kinetic from potential energy and heat from temperature, and convert any amount of energy among joules, calories, kilojoules, and food Calories.

Dr. Karmach

Same snack, two labels

The same snack bar sells in two countries. One label lists 230 Calories; the other lists 960 kJ. Both describe the same energy, counted in different units.

Dr. Karmach

Energy is never created or destroyed

Energy is the capacity to transfer heat or to do work. A process moves energy from one place to another or changes its form. The total amount never changes.

energy leaving one place = energy arriving in another
the total is fixed, so an amount of energy can be counted, like mass
Dr. Karmach

Kinetic and potential energy

Kinetic energy is energy of motion. Potential energy is energy stored by position or arrangement. Fuels hold chemical potential energy: stored in the arrangement of atoms, released when a reaction rearranges them.

Dr. Karmach

Two ways energy transfers: heat and work

Energy transfers between things in exactly two ways. Heat (q) is transfer driven by a temperature difference. Work (w) is transfer by a force moving something.

heat (q): hot pan → cool water
energy flows because the temperatures differ
work (w): expanding gas pushes a piston
energy moves because a force acts through a distance
Dr. Karmach

Temperature is not heat

Temperature measures the average kinetic energy of the particles: an intensity. Heat is an amount of energy in transfer. More sample means more energy at the same temperature.

a cup and a bathtub, both at 40 °C
same temperature, yet the tub transfers far more heat as it cools
Dr. Karmach

The units of energy

The SI unit is the joule (J). 1 cal = 4.184 J, exactly. The food Calorie has a capital C: 1 Cal = 1 kcal = 1000 cal. Each equality is an ordinary conversion factor.

Dr. Karmach

The method

  1. Write the given: number and unit.
  2. Plan the route: given unit → wanted unit. Read a capital C as 1000 cal.
  3. Chain the factors so each unit cancels.
  4. Sense-check the size and the surviving unit.
Dr. Karmach

Worked example 1: calories to joules

Step 1 · Write the given

1 cal = 4.184 J
given: 175 cal · wanted: J

A single-use hand warmer releases 175 cal of heat as the iron inside it rusts. Express the energy in joules.

Dr. Karmach

Worked example 1: solution

1 cal = 4.184 J
given: 175 cal · wanted: J

Step 2 · Plan the route

One arrow links the units: cal → J. One conversion factor is needed.

Dr. Karmach

Worked example 1: solution

1 cal = 4.184 J
given: 175 cal · wanted: J
Step 2 · Plan the route Step 3 · Chain the factors so each unit cancels

The factor takes cal in the denominator, so cal cancels and J survives:

175 cal × 4.184 J1 cal = 732 J
Dr. Karmach

Worked example 1: solution

1 cal = 4.184 J
given: 175 cal · wanted: J
Step 2 · Plan the route Step 3 · Chain the factors so each unit cancels
175 cal × 4.184 J1 cal = 732 J
Step 4 · Sense-check
A joule is smaller than a calorie, so the count in joules must be larger: 175 → 732. The heat itself is unchanged. ✓
Dr. Karmach

Worked example 1: the route on the map

1 cal = 4.184 J
given: 175 cal · found: 732 J

The units cal and J share one edge. One equality gives one conversion factor. ✓
Dr. Karmach

Worked example 2: kilojoules to calories

Step 1 · Write the given

1 kJ = 1000 J · 1 cal = 4.184 J
given: 2.50 kJ · wanted: cal

An instant cold pack absorbs 2.50 kJ of heat from the skin it touches. Express the energy in calories.

Dr. Karmach

Worked example 2: solution

1 kJ = 1000 J · 1 cal = 4.184 J
given: 2.50 kJ · wanted: cal · plan: kJ → J → cal

Step 2 · Plan the route

No single equality links kJ to cal. The route runs through the joule: kJ → J → cal. Two conversion factors are needed.

Dr. Karmach

Worked example 2: solution

1 kJ = 1000 J · 1 cal = 4.184 J
given: 2.50 kJ · wanted: cal · plan: kJ → J → cal
Step 2 · Plan the route Step 3 · Chain the factors so each unit cancels

The prefix factor cancels kJ; the calorie factor takes J in the denominator:

2.50 kJ × 1000 J1 kJ × 1 cal4.184 J = 598 cal
Dr. Karmach

Worked example 2: solution

1 kJ = 1000 J · 1 cal = 4.184 J
given: 2.50 kJ · wanted: cal · plan: kJ → J → cal
Step 2 · Plan the route Step 3 · Chain the factors so each unit cancels
2.50 kJ × 1000 J1 kJ × 1 cal4.184 J = 598 cal
Step 4 · Sense-check
One calorie holds 4.184 J, so 2500 J make fewer calories than joules: 598. The pack absorbs the same heat under either name. ✓
Dr. Karmach

Worked example 2: the route on the map

1 kJ = 1000 J · 1 cal = 4.184 J
given: 2.50 kJ · found: 598 cal

No edge joins kJ to cal. The route takes two edges through the joule: two conversion factors. ✓
Dr. Karmach

Your turn: calories to kilojoules

1 cal = 4.184 J · 1 kJ = 1000 J
given: 7.10 × 10³ cal · wanted: kJ · plan: cal → J → kJ

Burning one gram of ethanol releases 7.10 × 10³ cal.

7.10 × 10³ cal × 4.184 J1 cal × kJ J = kJ

Fill the second factor from 1 kJ = 1000 J, then compute.

Dr. Karmach

Your turn: calories to kilojoules

1 cal = 4.184 J · 1 kJ = 1000 J
given: 7.10 × 10³ cal · wanted: kJ · plan: cal → J → kJ

Burning one gram of ethanol releases 7.10 × 10³ cal.

7.10 × 10³ cal × 4.184 J1 cal × kJ J = kJ

Fill the second factor from 1 kJ = 1000 J, then compute.

7.10 × 10³ cal × 4.184 J1 cal × 1 kJ1000 J = 29.7 kJ
Dr. Karmach

Where this goes wrong

Writing the 4.184 factor upside down. 175 cal × (1 cal / 4.184 J) = 41.8 cal²/J. No unit cancels, and the answer is not in joules. The factor that cancels cal gives 732 J.
Stopping at joules. The plan cal → J → kJ has two arrows. Stopping after one leaves 2.97 × 10⁴ J: joules, not the wanted kilojoules. The chain ends at 29.7 kJ.
Reading temperature as an amount of energy. A cup of tea and a bathtub of water can both read 40 °C. The temperatures match; the tub holds far more energy. Temperature is an intensity; heat is an amount.
Dr. Karmach

Practice 1

1 kJ = 1000 J · 1 cal = 4.184 J
given: 6.20 kJ · wanted: cal

Dissolving calcium chloride in a beaker of water releases 6.20 kJ of heat. How many calories is that?

  1. 2.59 × 10⁴
  2. 1.48 × 10³
  3. 6.20 × 10³
  4. 1.48
Dr. Karmach

Practice 1 · answer: B

1 kJ = 1000 J · 1 cal = 4.184 J
given: 6.20 kJ · plan: kJ → J → cal
6.20 kJ × 1000 J1 kJ × 1 cal4.184 J = 1.48 × 10³ cal (answer B)

A flipped the 4.184 factor: 6.20 × 10³ × 4.184 = 2.59 × 10⁴, and no unit cancels. C stopped after the prefix factor: 6.20 × 1000 = 6.20 × 10³, a count of joules, not calories. D treated kilojoules as joules: 6.20 / 4.184 = 1.48, a thousand times too small.

Each calorie holds 4.184 J, so 6.20 × 10³ J make fewer calories than joules: 1.48 × 10³. ✓
Dr. Karmach

Worked example 3: the food Calorie

Step 1 · Write the given

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · wanted: kJ

A snack bar's label lists 230 Calories; the same bar abroad is labeled 960 kJ. Express 230 Cal in kilojoules.

A common first attempt treats 230 Calories as 230 calories. Test it.

Dr. Karmach

Worked example 3: solution

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · wanted: kJ

A common first attempt

230 cal × 4.184 J1 cal × 1 kJ1000 J = 0.962 kJ ✗
Dr. Karmach

Worked example 3: solution

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · wanted: kJ

A common first attempt

230 cal × 4.184 J1 cal × 1 kJ1000 J = 0.962 kJ ✗
The kilojoule label reads 960: this result is 1000 times too small. The label's unit is Cal, not cal. ✗
Dr. Karmach

Worked example 3: the correct chain

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · wanted: kJ

Step 2 · Plan the route

The capital C marks the food Calorie: 1 Cal = 1000 cal. The route: Cal → cal → J → kJ. Three conversion factors are needed.

Dr. Karmach

Worked example 3: the correct chain

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · wanted: kJ
Step 2 · Plan the route Step 3 · Chain the factors so each unit cancels
230 Cal × 1000 cal1 Cal × 4.184 J1 cal × 1 kJ1000 J = 962 kJ
Dr. Karmach

Worked example 3: the correct chain

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · wanted: kJ
Step 2 · Plan the route Step 3 · Chain the factors so each unit cancels
230 Cal × 1000 cal1 Cal × 4.184 J1 cal × 1 kJ1000 J = 962 kJ
Step 4 · Sense-check
The kilojoule label reads 960: the chain reproduces it, rounded. The same chain shows 1 Cal = 4.184 kJ. ✓
Dr. Karmach

Worked example 3: the route on the map

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 230 Cal · found: 962 kJ

Three edges, three conversion factors. The trip around the map reproduces the top edge: 1 Cal = 4.184 kJ. ✓
Dr. Karmach

Take-home: the food Calorie is a kilocalorie

Do: read the capital C as 1000 cal. Big C, big unit.

230 Cal × (1000 cal / 1 Cal) × (4.184 J / 1 cal) × (1 kJ / 1000 J) = 962 kJ
matches the 960 kJ label ✓

Do not: read Cal as cal. The answer lands 1000 times too small.

230 cal × (4.184 J / 1 cal) × (1 kJ / 1000 J) = 0.962 kJ
1000 times smaller than the label ✗
Dr. Karmach

Practice 2

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 8.50 Cal per minute · 40.0 min · wanted: kJ

Swimming laps burns about 8.50 Calories per minute. How many kilojoules do 40.0 minutes of laps use?

  1. 1.42
  2. 81.3
  3. 340.
  4. 1.42 × 10³
Dr. Karmach

Practice 2 · answer: D

1 Cal = 1000 cal · 1 cal = 4.184 J · 1 kJ = 1000 J
given: 8.50 Cal per minute · 40.0 min · plan: min → Cal → cal → J → kJ
40.0 min × 8.50 Cal1 min = 340. Cal
340. Cal × 1000 cal1 Cal × 4.184 J1 cal × 1 kJ1000 J = 1.42 × 10³ kJ (answer D)

A read Cal as cal: 340. × 4.184 / 1000 = 1.42, a thousand times too small. B flipped the 4.184 factor: 340. × 1000 / 4.184 / 1000 = 81.3, and the joule never cancels. C stopped at Calories: 340. is the energy in Cal, never converted to kJ.

One food Calorie is 4.184 kJ, so 340 Cal sits near 340 × 4 = 1360 kJ. The chain gives 1.42 × 10³. ✓
Dr. Karmach

Check yourself

  1. A label lists 95 Calories. Write the chain to kilojoules: which factor comes first, and what does each unit cancel into?
  2. A cup of water and a pot of water both read 60 °C. Which quantity matches, and which differs: temperature, or energy content?

Every joule a system gains or loses arrives as heat (q) or as work (w). The first law adds them: ΔE = q + w. At constant pressure the heat term earns its own name, the enthalpy change ΔH.

Dr. Karmach

2 · Internal Energy & the First Law

Track a system's internal energy with the first law, ΔE = q + w, assigning the correct signs to heat and work, computing pressure-volume work from w = −P·ΔV, and telling a state function (E, ΔE) from a path function (q, w).

Dr. Karmach

Energy has nowhere to hide

A system can gain or lose energy, but the total never vanishes. Every joule it loses turns up in the surroundings, crossing the boundary as heat or work.

Dr. Karmach

Internal energy: the system's whole energy account

The internal energy E is the total of every kinetic and potential energy inside the system: all the molecular motion and every bond and interaction, added together.

E = all kinetic energy + all potential energy inside the system
its absolute size is out of reach: thermochemistry tracks only the change, ΔE = E(final) − E(initial)
Dr. Karmach

The first law: energy is conserved

Energy is never created or destroyed: it only moves. A system's gains come from the surroundings; its losses go to them. It crosses the boundary as heat (q) or work (w).

ΔE = q + w
the first law of thermodynamics: a system's energy change equals the heat plus the work exchanged with its surroundings
Dr. Karmach

Open, closed, and isolated systems

open system: matter and energy both cross · an open pot of soup
steam escapes (matter) · heat escapes (energy)
closed system: energy crosses, matter cannot · a sealed flask
the glass passes heat · nothing inside gets out
isolated system: neither crosses · a stoppered vacuum thermos, nearly
no matter out · almost no heat out

Count what can cross the boundary: an open system passes 2 things, a closed system 1, an isolated system 0.

Dr. Karmach

Adding signed amounts

(+200) + (−50) = +150
a deposit of 200 and a withdrawal of 50 · money in is +, money out is − · the balance rises by 150

A bank statement signs every entry from the account's side, then adds. Energy is tracked the same way: heat and work are the entries, and ΔE is the change in the balance.

Dr. Karmach

One sign rule: positive means energy in

Give q and w a + sign when they add energy to the system, a − sign when they take energy out. Read every arrow from the system's point of view.

+q heat INTO system · −q heat OUT · +w work done ON system · −w work done BY system
endothermic: q > 0 · exothermic: q < 0 · compression: w > 0 · expansion: w < 0
Dr. Karmach

The method

  1. Sign each quantity: heat in +q, out −q; work on +w, by −w.
  2. Solve ΔE = q + w for the unknown: ΔE, q, or w.
  3. Read the sign: positive means energy in.

Dr. Karmach

Guided example: a refrigerator compressor

310 J of work done on the gas · 450 J of heat released by the gas
system: the coolant gas · wanted: ΔE of the gas

In a refrigerator, the compressor squeezes the coolant gas with 310 J of work. The hot gas then releases 450 J of heat to the kitchen air.

Find ΔE for the gas.

Dr. Karmach

Guided example: solution

Step 1 · Sign each quantity

The system is the gas. Heat leaves it, so q = −450 J. The compressor pushes on it, a compression, so w = +310 J.

Dr. Karmach

Guided example: solution

Step 1 · Sign each quantity
Step 2 · Solve ΔE = q + w for the unknown

ΔE is the unknown, so add the two signed values:

ΔE = q + w = (−450 J) + (+310 J) = −140 J
q: heat out, − · w: work on the gas, + · given: 310 J of work on, 450 J of heat out
Dr. Karmach

Guided example: solution

Step 1 · Sign each quantity
Step 2 · Solve ΔE = q + w for the unknown

ΔE = q + w = (−450 J) + (+310 J) = −140 J
q: heat out, − · w: work on the gas, + · given: 310 J of work on, 450 J of heat out
Step 3 · Read the sign

ΔE is negative: more energy left the gas than entered it.

Dr. Karmach

Guided example: solution

Step 1 · Sign each quantity
Step 2 · Solve ΔE = q + w for the unknown

ΔE = q + w = (−450 J) + (+310 J) = −140 J
q: heat out, − · w: work on the gas, + · given: 310 J of work on, 450 J of heat out
Step 3 · Read the sign

The gas lost 140 J: the 450 J of heat out outweighs the 310 J of work in. ✓
Dr. Karmach

Practice 1

ΔE = q + w
given: 165 J of heat lost · 58 J of work done by the gas · wanted: ΔE of the gas

Hot gas in an engine cylinder pushes its piston outward, doing 58 J of work, while it loses 165 J of heat to the cylinder walls. What is ΔE for the gas, in joules?

  1. +107
  2. −223
  3. +223
  4. −107
Dr. Karmach

Practice 1 · answer: B

ΔE = q + w = (−165 J) + (−58 J) = −223 J
heat lost: q = −165 J · work done by the gas, an expansion: w = −58 J · answer B

A flipped the heat sign: (+165) + (−58) = +107 J. C reversed both signs: 165 + 58 = +223 J, the surroundings' ΔE, not the gas's. D subtracted the work: (−165) − (−58) = −107 J.

Both flows carry energy out of the gas, so both terms are negative and so is their sum. ✓
Dr. Karmach

Practice 1 · answer: B

ΔE = q + w = (−165 J) + (−58 J) = −223 J
heat lost: q = −165 J · work done by the gas, an expansion: w = −58 J · answer B

A flipped the heat sign: (+165) + (−58) = +107 J. C reversed both signs: 165 + 58 = +223 J, the surroundings' ΔE, not the gas's. D subtracted the work: (−165) − (−58) = −107 J.

Both flows carry energy out of the gas, so both terms are negative and so is their sum. ✓

Dr. Karmach

State functions vs path functions

E and ΔE are state functions: they depend only on the initial and final states, never on the route. q and w are path functions: their values depend on the route.

altitude ↔ E (state) · distance walked ↔ q and w (path)
two routes share one ΔE, yet split it into different amounts of q and w
Dr. Karmach

Worked example: finding the heat

ΔE = q + w
given: ΔE = −150 J · 240 J of work done ON the system · wanted: q

A system's internal energy drops by 150 J even though the surroundings do 240 J of work on it. Find the heat, with its sign.

Dr. Karmach

Worked example: solution

ΔE = q + w
given: ΔE = −150 J · 240 J of work done ON the system · wanted: q

Step 1 · Sign each quantity

The energy fell: ΔE = −150 J. Work is done on the system: w = +240 J. The unknown is q.

Dr. Karmach

Worked example: solution

ΔE = q + w
given: ΔE = −150 J · 240 J of work done ON the system · wanted: q
Step 1 · Sign each quantity Step 2 · Solve ΔE = q + w for the unknown
q = ΔE − w = (−150 J) − (+240 J) = −390 J
the system released 390 J of heat
Dr. Karmach

Worked example: solution

ΔE = q + w
given: ΔE = −150 J · 240 J of work done ON the system · wanted: q
Step 1 · Sign each quantity Step 2 · Solve ΔE = q + w for the unknown
q = ΔE − w = (−150 J) − (+240 J) = −390 J
the system released 390 J of heat
Step 3 · Read the sign
The system gained 240 J by work yet still ended 150 J down, so heat had to carry away both amounts: 390 J out. Negative q, heat released. ✓
Dr. Karmach

Worked example: solution

ΔE = q + w
given: ΔE = −150 J · 240 J of work done ON the system · wanted: q
Step 1 · Sign each quantity Step 2 · Solve ΔE = q + w for the unknown
q = ΔE − w = (−150 J) − (+240 J) = −390 J
the system released 390 J of heat
Step 3 · Read the sign
The system gained 240 J by work yet still ended 150 J down, so heat had to carry away both amounts: 390 J out. Negative q, heat released. ✓

Dr. Karmach

Your turn: finding the work

ΔE = q + w
given: q = +425 J absorbed · ΔE = +125 J · wanted: w

A gas absorbs 425 J of heat, yet its internal energy rises by only 125 J.

w = ΔE − q = ( J) − ( J) = J
sign the two givens, subtract, and read the result's sign

Fill the blanks, then state what the sign of w says the gas did.

Dr. Karmach

Your turn: finding the work

ΔE = q + w
given: q = +425 J absorbed · ΔE = +125 J · wanted: w
w = ΔE − q = ( J) − ( J) = J
sign the two givens, subtract, and read the result's sign
w = ΔE − q = (+125 J) − (+425 J) = −300 J
w negative: the gas did 300 J of work on the surroundings · an expansion
Dr. Karmach

Your turn: finding the work

ΔE = q + w
given: q = +425 J absorbed · ΔE = +125 J · wanted: w
w = ΔE − q = ( J) − ( J) = J
sign the two givens, subtract, and read the result's sign
w = ΔE − q = (+125 J) − (+425 J) = −300 J
w negative: the gas did 300 J of work on the surroundings · an expansion

Dr. Karmach

Practice 2

ΔE = q + w
given: 75 J of heat given off · internal energy up by 115 J · wanted: w

Steam in a sealed cylinder gives off 75 J of heat while its internal energy goes up by 115 J. What is w for the steam, in joules?

  1. −190
  2. +40
  3. +190
  4. +75
Dr. Karmach

Practice 2 · answer: C

w = ΔE − q = (+115 J) − (−75 J) = +190 J
heat given off: q = −75 J · energy went up: ΔE = +115 J · answer C

A subtracted in reverse: q − ΔE = (−75) − (+115) = −190 J, the work read from the surroundings' side. B flipped the heat sign: 115 − 75 = +40 J, as if the steam had absorbed the heat. D treated ΔE as zero: w = −q = +75 J, true only for a cycle back to the start.

The steam lost 75 J as heat yet ended 115 J up, so work brought in both: 75 + 115 = 190 J. Positive w: the steam was compressed. ✓
Dr. Karmach

Practice 2 · answer: C

w = ΔE − q = (+115 J) − (−75 J) = +190 J
heat given off: q = −75 J · energy went up: ΔE = +115 J · answer C

A subtracted in reverse: q − ΔE = (−75) − (+115) = −190 J, the work read from the surroundings' side. B flipped the heat sign: 115 − 75 = +40 J, as if the steam had absorbed the heat. D treated ΔE as zero: w = −q = +75 J, true only for a cycle back to the start.

The steam lost 75 J as heat yet ended 115 J up, so work brought in both: 75 + 115 = 190 J. Positive w: the steam was compressed. ✓

Dr. Karmach

Practice 3

ΔE = q + w
given: path 1: q = +170 J, w = +50 J · path 2: q = +310 J · wanted: w on path 2

A gas is taken between the same two states along two paths. On path 1 it absorbs 170 J of heat while the surroundings do 50 J of work on it. On path 2 it absorbs 310 J of heat. What is w on path 2, in J?

  1. +530
  2. +220
  3. +50
  4. −90
Dr. Karmach

Practice 3 · answer: D

path 1: ΔE = q + w = (+170 J) + (+50 J) = +220 J
E is a state function: path 2 starts and ends in the same states, so its ΔE is also +220 J
path 2: w = ΔE − q = (+220 J) − (+310 J) = −90 J
answer D: w negative, so on path 2 the gas does 90 J of work on the surroundings

A flipped the sign of path 2's heat: 220 + 310 = +530 J, as if the 310 J had left the gas. B stopped at ΔE: +220 J is the energy change both paths share, not path 2's work. C copied path 1's work, +50 J: w is a path function and changes with the route.

Path 2 brings in 310 J of heat but may keep only 220 J, so 90 J must leave as work. ✓
Dr. Karmach

Practice 3 · answer: D

path 1: ΔE = q + w = (+170 J) + (+50 J) = +220 J
E is a state function: path 2 starts and ends in the same states, so its ΔE is also +220 J
path 2: w = ΔE − q = (+220 J) − (+310 J) = −90 J
answer D: w negative, so on path 2 the gas does 90 J of work on the surroundings

A flipped the sign of path 2's heat: 220 + 310 = +530 J, as if the 310 J had left the gas. B stopped at ΔE: +220 J is the energy change both paths share, not path 2's work. C copied path 1's work, +50 J: w is a path function and changes with the route.

Path 2 brings in 310 J of heat but may keep only 220 J, so 90 J must leave as work. ✓

Dr. Karmach

ΔH: the heat at constant pressure

qp = ΔH
constant pressure: an open flask on the bench · the heat measured there is the enthalpy change

Run a process open to the air and its heat is the enthalpy change, ΔH. Most chemistry runs at constant pressure, which is why ΔH is the number tables report.

Dr. Karmach

Where this goes wrong

Adding magnitudes, ignoring signs. Work done BY the system is −w. A gas that absorbs 125 J and does 78 J of work has ΔE = 125 − 78 = 47 J, not 203 J.
Flipping the heat sign. Heat absorbed is +q (endothermic); heat released is −q (exothermic). Reading "releases" as + gives the wrong ΔE, often the wrong sign entirely.
Signing the work by the wrong party. "The surroundings do 240 J of work ON the system" means w = +240 J. Read it as work done BY the system and w flips to −240 J, landing ΔE a full 480 J off. Every sign reads from the system's side.
Calling q or w a state function. Only E and ΔE are path-independent. Heat and work depend on the route: one ΔE can come from many different q, w pairs.
Dr. Karmach

Extra example 1: heat in, work out

absorbs 125 J of heat · does 78 J of work on the surroundings
wanted: ΔE of the system

A gas in a cylinder absorbs 125 J of heat, then does 78 J of work pushing its piston outward. Find the change in its internal energy.

Dr. Karmach

Extra example 1: solution

Step 1 · Sign each quantity

Heat flows into the system, so q = +125 J. The system does work on the surroundings (expansion), so w = −78 J.

Dr. Karmach

Extra example 1: solution

Step 1 · Sign each quantity
Step 2 · Solve ΔE = q + w for the unknown

ΔE = q + w = (+125 J) + (−78 J) = +47 J
energy in (125) outweighs energy out (78), so E rises by 47 J
Dr. Karmach

Extra example 1: solution

Step 1 · Sign each quantity
Step 2 · Solve ΔE = q + w for the unknown

ΔE = q + w = (+125 J) + (−78 J) = +47 J
energy in (125) outweighs energy out (78), so E rises by 47 J
Step 3 · Read the sign
Watch the signs: adding the magnitudes (125 + 78 = 203 J) would treat the expansion as energy gained. The system spent 78 J doing work, so it keeps only 47 J of the 125 J it took in. ✓
Dr. Karmach

Extra example 1: solution

Step 1 · Sign each quantity
Step 2 · Solve ΔE = q + w for the unknown

ΔE = q + w = (+125 J) + (−78 J) = +47 J
energy in (125) outweighs energy out (78), so E rises by 47 J
Step 3 · Read the sign
Watch the signs: adding the magnitudes (125 + 78 = 203 J) would treat the expansion as energy gained. The system spent 78 J doing work, so it keeps only 47 J of the 125 J it took in. ✓

Dr. Karmach

Work from a changing volume

w = −P·ΔV
P: the constant external pressure, in atm · ΔV = V(final) − V(initial), in L · 1 L·atm = 101.325 J

A gas that expands pushes the surroundings back: it spends energy, w negative. A gas that is compressed receives that push: w positive. The minus sign in the formula produces both results automatically.

Dr. Karmach

Extra example 2: work of an expanding gas

w = −P·ΔV · 1 L·atm = 101.325 J
given: a gas expands from 264 mL to 971 mL · wanted: w (a) against a vacuum (b) against a constant 4.0 atm

A gas expands from 264 mL to 971 mL at constant temperature. Find the work done by the gas if it expands (a) against a vacuum and (b) against a constant pressure of 4.0 atm.

Dr. Karmach

Extra example 2: solution

a gas expands from 264 mL to 971 mL
w = −P·ΔV · 1 L·atm = 101.325 J · (a) vacuum (b) 4.0 atm

Part (a) · expansion against a vacuum

w = −P·ΔV = −(0)(0.707 L) = 0
there is no pressure in a vacuum, so w = 0 · nothing pushes back, no work
Dr. Karmach

Extra example 2: solution

a gas expands from 264 mL to 971 mL
w = −P·ΔV · 1 L·atm = 101.325 J · (a) vacuum (b) 4.0 atm
Part (a) · expansion against a vacuum
w = −P·ΔV = −(0)(0.707 L) = 0
there is no pressure in a vacuum, so w = 0 · nothing pushes back, no work
Part (b) · expansion against 4.0 atm

In liters, ΔV = 0.971 − 0.264 = +0.707 L. The external pressure is constant, so w = −P·ΔV, and the L·atm converts to joules:

w = −4.0 atm × 0.707 L = −2.83 L·atm × 101.325 J1 L·atm = −2.9 × 10² J
Dr. Karmach

Extra example 2: solution

a gas expands from 264 mL to 971 mL
w = −P·ΔV · 1 L·atm = 101.325 J · (a) vacuum (b) 4.0 atm
Part (a) · expansion against a vacuum
w = −P·ΔV = −(0)(0.707 L) = 0
there is no pressure in a vacuum, so w = 0 · nothing pushes back, no work
Part (b) · expansion against 4.0 atm
w = −4.0 atm × 0.707 L = −2.83 L·atm × 101.325 J1 L·atm = −2.9 × 10² J
Expansion is work done BY the gas, so w is negative: −286.5 J, kept to two significant figures as −2.9 × 10² J. Against a vacuum the same expansion costs nothing; work needs something to push against. ✓
Dr. Karmach

Extra practice

w = −P·ΔV · 1 L·atm = 101.325 J
given: a gas is compressed from 982 mL to 351 mL by a constant 3.0 atm · wanted: w

A piston compresses a gas from 982 mL to 351 mL under a constant external pressure of 3.0 atm. What is w for the gas, in J?

  1. +1.9 × 10²
  2. −1.9 × 10²
  3. +1.9
  4. +1.9 × 10⁻²
Dr. Karmach

Extra practice · answer: A

ΔV = 0.351 L − 0.982 L = −0.631 L
compression: the volume falls, so ΔV is negative
w = −3.0 atm × (−0.631 L) = +1.89 L·atm × 101.325 J1 L·atm = +1.9 × 10² J (answer A)

B dropped the minus sign in w = −P·ΔV: 3.0 × (−0.631) × 101.325 = −1.9 × 10² J, which would say the squeezed gas lost energy. C stopped at +1.89 L·atm and wrote it as joules; only the 101.325 J per L·atm factor makes joules. D turned the conversion factor upside down: 1.89 / 101.325 = 1.9 × 10⁻² J.

Compression is work done ON the gas: energy flows in, so w must be positive. The formula's minus sign and the negative ΔV cancel to say exactly that. ✓
Dr. Karmach

Check yourself

  1. A system releases 90 J of heat and has 140 J of work done on it. Find ΔE, and say whether its energy rose or fell.
  2. A gas is taken between the same two states by two different routes. Which of q, w, and ΔE must be the same on both routes, and why?

At constant pressure, the heat q gets its own name: the enthalpy change ΔH. Its sign sorts every process into exothermic or endothermic.

Dr. Karmach

3 · Exothermic & Endothermic

Classify any process as exothermic or endothermic (from the sign of ΔH, from an energy diagram, or from a heat term written into the equation) and state which way heat flows between system and surroundings.

Dr. Karmach

Two pouches from the drugstore

Snap the pouch inside a hand warmer and it climbs to 54 °C. Snap a cold pack and it drops near freezing. Sealed chemicals drive both changes.

Dr. Karmach

The system and its surroundings

The reaction is the system; the flask, your hand, the room are the surroundings. ΔH records the system's heat: out negative, in positive. The sign follows the system, not your hand.

Dr. Karmach

Enthalpy

Enthalpy, H, is the heat content of a system. A change in it, ΔH, equals the heat of the process at constant pressure. An open flask or a pouch in your hand qualifies.

ΔH = heat of the process at constant pressure
heat out of the system → ΔH negative · heat in → ΔH positive
Dr. Karmach

Exothermic and endothermic

exothermic: heat exits the system
surroundings warm up · ΔH negative · burning fuel, the hand-warmer pouch
endothermic: heat enters the system
surroundings cool down · ΔH positive · melting ice, the cold-pack pouch
memory hook: EXo, heat EXits · ENdo, heat ENters
the prefix names the heat's direction, read from the system's side

Heat "flows from a hot object to a cold object". A process sending heat out is exothermic; one taking heat in is endothermic. Both names describe the system; the surroundings show the opposite change.

Dr. Karmach

Energy diagrams

An energy diagram plots energy against reaction progress. Products below the reactants: the difference left as heat, exothermic. Products above: the difference came in as heat, endothermic.

Dr. Karmach

Heat written into the equation

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) + 890 kJ
heat on the product side: it leaves with the products · ΔH = −890 kJ · exothermic
2 H₂O(l) + 572 kJ → 2 H₂(g) + O₂(g)
heat on the reactant side: it must be supplied · ΔH = +572 kJ · endothermic

A thermochemical equation may carry its heat in-line. Product side: heat released, exothermic. Reactant side: heat absorbed, endothermic. The separate ΔH states the same fact with a sign.

Dr. Karmach

The method

  1. Name the system. The process is the system; all else is surroundings.
  2. Find the heat's direction. From the ΔH sign, diagram levels, or heat term.
  3. State the verdict. Heat out: exothermic, ΔH negative. Heat in: endothermic, ΔH positive.
Dr. Karmach

Worked example 1: a hand warmer's reaction

4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) · ΔH = −1648 kJ
given: the equation and its ΔH · wanted: the verdict and the heat's direction

Inside a hand warmer, iron powder reacts with oxygen from the air.

Classify the reaction and state which way heat flows.

Dr. Karmach

Worked example 1: solution

4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) · ΔH = −1648 kJ
given: the equation and its ΔH

Step 1 · Name the system

The iron and oxygen are the system. The pouch, the air, your cold hands: surroundings.

Dr. Karmach

Worked example 1: solution

4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) · ΔH = −1648 kJ
given: the equation and its ΔH
Step 1 · Name the system Step 2 · Find the heat's direction

ΔH is negative: −1648 kJ. Negative marks heat leaving the system.

Dr. Karmach

Worked example 1: solution

4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) · ΔH = −1648 kJ
given: the equation and its ΔH
Step 1 · Name the system Step 2 · Find the heat's direction Step 3 · State the verdict
4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) + 1648 kJ → exothermic
heat out · ΔH = −1648 kJ · the surroundings (your hands) warm up
Dr. Karmach

Worked example 1: solution

4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) · ΔH = −1648 kJ
given: the equation and its ΔH
Step 1 · Name the system Step 2 · Find the heat's direction Step 3 · State the verdict
4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) + 1648 kJ → exothermic
heat out · ΔH = −1648 kJ · the surroundings (your hands) warm up
The pouch warms your hand: the surroundings gain exactly the heat the system loses. A negative ΔH and a warming hand agree.
Dr. Karmach

Worked example 1: the clue used

4 Fe(s) + 3 O₂(g) → 2 Fe₂O₃(s) · ΔH = −1648 kJ
clue read: the sign of ΔH · verdict: exothermic

Any one of the three clues gives the heat's direction. Here the sign settled it: negative, heat out, exothermic. ✓
Dr. Karmach

Worked example 2: hydrogen peroxide decomposes

2 H₂O₂(l) → 2 H₂O(l) + O₂(g)
given: the energy diagram · wanted: the verdict and ΔH with its sign

Hydrogen peroxide fizzing on a cut breaks down into water and oxygen. Classify the process from the diagram and give ΔH.

Dr. Karmach

Worked example 2: solution

Step 1 · Name the system

The decomposing peroxide is the system; the cut, the skin, the air are surroundings.

Dr. Karmach

Worked example 2: solution


Step 1 · Name the system
Step 2 · Find the heat's direction

The products sit 196 kJ below the reactants. That difference left the system as heat.

Dr. Karmach

Worked example 2: solution


Step 1 · Name the system
Step 2 · Find the heat's direction
Step 3 · State the verdict

2 H₂O₂(l) → 2 H₂O(l) + O₂(g) → exothermic
products lower · heat out · ΔH = −196 kJ
Dr. Karmach

Worked example 2: solution


Step 1 · Name the system
Step 2 · Find the heat's direction
Step 3 · State the verdict

2 H₂O₂(l) → 2 H₂O(l) + O₂(g) → exothermic
products lower · heat out · ΔH = −196 kJ
Downhill on an energy diagram is heat out. The products hold less energy than the reactants, and the fizzing cut warms slightly.
Dr. Karmach

Worked example 2: the clue used

2 H₂O₂(l) → 2 H₂O(l) + O₂(g)
clue read: the energy-diagram levels · verdict: exothermic, ΔH = −196 kJ

No ΔH was written, and none was needed for the direction: products below the reactants is heat out. ✓
Dr. Karmach

Your turn: photosynthesis

6 CO₂(g) + 6 H₂O(l) + 2803 kJ → C₆H₁₂O₆(s) + 6 O₂(g)
a leaf builds glucose; the 2803 kJ arrives as sunlight
step question answer
1 · name the system what is changing? the CO₂ and water becoming glucose
2 · find the heat's direction which side carries the heat term? the side; heat the system
3 · state the verdict · ΔH = kJ

Complete the three steps.

Dr. Karmach

Your turn: photosynthesis

6 CO₂(g) + 6 H₂O(l) + 2803 kJ → C₆H₁₂O₆(s) + 6 O₂(g)
a leaf builds glucose; the 2803 kJ arrives as sunlight
step question answer
1 · name the system what is changing? the CO₂ and water becoming glucose
2 · find the heat's direction which side carries the heat term? the side; heat the system
3 · state the verdict · ΔH = kJ

Complete the three steps.

photosynthesis → endothermic
heat term on the reactant side · heat enters the system · ΔH = +2803 kJ
Dr. Karmach

Where this goes wrong

Reading the sign from your hand. A cold pack chills your skin, and the chill gets recorded as heat lost: ΔH = −26 kJ. The skin is surroundings. Its loss is the system's gain: ΔH = +26 kJ.
Pairing a label with the opposite flow. "Exothermic, and it absorbs heat" contradicts itself. The label names the flow: exothermic releases heat, endothermic absorbs it. One verdict carries both parts.
Reading the heat term from the wrong side. In 2 H₂O(l) + 572 kJ → 2 H₂(g) + O₂(g), the 572 kJ gets reported as released. It sits with the reactants, so it is consumed: absorbed, ΔH = +572 kJ.
Calling the higher level the bigger release. Height on an energy diagram is energy stored, not energy given off. Products above the reactants means the system took energy in: endothermic, ΔH positive.
Dr. Karmach

Practice 1

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH = −198 kJ
given: the equation and its ΔH

Sulfur dioxide converts to sulfur trioxide during sulfuric acid manufacture. Which statement describes the reaction?

  1. Endothermic: heat is absorbed by the system from the surroundings
  2. Exothermic: heat is absorbed by the system from the surroundings
  3. Exothermic: heat is released by the system to the surroundings
  4. Endothermic: heat is released by the system to the surroundings
Dr. Karmach

Practice 1 · answer: C

ΔH = −198 kJ → negative → heat out → exothermic (answer C)
heat released by the system · the surroundings warm up

A flipped the sign convention: heat absorbed would be counted into the system, +198 kJ, not −198 kJ. B paired the right label with the wrong flow: exothermic means heat exits the system. D paired the right flow with the wrong label: a heat-releasing reaction is exothermic.

Negative ΔH, heat out, exothermic, warmer surroundings: four readings of the same event.
Dr. Karmach

Worked example 3: the cold pack

NH₄NO₃(s) → NH₄NO₃(aq)
given: the pouch turns icy in your hand · wanted: the verdict and the sign of ΔH

Snapping the pack lets ammonium nitrate dissolve in water, and the pouch turns icy.

A common first answer: the pack is cold, so it is losing heat: exothermic. Test it.

Dr. Karmach

Worked example 3: solution

NH₄NO₃(s) → NH₄NO₃(aq)
the pouch turns icy in your hand

A common first answer

cold pack, so the pack is losing heat → exothermic?
cold marks heat leaving the pack only if the pack were the surroundings ✗

The cold skin is the evidence. Your hand is losing heat, and the hand is surroundings, not system.

Dr. Karmach

Worked example 3: solution

NH₄NO₃(s) → NH₄NO₃(aq)
the pouch turns icy in your hand
A common first answer
cold pack, so the pack is losing heat → exothermic?
cold marks heat leaving the pack only if the pack were the surroundings ✗
Step 1 · Name the system

The dissolving salt and water are the system. The pouch, your hand: surroundings.

Dr. Karmach

Worked example 3: solution

NH₄NO₃(s) → NH₄NO₃(aq)
the pouch turns icy in your hand
A common first answer
cold pack, so the pack is losing heat → exothermic?
cold marks heat leaving the pack only if the pack were the surroundings ✗
Step 1 · Name the system Step 2 · Find the heat's direction

Your hand cools: heat is leaving the surroundings and entering the system.

Dr. Karmach

Worked example 3: solution

NH₄NO₃(s) → NH₄NO₃(aq)
the pouch turns icy in your hand
A common first answer
cold pack, so the pack is losing heat → exothermic?
cold marks heat leaving the pack only if the pack were the surroundings ✗
Step 1 · Name the system Step 2 · Find the heat's direction Step 3 · State the verdict
NH₄NO₃(s) → NH₄NO₃(aq) → endothermic
heat in · measured ΔH = +26 kJ per mole dissolved · the surroundings (your hand) cool
Dr. Karmach

Worked example 3: solution

NH₄NO₃(s) → NH₄NO₃(aq)
the pouch turns icy in your hand
A common first answer
cold pack, so the pack is losing heat → exothermic?
cold marks heat leaving the pack only if the pack were the surroundings ✗
Step 1 · Name the system Step 2 · Find the heat's direction Step 3 · State the verdict
NH₄NO₃(s) → NH₄NO₃(aq) → endothermic
heat in · measured ΔH = +26 kJ per mole dissolved · the surroundings (your hand) cool
The pack feels cold *because* it absorbs heat. A cooling hand is the surroundings' loss and the system's gain: ΔH = +26 kJ, never −26 kJ.
Dr. Karmach

Take-home: your hand is the surroundings

feels hot → the surroundings are gaining heat → the system is losing it
exothermic · ΔH negative
feels cold → the surroundings are losing heat → the system is gaining it
endothermic · ΔH positive

Skin and thermometers sit in the surroundings. They report the surroundings' change, and the system did the opposite. Feels cold: the system is absorbing heat: endothermic, ΔH positive.

Dr. Karmach

Practice 2

CaO(s) + H₂O(l) → Ca(OH)₂(s) + 65 kJ
given: the equation · the bucket turns hot

Water is stirred into quicklime and the bucket turns hot. A classmate writes: "The 65 kJ ends up with the products, so the system gains heat: endothermic, ΔH = +65 kJ." What is wrong with the reasoning, if anything?

  1. Heat written with the products is released: exothermic, ΔH = −65 kJ. The hot bucket is the surroundings.
  2. Nothing is wrong: heat written with the products is heat gained, so ΔH = +65 kJ.
  3. Only the label is wrong: ΔH = +65 kJ stands, but a hot bucket means exothermic.
  4. Only the sign is wrong: it is endothermic, but heat that warms the bucket is −65 kJ.
Dr. Karmach

Practice 2 · answer: A

CaO(s) + H₂O(l) → Ca(OH)₂(s) + 65 kJ → exothermic, ΔH = −65 kJ (answer A)
heat term on the product side: released · the hot bucket is the surroundings gaining that heat

B read a product-side heat term as heat gained: it leaves with the products, so it is released, −65 kJ, not +65 kJ. C matched the sign but not the label: a positive ΔH would mean heat in, and a bucket cannot turn hot from that. D matched the label but not the sign: endothermic and ΔH = −65 kJ contradict each other.

Two pieces of evidence, one verdict: the heat term sits with the products, and the surroundings warm. Heat out, exothermic, ΔH negative.
Dr. Karmach

Extra practice 1

Ba(OH)₂·8H₂O(s) + 2 NH₄Cl(s) → BaCl₂(aq) + 2 NH₃(aq) + 10 H₂O(l)
given: the flask rests on a wet wooden board · the water under it freezes

Two white solids are stirred together in a flask on a wet board, and within minutes the water under the flask freezes. Which statement describes the reaction?

  1. Exothermic, ΔH negative: heat flows from the flask into the board
  2. Exothermic, ΔH positive: heat flows from the board into the flask
  3. Endothermic, ΔH positive: heat flows from the board into the flask
  4. Endothermic, ΔH negative: heat flows from the board into the flask
Dr. Karmach

Extra practice 1 · answer: C

Ba(OH)₂·8H₂O(s) + 2 NH₄Cl(s) → BaCl₂(aq) + 2 NH₃(aq) + 10 H₂O(l)
surroundings: the board and its water · heat flows board → flask · endothermic, ΔH positive (answer C)

A took the freezing as the reaction's own change. Freezing does release heat, but the water is surroundings, and its heat went into the flask. B paired the label with the wrong flow: heat into the system is endothermic. D read the sign from the surroundings: the board loses heat, the system gains it, so ΔH is positive.

Water freezes only when heat is pulled out of it. The flask pulled it out: the system absorbed heat, endothermic, ΔH positive. ✓
Dr. Karmach

Extra practice 2

2 HgO(s) + 43.4 kcal → 2 Hg(l) + O₂(g)
given: the heat term in kcal · 1 cal = 4.184 J

Strong heating breaks red mercury(II) oxide into mercury and oxygen. What is ΔH for the reaction, in kJ, sign included?

  1. +182
  2. −182
  3. +10.4
  4. +0.182
  5. +43.4
Dr. Karmach

Extra practice 2 · answer: A

2 HgO(s) + 43.4 kcal → 2 Hg(l) + O₂(g) → endothermic
heat term on the reactant side: absorbed · ΔH positive

Three conversion factors are needed: kcal → cal → J → kJ.

43.4 kcal × 1000 cal1 kcal × 4.184 J1 cal × 1 kJ1000 J = +182 kJ · answer A

B read the heat term from the wrong side: it sits with the reactants, so it is absorbed, +182 kJ. C flipped the 4.184 factor: 43.4 ÷ 4.184 = 10.4. D read kcal as cal: 43.4 × 4.184 = 182 J, only 0.182 kJ. E skipped the conversion: 43.4 is the heat in kcal, not kJ.

A kilojoule is smaller than a kilocalorie, so the kJ value must be the larger number: 43.4 × 4.184 = 182. ✓
Dr. Karmach

Extra practice 3

Zn(s) + 2 HCl(aq) → ZnCl₂(aq) + H₂(g)
given: 154 kJ of heat released · 2.48 kJ of work done by the H₂ pushing back the air

One mole of zinc dissolves in hydrochloric acid in an open flask. Which statement describes the reaction?

  1. Endothermic · ΔH = −154 kJ · ΔE = −156 kJ
  2. Exothermic · ΔH = −154 kJ · ΔE = −152 kJ
  3. Endothermic · ΔH = +154 kJ · ΔE = +152 kJ
  4. Exothermic · ΔH = −154 kJ · ΔE = −156 kJ
Dr. Karmach

Extra practice 3 · answer: D

Zn(s) + 2 HCl(aq) → ZnCl₂(aq) + H₂(g) → exothermic
open flask: ΔH = q = −154 kJ · the H₂ pushes back the air, work done BY the system: w = −2.48 kJ
ΔE = q + w = (−154 kJ) + (−2.48 kJ) = −156 kJ (answer D)
ΔH counts the heat alone · ΔE counts the heat and the work

A paired the label with the wrong sign: heat out is exothermic. B signed the work as done on the system: −154 + 2.48 = −152 kJ. The H₂ pushed the air back, so that energy left. C read the heat sign from the surroundings: +154 − 2.48 = +152 kJ. The room gains the heat; the system loses it.

Heat and work both leave the system, so ΔE is a little more negative than ΔH. Both negative: the flask warms its surroundings. ✓
Dr. Karmach

Check yourself

  1. Propane burns in a camp stove: C₃H₈(g) + 5 O₂(g) → 3 CO₂(g) + 4 H₂O(l), ΔH = −2220 kJ. State the verdict and which way heat flows.
  2. An energy diagram shows the products 178 kJ above the reactants. Give the sign of ΔH and the verdict.

Exothermic or endothermic names the heat's direction. How much heat a sample gains or loses depends on its mass, its substance, and its temperature change: q = m·c·ΔT.

Dr. Karmach

4 · Specific Heat & q = mcΔT

Use q = m·c·ΔT to find the heat, the mass, the specific heat, or the temperature change, with ΔT measured final minus initial so the sign of q shows which way the heat flowed.

Dr. Karmach

One burner, two temperatures

Five minutes in, the iron handle is too hot to touch; the water is barely warm. Iron needs far less heat than water for each degree it climbs.

Dr. Karmach

Specific heat: joules per gram per degree

specific heat c: the heat that raises 1 g of a substance by 1 °C
J/g·°C: water 4.184 · ethyl alcohol 2.46 · aluminum 0.897 · iron 0.449 · copper 0.385 · gold 0.129 · lead 0.128

Heat flowing in raises a substance's temperature; heat flowing out lowers it. The joules needed to move each gram by one degree are fixed for each substance: its specific heat, c.

Dr. Karmach

The heat equation

Three factors set the heat: the mass m, the substance's specific heat c, and the temperature change ΔT. One equation, four solvable quantities.

Dr. Karmach

ΔT carries a sign

ΔT = Tfinal − Tinitial
heating 20.0 → 50.0 °C: ΔT = +30.0 °C · cooling 50.0 → 20.0 °C: ΔT = −30.0 °C

ΔT is final minus initial, in that order. A cooling sample has a negative ΔT, so q comes out negative: the sample released heat. The sign records the direction of the flow.

Dr. Karmach

Specific heat c vs heat capacity C

C = m · c
60.0 g of water: C = 60.0 g × 4.184 J/g·°C = 251 J/°C · c stays 4.184 J/g·°C for any amount of water

Specific heat is intensive: per gram, the same for a drop or a lake. Heat capacity C is extensive: it grows with the sample, because m is in it.

memory hook: little c, one gram · big C, the whole sample
the food Calorie's cue again: the capital letter marks the bigger quantity
Dr. Karmach

The method

  1. List the pieces: m, c, ΔT = Tfinal − Tinitial. Mark the unknown.
  2. Rearrange for the unknown before numbers go in.
  3. Substitute and cancel units.
  4. Check the sign: cooling means negative ΔT and negative q.
Dr. Karmach

Worked example 1: heat to warm water

q = m · c · ΔT
given: 250 g water · c = 4.184 J/g·°C · 20.0 °C → 50.0 °C · wanted: q

A kettle warms 250 g of water from 20.0 °C to 50.0 °C. How much heat does the water absorb? (c of water: 4.184 J/g·°C)

List the pieces: m, c, and ΔT = Tfinal − Tinitial.

Dr. Karmach

Worked example 1: solution

q = m · c · ΔT
given: 250 g water · c = 4.184 J/g·°C · 20.0 °C → 50.0 °C · wanted: q

Step 1 · List the pieces

m = 250 g. c = 4.184 J/g·°C. ΔT = 50.0 − 20.0 = +30.0 °C. The unknown is q.

Dr. Karmach

Worked example 1: solution

q = m · c · ΔT
given: 250 g water · c = 4.184 J/g·°C · 20.0 °C → 50.0 °C · wanted: q
Step 1 · List the pieces Step 2 · Rearrange for the unknown

q already stands alone on its side of the equation; no rearranging is needed.

Dr. Karmach

Worked example 1: solution

q = m · c · ΔT
given: 250 g water · c = 4.184 J/g·°C · 20.0 °C → 50.0 °C · wanted: q
Step 1 · List the pieces Step 2 · Rearrange for the unknown Step 3 · Substitute and cancel units
q = 250 g × 4.184 J1 g·°C × 30.0 °C = 31,400 J
Dr. Karmach

Worked example 1: solution

q = m · c · ΔT
given: 250 g water · c = 4.184 J/g·°C · 20.0 °C → 50.0 °C · wanted: q
Step 1 · List the pieces Step 2 · Rearrange for the unknown Step 3 · Substitute and cancel units
q = 250 g × 4.184 J1 g·°C × 30.0 °C = 31,400 J
Step 4 · Check the sign
The water warmed, so ΔT and q are both positive: 31,400 J (31.4 kJ) absorbed. More grams or more degrees would cost more heat. ✓
Dr. Karmach

Worked example 1: solving for q

q = m · c · ΔT
given: 250 g water · c = 4.184 J/g·°C · ΔT = +30.0 °C · found: q = 31,400 J

q is the unknown, so no rearranging: m, c and ΔT go straight in. ✓
Dr. Karmach

Worked example 2: find c, identify the substance

q = m · c · ΔT
given: q = 1347 J · m = 125 g · 22.0 °C → 46.0 °C · wanted: c

A 125-g metal block absorbs 1347 J as it warms from 22.0 °C to 46.0 °C. Candidate specific heats, in J/g·°C:

aluminum iron copper gold lead
0.897 0.449 0.385 0.129 0.128

Find the block's specific heat and match it to the table.

Dr. Karmach

Worked example 2: solution

q = m · c · ΔT
given: q = 1347 J · m = 125 g · 22.0 °C → 46.0 °C · wanted: c

Step 1 · List the pieces

q = 1347 J. m = 125 g. ΔT = 46.0 − 22.0 = +24.0 °C. The unknown is c.

Dr. Karmach

Worked example 2: solution

q = m · c · ΔT
given: q = 1347 J · m = 125 g · 22.0 °C → 46.0 °C · wanted: c
Step 1 · List the pieces Step 2 · Rearrange for the unknown
q = m · c · ΔT → c = qm · ΔT

Divide both sides by m·ΔT before any numbers go in.

Dr. Karmach

Worked example 2: solution

q = m · c · ΔT
given: q = 1347 J · m = 125 g · 22.0 °C → 46.0 °C · wanted: c
Step 1 · List the pieces Step 2 · Rearrange for the unknown
q = m · c · ΔT → c = qm · ΔT
Step 3 · Substitute and cancel units
c = 1347 J125 g × 24.0 °C = 0.449 J/g·°C

No unit cancels here; they assemble into J/g·°C: the unit of a specific heat.

Dr. Karmach

Worked example 2: solution

q = m · c · ΔT
given: q = 1347 J · m = 125 g · 22.0 °C → 46.0 °C · wanted: c
Step 1 · List the pieces Step 2 · Rearrange for the unknown
q = m · c · ΔT → c = qm · ΔT
Step 3 · Substitute and cancel units
c = 1347 J125 g × 24.0 °C = 0.449 J/g·°C
0.449 J/g·°C sits in the range of a metal's specific heat, ready to identify. ✓
Dr. Karmach

Worked example 2: identify the metal

c = 0.449 J/g·°C
from q = 1347 J · m = 125 g · ΔT = +24.0 °C, both positive

Match the property

aluminum iron copper gold lead
0.897 0.449 0.385 0.129 0.128

Only iron matches 0.449 J/g·°C. The block is iron.

Dr. Karmach

Worked example 2: identify the metal

c = 0.449 J/g·°C
from q = 1347 J · m = 125 g · ΔT = +24.0 °C, both positive
Match the property
aluminum iron copper gold lead
0.897 0.449 0.385 0.129 0.128

Step 4 · Check the sign

The block warmed: ΔT and q are both positive. Plug back in: 125 g × 0.449 J/g·°C × 24.0 °C returns 1347 J. ✓
Dr. Karmach

Worked example 2: solving for c

q = m · c · ΔT
given: q = 1347 J · m = 125 g · ΔT = +24.0 °C · found: c = 0.449 J/g·°C, iron

c is the unknown. Dividing both sides by m · ΔT isolates it before any numbers go in. ✓
Dr. Karmach

Your turn: mass of ethyl alcohol

q = m · c · ΔT
given: q = 8020 J · c = 2.46 J/g·°C · 18.0 °C → 43.0 °C · wanted: m

Ethyl alcohol (c = 2.46 J/g·°C) absorbs 8020 J and warms from 18.0 °C to 43.0 °C.

m = qc · ΔT = 8020 J J/g·°C × °C = g

Fill in c and ΔT = Tfinal − Tinitial, then compute the mass.

Dr. Karmach

Your turn: mass of ethyl alcohol

q = m · c · ΔT
given: q = 8020 J · c = 2.46 J/g·°C · 18.0 °C → 43.0 °C · wanted: m

Ethyl alcohol (c = 2.46 J/g·°C) absorbs 8020 J and warms from 18.0 °C to 43.0 °C.

m = qc · ΔT = 8020 J J/g·°C × °C = g

Fill in c and ΔT = Tfinal − Tinitial, then compute the mass.

m = 8020 J2.46 J/g·°C × 25.0 °C = 130. g
2.46 J warms one gram by one degree, so 8020 J spread over 25.0 degrees warms about 130 g. ✓
Dr. Karmach

Where this goes wrong

q = m · c · ΔT
250 g water · c = 4.184 J/g·°C · 20.0 → 50.0 °C · correct q = 31,400 J
Leaving out the mass. 4.184 × 30.0 = 126 J is the heat for a single gram. The sample has 250 of them. All three factors multiply: q = m·c·ΔT = 31,400 J.
Leaving out the temperature change. 250 × 4.184 = 1046 J warms the water by one degree only. Multiply by the full ΔT of 30.0 °C.
Dividing by the specific heat. 250 × 30.0 ÷ 4.184 = 1790, and its units are g²·°C²/J, not joules. c multiplies on top: (4.184 J / 1 g·°C).
Subtracting the temperatures in the wrong order. ΔT = 20.0 − 50.0 = −30.0 °C gives q = −31,400 J: heat released by water that is warming. ΔT is Tfinal − Tinitial.
Dr. Karmach

Practice 1

q = m · c · ΔT
given: 75.0 g copper · c = 0.385 J/g·°C · ΔT = +20.0 °C · wanted: q

A 75.0-g copper fitting warms by 20.0 °C as hot water flows past it. How much heat, in J, does the copper absorb? (c of copper: 0.385 J/g·°C)

  1. 7.70
  2. 28.9
  3. 578
  4. 3.90 × 10³
Dr. Karmach

Practice 1 · answer: C

q = m · c · ΔT
given: 75.0 g copper · c = 0.385 J/g·°C · ΔT = +20.0 °C
q = 75.0 g × 0.385 J1 g·°C × 20.0 °C = 578 J (answer C)

A left out the mass: 0.385 × 20.0 = 7.70 J warms one gram. B left out the temperature change: 75.0 × 0.385 = 28.9 J is one degree's worth. D divided by the specific heat: 75.0 × 20.0 ÷ 0.385 = 3.90 × 10³, with units g²·°C²/J.

Copper takes only 0.385 J per gram per degree, but 75 grams and 20 degrees multiply that into hundreds of joules. ✓
Dr. Karmach

Worked example 3: final temperature of a cooling sample

q = m · c · ΔT
given: 150 g aluminum · c = 0.897 J/g·°C · Tinitial = 95.0 °C · releases 8100 J · wanted: Tfinal

A 150-g aluminum pan lid at 95.0 °C releases 8100 J as it cools. What is its final temperature? (c of aluminum: 0.897 J/g·°C)

A common first attempt: substitute 8100 J with no sign. Test the result.

Dr. Karmach

Worked example 3: solution

q = m · c · ΔT
given: 150 g aluminum · c = 0.897 J/g·°C · Tinitial = 95.0 °C · releases 8100 J · wanted: Tfinal

A common first attempt

ΔT = +8100 J150 g × 0.897 J/g·°C = +60.2 °C → Tfinal = 95.0 + 60.2 = 155.2 °C ✗

A lid that is releasing heat cannot end up hotter. The sign of q was dropped.

Dr. Karmach

Worked example 3: solution

q = m · c · ΔT
given: 150 g aluminum · c = 0.897 J/g·°C · Tinitial = 95.0 °C · releases 8100 J · wanted: Tfinal
A common first attempt
ΔT = +8100 J150 g × 0.897 J/g·°C = +60.2 °C → Tfinal = 95.0 + 60.2 = 155.2 °C ✗
Step 1 · List the pieces

Released heat leaves the sample, so q = −8100 J. m = 150 g. c = 0.897 J/g·°C. The unknown is ΔT, then Tfinal.

Dr. Karmach

Worked example 3: solution

q = m · c · ΔT
given: 150 g aluminum · c = 0.897 J/g·°C · Tinitial = 95.0 °C · releases 8100 J · wanted: Tfinal
A common first attempt
ΔT = +8100 J150 g × 0.897 J/g·°C = +60.2 °C → Tfinal = 95.0 + 60.2 = 155.2 °C ✗
Step 1 · List the pieces Step 2 · Rearrange for the unknown
ΔT = qm · c , then Tfinal = Tinitial + ΔT
With q entered as −8100 J, the formula is set to return a negative ΔT: a temperature drop. ✓
Dr. Karmach

Worked example 3: final temperature

q = −8100 J released · 150 g aluminum · c = 0.897 J/g·°C
Tinitial = 95.0 °C · wanted: Tfinal

Step 3 · Substitute and cancel units

ΔT = −8100 J150 g × 0.897 J/g·°C = −8100 J134.55 J/°C = −60.2 °C
Tfinal = 95.0 °C + (−60.2 °C) = 34.8 °C
Dr. Karmach

Worked example 3: final temperature

q = −8100 J released · 150 g aluminum · c = 0.897 J/g·°C
Tinitial = 95.0 °C · wanted: Tfinal
Step 3 · Substitute and cancel units
ΔT = −8100 J150 g × 0.897 J/g·°C = −8100 J134.55 J/°C = −60.2 °C
Tfinal = 95.0 °C + (−60.2 °C) = 34.8 °C
Step 4 · Check the sign
Released heat means negative q, negative ΔT, and a lower final temperature: 95.0 → 34.8 °C. ✓ The signless route predicted 155.2 °C, a cooling lid ending hotter. ✗
Dr. Karmach

Worked example 3: solving for ΔT, then Tfinal

q = −8100 J · 150 g aluminum · c = 0.897 J/g·°C · Tinitial = 95.0 °C
found: ΔT = −60.2 °C · Tfinal = 34.8 °C

ΔT is a change, not an end point. Tfinal = 95.0 + (−60.2) = 34.8 °C. ✓
Dr. Karmach

Take-home: ΔT is final minus initial

warming: 20.0 °C → 50.0 °C · ΔT = 50.0 − 20.0 = +30.0 °C · q positive
heat absorbed ✓
cooling: 95.0 °C → 34.8 °C · ΔT = 34.8 − 95.0 = −60.2 °C · q negative
heat released ✓

ΔT is always Tfinal − Tinitial, and released heat enters as negative q. The sign is part of the quantity; it records which way the heat flowed.

Dr. Karmach

Practice 2

q = m · c · ΔT
given: 100. g lead · c = 0.128 J/g·°C · 62.0 °C → 22.0 °C · wanted: q

A 100.-g lead sinker at 62.0 °C drops into a stream and cools to 22.0 °C. What is q for the lead, in J? (c of lead: 0.128 J/g·°C)

  1. 512
  2. −512
  3. 12.8
  4. −5.12
Dr. Karmach

Practice 2 · answer: B

q = m · c · ΔT
given: 100. g lead · c = 0.128 J/g·°C · ΔT = 22.0 − 62.0 = −40.0 °C
q = 100. g × 0.128 J1 g·°C × (−40.0 °C) = −512 J (answer B)

A subtracted the temperatures in the wrong order: 62.0 − 22.0 = +40.0 °C gives +512 J, heat absorbed by a cooling sinker. C stopped at m × c: 100. × 0.128 = 12.8 J, one degree's worth with no sign. D left out the mass: 0.128 × (−40.0) = −5.12 J, the heat for a single gram.

The sinker cooled 40 degrees, so it released heat: q must be negative. ✓
Dr. Karmach

Practice 3

q = m · c · ΔT
given: 25.0 g gold · Tinitial = 27.0 °C · absorbs 2.34 kJ · c = 0.129 J/g·°C · wanted: Tfinal

25.0 g of gold at 27.0 °C absorbs 2.34 kJ of heat. What is the final temperature, in °C? (c of gold: 0.129 J/g·°C)

  1. 27.7
  2. 699
  3. 726
  4. 753
  5. 39.1
Dr. Karmach

Practice 3 · answer: D

ΔT = q / (m · c), then Tfinal = Tinitial + ΔT
given: 25.0 g gold · Tinitial = 27.0 °C · q = +2340 J · c = 0.129 J/g·°C
ΔT = 2340 J25.0 g × 0.129 J/g·°C = +725.6 °C → Tfinal = 27.0 + 725.6 = 753 °C (answer D)

A left q in kilojoules: ΔT = 0.726 °C, so 27.7 °C. B subtracted Tinitial: 725.6 − 27.0 = 699 °C; Tfinal = Tinitial + ΔT. C stopped at ΔT: 726 °C is the change, not the final temperature. E multiplied by c: 2340 × 0.129 ÷ 25.0 = 12.07 °C, then 39.1 °C.

A tiny specific heat means a huge swing: over 700 degrees, most of the way to gold's 1064 °C melting point. ✓
Dr. Karmach

Practice 4

q = m · c · ΔT
given: 2.0 kg aluminum pan · 23.0 °C → 180.0 °C · c = 0.89 J/g·°C · wanted: q · the mass arrives in kilograms

A 2.0-kg aluminum pan heats from 23.0 °C to 180.0 °C on a burner. How much heat, in J, does the pan absorb? (c of aluminum: 0.89 J/g·°C)

  1. 280
  2. 1.8 × 10³
  3. 2.8 × 10⁵
  4. 3.2 × 10⁵
Dr. Karmach

Practice 4 · answer: C

q = m · c · ΔT
m = 2.0 kg = 2000 g · c = 0.89 J/g·°C · ΔT = 180.0 − 23.0 = +157.0 °C
q = 2.0 kg × 1000 g1 kg × 0.89 J1 g·°C × 157.0 °C = 279,460 J ≈ 2.8 × 10⁵ J (answer C)

c is per gram, so the kilograms convert inside the chain: 2.0 kg is 2000 g. A used 2.0 as if it were grams: 2.0 × 0.89 × 157.0 = 280 J, a thousand times short. B left out the temperature change: 2000 × 0.89 = 1.8 × 10³ J, one degree's worth. D used 180.0 as ΔT: 2000 × 0.89 × 180.0 = 3.2 × 10⁵ J. ΔT is final minus initial: 157.0 °C.

Two thousand grams climbing 157 degrees, even at aluminum's modest 0.89 J per gram per degree, costs about 280 kJ. ✓
Dr. Karmach

Check yourself

  1. Water cools from 50.0 °C to 20.0 °C. Write ΔT with its sign. What is the sign of q, and what does it say about the heat?
  2. Solve q = m·c·ΔT for m, in symbols. Which units cancel, and which unit survives?

Two samples can receive the same heat and change temperature by different amounts. Equal masses, equal q: the substance with the smaller specific heat shows the larger ΔT.

Dr. Karmach

5 · Comparing Specific Heats

For the same heat, read specific heat in reverse (equal masses, the smaller c means the larger temperature change; unequal masses, compare the whole sample's m·c), confirming with ΔT = q/mc when a number is wanted.

Dr. Karmach

The beach, twelve hours apart

At noon the sand scorches bare feet while the ocean stays cool. By midnight the sand is cold, and the water is the warm place to be.

Dr. Karmach

Same heat and mass: c and ΔT trade off

Give equal masses the same heat. Their temperature changes are not equal. Specific heat sits in the denominator of ΔT = q/mc, so the smaller c, the larger the temperature change.

ΔT = q / (m · c)
same q, same m: c in the denominator: smaller c, larger ΔT
Dr. Karmach

Ranking substances by specific heat

Every substance has its own specific heat; water's is several times any metal's. Higher c, smaller temperature change from the same heat.

water 4.184 · ethyl alcohol 2.46 · aluminum 0.897 · iron 0.449 · copper 0.385 · silver 0.235 · gold 0.129 · lead 0.128
specific heat c, in J/g·°C: smaller c, larger temperature change for the same heat and mass
Dr. Karmach

Why water resists temperature swings

Water soaks up heat with only a small temperature rise and releases it slowly, so coastlines stay mild. The cause is the strong grip between water molecules: hydrogen bonding.

2092 J into 100 g of each: water rises +5.0 °C · iron rises +46.6 °C
water's specific heat is 9.3× iron's, so the same heat moves it 9.3× less
Dr. Karmach

The method

  1. Compare the specific heats. Same heat and mass: smaller c means larger ΔT.
  2. Name the response. The substance with the smaller c swings more.
  3. Confirm with ΔT = q/mc. c and m are in the denominator.
Dr. Karmach

Worked example: when the masses differ

ΔT = q / (m · c)
200 g copper (c = 0.385) and 50.0 g aluminum (c = 0.897) · q = 2000 J each · wanted: which ends hotter

A 200 g copper block and a 50.0 g aluminum block each absorb 2000 J.

A common first answer: copper has the smaller specific heat, so copper wins. Check it: the masses are not equal.

Dr. Karmach

Worked example: solution

ΔT = q / (m · c)
200 g copper (c = 0.385) · 50.0 g aluminum (c = 0.897) · q = 2000 J each

Step 1 · Compare the specific heats

Copper's c, 0.385, is smaller than aluminum's, 0.897. But mass is in the denominator too, and the copper sample is four times heavier.

Dr. Karmach

Worked example: solution

ΔT = q / (m · c)
200 g copper (c = 0.385) · 50.0 g aluminum (c = 0.897) · q = 2000 J each
Step 1 · Compare the specific heats Step 2 · Name the response

Compare the whole sample's m·c: copper 200 × 0.385 = 77.0 J/°C, aluminum 50.0 × 0.897 = 44.85 J/°C. Aluminum's is smaller, so aluminum swings more.

Dr. Karmach

Worked example: solution

ΔT = q / (m · c)
200 g copper (c = 0.385) · 50.0 g aluminum (c = 0.897) · q = 2000 J each
Step 1 · Compare the specific heats Step 2 · Name the response Step 3 · Confirm with ΔT = q/mc
copper: ΔT = 2000 J200 g × 0.385 J/g·°C = 2000 J77.0 J/°C = +26.0 °C
aluminum: ΔT = 2000 J50.0 g × 0.897 J/g·°C = 2000 J44.85 J/°C = +44.6 °C
Dr. Karmach

Worked example: solution

ΔT = q / (m · c)
200 g copper (c = 0.385) · 50.0 g aluminum (c = 0.897) · q = 2000 J each
Step 1 · Compare the specific heats Step 2 · Name the response Step 3 · Confirm with ΔT = q/mc
copper: ΔT = 2000 J200 g × 0.385 J/g·°C = 2000 J77.0 J/°C = +26.0 °C
aluminum: ΔT = 2000 J50.0 g × 0.897 J/g·°C = 2000 J44.85 J/°C = +44.6 °C
Aluminum ends hotter, 44.6 °C against 26.0 °C, even though copper has the smaller specific heat. When the masses differ, compare m·c, not c alone. ✓
Dr. Karmach

Worked example: the route on the strip

ΔT = q / (m · c)
given: 200 g copper · 50.0 g aluminum · 2000 J each · found: copper +26.0 °C · aluminum +44.6 °C

Unequal masses, so compare m·c: aluminum's 44.85 J/°C is the smaller, so aluminum swings more. The equation confirms it. ✓
Dr. Karmach

Take-home: compare m·c, not c alone

200 g copper: m·c = 77.0 J/°C · 50.0 g aluminum: m·c = 44.85 J/°C
same 2000 J: copper +26.0 °C · aluminum +44.6 °C · the smaller m·c swings more

Comparing c alone assumes equal masses. When the masses differ, the whole sample's m·c sets the response: the smaller m·c, the larger the temperature change.

Dr. Karmach

Where this goes wrong

Equal heat, equal temperature. Equal q into equal mass does not give equal ΔT. 1000 J into 50.0 g of water raises it 4.78 °C; the same 1000 J into 50.0 g of copper raises it 51.9 °C. The specific heats differ, so the temperature changes differ.
Right substance, backwards reason. Naming the low-c substance as the one that ends hotter "because it stores more heat per gram." It stores less per gram: lead takes 0.128 J to warm a gram by a degree, aluminum 0.897 J. That low cost per degree is exactly why lead swings more.
Comparing c when the masses differ. The rule "smaller c wins" assumes equal mass. When the masses are not equal, mass is in the denominator too. Compare the whole sample's m·c, or run ΔT = q/mc for each.
Dr. Karmach

Practice

ΔT = q / (m · c)
given: 400. g lead (c = 0.128) · 150. g silver (c = 0.235) · 1200 J each · same start

A 400. g block of lead (c = 0.128 J/g·°C) and a 150. g block of silver (c = 0.235 J/g·°C) start at the same temperature and each absorb 1200 J. Which statement matches the outcome?

  1. Lead warms by about 23.4 °C and silver by about 34.0 °C, so silver ends hotter.
  2. Lead ends hotter: its smaller specific heat turns the same heat into the larger rise.
  3. Both warm by the same amount, since each absorbs the same 1200 J.
  4. Lead warms by about 34.0 °C and silver by about 23.4 °C, so lead ends hotter.
Dr. Karmach

Practice · answer: A

ΔT = q / (m · c) · the masses differ, so compare m·c
lead: 400. × 0.128 = 51.2 J/°C · silver: 150. × 0.235 = 35.25 J/°C · silver's is smaller
lead: ΔT = 1200 J51.2 J/°C = +23.4 °C · silver: ΔT = 1200 J35.25 J/°C = +34.0 °C (answer A)

B compared c alone: "smaller c wins" holds only at equal masses, and the lead block is heavier. C equal heat does not mean equal ΔT: the two samples' m·c differ. D computed both rises and pinned them on the wrong metals.

Silver has the larger c, yet its smaller m·c makes it swing more: 34.0 °C against 23.4 °C. ✓
Dr. Karmach

Extra practice 1

ΔT = q / (m · c)
lead: c = 0.128 J/g·°C · copper: c = 0.385 J/g·°C · equal masses · same heat

Two blocks of equal mass, one lead and one copper, take in the same heat. The lead warms by 36.0 °C. By how much, in °C, does the copper warm?

  1. 36.0
  2. 12.0
  3. 108
  4. 4.61
Dr. Karmach

Extra practice 1 · answer: B

ΔT = q / (m · c) · equal masses, same heat: c alone decides
lead 0.128 · copper 0.385 J/g·°C · copper's c is larger, so copper warms less
q/m = 0.128 × 36.0 = 4.61 J/g  →  copper: ΔT = 4.61 J/g0.385 J/g·°C = +12.0 °C · answer B

A took equal heat as an equal rise: 36.0 °C holds only when the specific heats match. C flipped the ratio: 36.0 × 0.385 / 0.128 = 108, but the larger c gives the smaller rise. D stopped halfway: 0.128 × 36.0 = 4.61 is the heat per gram, in J/g, not copper's rise.

Copper's c is 3.0 times lead's (0.385 / 0.128), so copper warms a third as far: 36.0 / 3.0 = 12.0 °C. ✓
Dr. Karmach

Extra practice 2

q = m · c · ΔT
silver: c = 0.235 J/g·°C · iron: c = 0.449 J/g·°C · 1 cal = 4.184 J

A silver bar and an iron bar, 60.0 g each, both warm by 25.0 °C. How much more heat, in cal, does the iron bar absorb?

  1. 76.7
  2. 321
  3. 1.34 × 10³
  4. 161
Dr. Karmach

Extra practice 2 · answer: A

q = m · c · ΔT · same m and ΔT: the larger c takes more heat
60.0 g each · +25.0 °C each · iron 0.449 · silver 0.235 J/g·°C · 1 cal = 4.184 J
iron: 60.0 × 0.449 × 25.0 = 673.5 J  ·  silver: 60.0 × 0.235 × 25.0 = 352.5 J
673.5 J − 352.5 J = 321 J × 1 cal4.184 J = 76.7 cal · answer A

B stopped in joules: 321 J is the right gap in the wrong unit. C put the factor upside down: 321 × 4.184 = 1.34 × 10³. D never subtracted silver's heat: 673.5 / 4.184 = 161 cal is iron's whole heat.

Iron's c beats silver's by 0.214 J/g·°C. Over 60.0 g and 25.0 °C that is 321 J, about 77 cal. ✓
Dr. Karmach

Extra practice 3

ΔT = q / (m · c), then Tfinal = Tinitial + ΔT
iron: c = 0.449 J/g·°C · aluminum: c = 0.897 J/g·°C

A 140. g iron block at 30.0 °C and a 40.0 g aluminum block at 22.0 °C each absorb 1500. J. Which statement matches the outcome?

  1. Iron ends hotter: it starts warmer, and the same heat gives the same rise.
  2. Iron ends hotter, at 53.9 °C: its smaller specific heat gives the larger rise.
  3. Aluminum ends hotter, at 41.8 °C.
  4. Aluminum ends hotter, at 63.8 °C.
Dr. Karmach

Extra practice 3 · answer: D

ΔT = q / (m · c) · the masses differ, so compare m·c
iron: 140. × 0.449 = 62.86 J/°C · aluminum: 40.0 × 0.897 = 35.88 J/°C · 1500. J each
iron: ΔT = 1500. J62.86 J/°C = +23.9 °C  →  30.0 °C + 23.9 °C = 53.9 °C
aluminum: ΔT = 1500. J35.88 J/°C = +41.8 °C  →  22.0 °C + 41.8 °C = 63.8 °C · answer D

A took equal heat as an equal rise: that holds only when m·c matches, and 62.86 is not 35.88. B compared c alone: iron's 140. g makes its m·c the larger, so it rises only 23.9 °C. C stopped at the rise: 41.8 °C is how far aluminum climbs from 22.0 °C, not where it ends.

Aluminum starts 8.0 °C cooler but climbs about 18 °C further, so it finishes about 10 °C ahead. ✓
Dr. Karmach

Check yourself

  1. Equal masses of copper and water absorb the same heat from the same start. Which ends hotter, and which term in ΔT = q/mc decides it?
  2. Two iron bars, 50 g and 150 g, absorb the same heat. Which shows the larger temperature change, and why?

Heat can also flow in while the thermometer holds still. At 0 °C ice melts, and at 100 °C water boils, with no temperature change at all. That heat goes into changing the phase, and it has its own per-gram price.

Dr. Karmach

6 · Heat of a Phase Change

Find the heat of a phase change with q = mass × ΔH in J/g or q = n × ΔH in kJ/mol, 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

Six changes of state

Changes toward the gas pull particles apart and absorb heat: endothermic. The reverses release that same heat: exothermic. Vaporization is also called evaporation. Dry ice goes straight from solid to gas; so does iodine warmed gently.

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 same heats, per mole

q = n × ΔH
for water: ΔHfus = 6.02 kJ/mol · ΔHvap = 40.7 kJ/mol · grams → moles → kilojoules

Phase-change heats also come per mole: 6.02 kJ melts a mole of ice, 40.7 kJ boils a mole of water. A mass in grams becomes moles first; either route lands on the same heat.

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: mass × ΔH (J/g), or moles × ΔH (kJ/mol).
  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 1: the route on the map

q = mass × ΔHfus
given: 60.0 g ice at 0 °C · found: q = +20,100 J

Melting picks ΔHfus and a plus sign. Grams in with a per-gram heat: the top lane, one factor. ✓
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

Worked example 2: the route on the map

q = mass × ΔHvap
given: 20.0 g water at 100 °C · found: q = +45,180 J

Boiling picks ΔHvap. Same top lane as melting; only the factor changed. ✓
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: 5.00 × 10⁴ J absorbed by water at 100 °C · ΔHvap = 2259 J/g · wanted: mass boiled away

A kettle delivers 5.00 × 10⁴ J to water already boiling at 100 °C. What mass of water, in grams, boils away? (ΔHvap of water: 2259 J/g)

  1. 22.1
  2. 149
  3. 1.20 × 10⁴
  4. 1.13 × 10⁸
Dr. Karmach

Practice 1 answer: A

q = mass × ΔHvap
given: 5.00 × 10⁴ J absorbed at 100 °C · ΔHvap = 2259 J/g · wanted: g
5.00 × 10⁴ J × 1 g2259 J = 22.1 g · answer A

The heat is given, so ΔHvap enters upside down: J on the bottom, so joules cancel. B used the heat of fusion: 5.00 × 10⁴ ÷ 335 = 149 g is the ice this heat would melt, not the water it boils. C used water's specific heat: 5.00 × 10⁴ ÷ 4.184 = 1.20 × 10⁴, but a plateau has no ΔT, so c does not apply. D kept the factor right side up: 5.00 × 10⁴ × 2259 = 1.13 × 10⁸, in J²/g, nothing cancels.

Each gram takes 2259 J to boil, so 50,000 J boils a little over 20 g. ✓
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

Worked example 3: the route on the map

q = mass × ΔHvap
given: 8.00 g steam condenses at 100 °C · found: q = −18,072 J

Condensing sits in the releases column: ΔHvap with a minus sign. The route is the top lane, with no m·c·ΔT anywhere. ✓
Dr. Karmach

Worked example 4: melting by the molar route

q = n × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 6.02 kJ/mol · molar mass of water 18.02 g/mol · wanted: q in kJ

60.0 g of ice at 0 °C melts to water. Find the heat with the molar heat of fusion, 6.02 kJ/mol. The heat is per mole, so the grams must become moles first.

Dr. Karmach

Worked example 4: solution

q = n × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 6.02 kJ/mol · molar mass of water 18.02 g/mol

Step 1 · Name the phase change

The ice is melting at 0 °C, the same change as ever. Only the units of its heat are new: kilojoules per mole.

Dr. Karmach

Worked example 4: solution

q = n × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 6.02 kJ/mol · molar mass of water 18.02 g/mol
Step 1 · Name the phase change Step 2 · Pick its ΔH

Melting uses the heat of fusion: ΔHfus = 6.02 kJ/mol.

Dr. Karmach

Worked example 4: solution

q = n × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 6.02 kJ/mol · molar mass of water 18.02 g/mol
Step 1 · Name the phase change Step 2 · Pick its ΔH Step 3 · Multiply
60.0 g × 1 mol18.02 g × 6.02 kJ1 mol = 20.0 kJ

Grams cancel into moles, moles cancel into kilojoules.

Dr. Karmach

Worked example 4: solution

q = n × ΔHfus
given: 60.0 g ice at 0 °C · ΔHfus = 6.02 kJ/mol · molar mass of water 18.02 g/mol
Step 1 · Name the phase change Step 2 · Pick its ΔH Step 3 · Multiply
60.0 g × 1 mol18.02 g × 6.02 kJ1 mol = 20.0 kJ
Step 4 · Set the direction

The per-gram route on the same sample: 60.0 g × 335 J/g = 20,100 J = 20.1 kJ. Two routes, one heat, agreeing to the rounding of the constants.

Melting absorbs heat: q = +20.0 kJ. 3.33 mol of ice at 6.02 kJ each is about 20 kJ, and the 335 J/g route lands on the same number. ✓
Dr. Karmach

Worked example 4: the route on the map

q = n × ΔHfus
given: 60.0 g ice at 0 °C · found: q = +20.0 kJ

Grams given with a heat per mole: the bottom lane, molar mass first, then ΔHfus. Two factors. ✓
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 or q = n × 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 = n × ΔH
given: 15.0 kJ removed from liquid water at 0 °C · ΔHfus = 6.02 kJ/mol · ΔHvap = 40.7 kJ/mol · water 18.02 g/mol · wanted: g of ice

A freezer removes 15.0 kJ of heat from liquid water at 0 °C. What mass of ice, in grams, forms?

  1. 6.64
  2. 44.9
  3. 0.138
  4. 2.49
Dr. Karmach

Practice 2 answer: B

q = n × ΔHfus
freezing is melting reversed: the fusion heat applies · 15.0 kJ released by the water · 18.02 g/mol
15.0 kJ × 1 mol6.02 kJ × 18.02 g1 mol = 44.9 g · answer B

The heat is given, so ΔHfus enters upside down and kJ cancels. A picked the vaporization heat: 15.0 ÷ 40.7 × 18.02 = 6.64 g, but no boiling or condensing happens here. C divided by the molar mass: 2.49 ÷ 18.02 = 0.138 g. D stopped at moles: 2.49 mol of water, one factor short of grams.

Freezing releases heat, so q for the water is −15.0 kJ; the mass of ice is positive. 2.49 mol at 18.02 g each is about 45 g. ✓
Dr. Karmach

Practice 3

q = mass × ΔH
given: 28.0 g boiled vs 28.0 g melted · ΔHfus = 335 J/g · ΔHvap = 2259 J/g · wanted: difference

How much more heat, in joules, does it take to boil away 28.0 g of water at 100 °C than to melt 28.0 g of ice at 0 °C?

  1. 7.26 × 10⁴
  2. 6.74
  3. 6.33 × 10⁴
  4. 5.39 × 10⁴
Dr. Karmach

Practice 3 answer: D

q = mass × ΔH, once for each change
28.0 g · boil: ΔHvap = 2259 J/g · melt: ΔHfus = 335 J/g · wanted: boil minus melt
28.0 g × 2259 J1 g = 63,252 J  ·  28.0 g × 335 J1 g = 9,380 J
63,252 J − 9,380 J = 5.39 × 10⁴ J · answer D

A added the two heats: 63,252 + 9,380 = 7.26 × 10⁴ J is the cost of both changes, not the gap. B divided the heats: 2259 ÷ 335 = 6.74 says how many times more, not how many joules more. C stopped at the boiling heat: 28.0 × 2259 = 6.33 × 10⁴ J, with the melt never subtracted.

Each gram costs 2259 − 335 = 1924 J more to boil than to melt. 28.0 g of that is about 54,000 J. ✓
Dr. Karmach

Practice 4

q = n × ΔH
given: 62.0 g C₂H₅OH boiled · ΔHvap of ethanol = 38.6 kJ/mol · wanted: q in kJ

A still boils off 62.0 g of ethanol, C₂H₅OH, at its boiling point. How much heat, in kJ, does the ethanol absorb?

  1. 51.9
  2. 2.39 × 10³
  3. 133
  4. 1.10 × 10⁵
Dr. Karmach

Practice 4 answer: A

q = n × ΔHvap
boiling: the vaporization heat applies · 62.0 g C₂H₅OH · 38.6 kJ/mol · molar mass from the formula

Two conversion factors are needed, and the first one is ethanol's molar mass: 2(12.01) + 6(1.008) + 16.00 = 46.07 g/mol.

62.0 g × 1 mol46.07 g × 38.6 kJ1 mol = 51.9 kJ · answer A

B skipped the molar mass: 62.0 × 38.6 = 2.39 × 10³, as if each gram were a mole. C used water's molar mass: 62.0 ÷ 18.02 × 38.6 = 133, but the liquid is ethanol. D put the molar mass upside down: 62.0 × 46.07 × 38.6 = 1.10 × 10⁵, and grams do not cancel.

Boiling absorbs heat: q = +51.9 kJ. About 1.35 mol at about 39 kJ each is about 52 kJ. ✓
Dr. Karmach

Practice 5

q = mass × ΔHfus, then q = m · c · ΔT
given: 32.0 g ice melts · the same heat instead goes into 400. g water at 21.0 °C · ΔHfus = 335 J/g · c = 4.184 J/g·°C

Melting 32.0 g of ice at 0 °C takes a certain heat. If that same heat instead warmed 400. g of water at 21.0 °C, what final temperature, in °C, would the water reach?

  1. 6.41
  2. 101.1
  3. 27.4
  4. 64.2
Dr. Karmach

Practice 5 answer: C

q = mass × ΔHfus, then ΔT = q ÷ (m · c)
32.0 g ice melts · the same heat instead goes into 400. g water at 21.0 °C · 335 J/g · 4.184 J/g·°C
32.0 g × 335 J1 g = 10,720 J  →  ΔT = 10,720 J400. g × 4.184 J/g·°C = 6.41 °C
Tfinal = 21.0 °C + 6.41 °C = 27.4 °C · answer C

A stopped at ΔT: 6.41 °C is the rise, not the final temperature. B warmed the ice's 32.0 g: 21.0 + 10,720 ÷ (32.0 × 4.184) = 101.1, but the 400. g of water takes the heat. D used the heat of vaporization: 32.0 × 2259 = 72,288 J, giving 64.2, but nothing boils.

The water took in heat instead of the ice, so 27.4 °C sits above 21.0 °C. ✓
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

7 · 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) = 2.03 · c(liquid water) = 4.184 · c(steam) = 1.9 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. Ice and steam sit near 2 J/g·°C; only liquid water earns 4.184.

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 1: the route on the curve

total q = melt + warm
given: 30 g ice at 0 °C → liquid water at 25 °C · found: q = 13,188 J

The ice starts on the plateau, so no ice warms. Two pieces: melt, then warm water. ✓
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 plateau-times-ΔT shortcut, 603,000 J, was about 27 times too large. ✓
Dr. Karmach

Worked example 2: the route on the curve

total q = melt + warm
given: 45 g ice at 0 °C → liquid water at 40 °C · found: q = 22,606 J

The same two pieces. Only the slope carries a ΔT; the plateau is m·ΔHfus alone. ✓
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) 2.03 · c(water) 4.184 · c(steam) 1.9 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 × 2.03 J1 g·°C × 20 °C = 812 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 2.03, 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 812 · 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 × 1.9 J1 g·°C × 20 °C = 760 J
Dr. Karmach

Worked example 3: boiling, then the total

total q = warm ice + melt + warm water + boil + warm steam
warm ice 812 · 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 × 1.9 J1 g·°C × 20 °C = 760 J
Step 3 · Add every piece
q = 812 + 6700 + 8368 + 45,180 + 760 = 61,820 J
Boiling alone is 45,180 J, about three-quarters of the total. Vaporizing water takes the most heat. ✓
Dr. Karmach

Worked example 3: the route on the curve

total q = warm ice + melt + warm water + boil + warm steam
given: 20 g ice at −20 °C → steam at 120 °C · found: q = 61,820 J

The whole curve: three slopes, each with its own c, and both plateaus. ✓
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) 2.03 · 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 2.03: 20 g × 2.03 × 20 °C = 812 J.
Dr. Karmach

Practice 1

total q = melt + warm
given: 20.0 g ice at 0 °C → liquid water at 30.0 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C · wanted: q

A 20.0 g block of ice at 0 °C is melted and warmed to 30.0 °C. How much heat, in J, does it take?

  1. 2.51 × 10³
  2. 6.70 × 10³
  3. 9.21 × 10³
  4. 2.01 × 10⁵
Dr. Karmach

Practice 1 answer: C

total q = melt + warm
given: 20.0 g ice at 0 °C → liquid water at 30.0 °C · ΔHfus = 335 J/g · c(water) = 4.184 J/g·°C
melt: 20.0 g × (335 J / 1 g) = 6.70 × 10³ J · warm: 20.0 g × 4.184 J/(g·°C) × 30.0 °C = 2.51 × 10³ J
q = 6.70 × 10³ J + 2.51 × 10³ J = 9.21 × 10³ J · answer C

A skipped the melting plateau: 20.0 × 4.184 × 30.0 = 2.51 × 10³ J warms the liquid but never melts the ice. B stopped at the melting point: 20.0 × 335 = 6.70 × 10³ J leaves the water at 0 °C. D multiplied the plateau by a ΔT: 20.0 × 335 × 30.0 = 2.01 × 10⁵ J.

Melting and warming are two separate costs, so both add ✓
Dr. Karmach

Practice 2

total q = cool steam + condense + cool water
given: 10.0 g steam at 115 °C → liquid water at 70.0 °C · c(steam) 1.9 · c(water) 4.184 J/g·°C · ΔHvap 2259 J/g · wanted: q, signed

A 10.0 g sample of steam at 115 °C cools, condenses, and ends as liquid water at 70.0 °C. What is q for the sample, in J?

  1. +2.41 × 10⁴
  2. −1.54 × 10³
  3. −2.29 × 10⁴
  4. −2.41 × 10⁴
Dr. Karmach

Practice 2 answer: D

total q = cool steam + condense + cool water
given: 10.0 g · 115 °C → 70.0 °C · c(steam) 1.9 · c(water) 4.184 J/g·°C · ΔHvap 2259 J/g · ΔT = Tfinal − Tinitial
cool steam: 10.0 g × 1.9 × (100 − 115) °C = −285 J · condense: −(10.0 g × 2259 J/g) = −22,590 J · cool water: 10.0 g × 4.184 × (70.0 − 100) °C = −1255 J
q = −285 J + (−22,590 J) + (−1255 J) = −24,130 J = −2.41 × 10⁴ J · answer D

A lost the sign: a cooling path releases heat, so q is negative. B skipped the condensation plateau: −285 − 1255 = −1.54 × 10³ J. C stopped at 100 °C: −285 − 22,590 = −2.29 × 10⁴ J.

Heating curve run backward: every step is negative, condensing dominates ✓
Dr. Karmach

Practice 3

total q = cool water + freeze
given: 50.0 g liquid water at 22.0 °C → ice at 0 °C · c(water) 4.184 · c(ice) 2.03 J/g·°C · ΔHfus 335 J/g · wanted: q, signed

A bottle holding 50.0 g of water at 22.0 °C goes into a freezer and ends as ice at 0 °C. What is q for the water, in J?

  1. −1.68 × 10⁴
  2. +2.14 × 10⁴
  3. −4.60 × 10³
  4. −2.14 × 10⁴
  5. −1.90 × 10⁴
Dr. Karmach

Practice 3 answer: D

total q = cool water + freeze
given: 50.0 g · 22.0 °C → ice at 0 °C · c(water) 4.184 J/g·°C · ΔHfus 335 J/g · ΔT = Tfinal − Tinitial
cool water: 50.0 g × 4.184 J/(g·°C) × (0 − 22.0) °C = −4602 J
freeze: −(50.0 g × 335 J/g) = −16,750 J
q = −4602 J + (−16,750 J) = −21,352 J = −2.14 × 10⁴ J · answer D

A skipped the cooling leg: −16,750 J = −1.68 × 10⁴ J. B lost the sign: the water releases heat, so q is negative. C skipped the freezing plateau: −4.60 × 10³ J. E cooled the liquid with ice's c: 50.0 × 2.03 × (−22.0) − 16,750 = −1.90 × 10⁴ J.

Freezing releases more than three times the heat of the cooling. ✓
Dr. Karmach

Practice 4

total q = the sum of every segment crossed
given: 35.0 g ice at −25.0 °C → steam at 110.0 °C · c(ice) 2.03 · c(water) 4.184 · c(steam) 1.9 J/g·°C · ΔHfus 335 · ΔHvap 2259 J/g · wanted: q in kJ

A 35.0 g block of ice at −25.0 °C is heated until it is steam at 110.0 °C. How much heat, in kJ, does it absorb?

  1. 96.2
  2. 115
  3. 108
  4. 1.08 × 10⁵
  5. 28.1
Dr. Karmach

Practice 4 answer: C

given: 35.0 g ice, −25.0 °C → steam, 110.0 °C · c(ice) 2.03 · c(water) 4.184 · c(steam) 1.9 J/g·°C · ΔHfus 335 · ΔHvap 2259 J/g
warm ice: 35.0 × 2.03 × 25.0 = 1776 J · melt: 35.0 × 335 = 11,725 J
warm water: 35.0 × 4.184 × 100 = 14,644 J · boil: 35.0 × 2259 = 79,065 J
warm steam: 35.0 × 1.9 × 10.0 = 665 J · q = 107,875 J = 108 kJ · answer C

A skipped the melt: 107,875 − 11,725 = 96.2 kJ. B used 110.0 °C as the steam's ΔT: 35.0 × 1.9 × 110.0 = 7315 J, total 115 kJ. D left the total in joules: 1.08 × 10⁵. E stopped before boiling: 1776 + 11,725 + 14,644 = 28.1 kJ.

Boiling alone is 79.1 kJ, nearly three-quarters of the total. ✓
Dr. Karmach

Practice 5

heat absorbed = the sum of every segment crossed
given: 25.0 g ice at −10.0 °C · absorbs 1.500 × 10⁴ J · ends as liquid water · c(ice) 2.03 · c(water) 4.184 J/g·°C · ΔHfus 335 J/g · wanted: Tfinal

A 25.0 g ice cube at −10.0 °C absorbs 1.500 × 10⁴ J and ends as liquid water. What is its final temperature, in °C?

  1. 63.3
  2. 58.5
  3. 139
  4. 48.5
  5. 53.3
Dr. Karmach

Practice 5 answer: B

given: 25.0 g ice at −10.0 °C · absorbs 15,000 J · c(ice) 2.03 · c(water) 4.184 J/g·°C · ΔHfus 335 J/g
warm ice: 25.0 × 2.03 × 10.0 = 507.5 J · melt: 25.0 × 335 = 8375 J · left for the water: 15,000 − 507.5 − 8375 = 6117.5 J
ΔT = 6117.5 J25.0 g × 4.184 J/(g·°C) = 58.5 °C · Tfinal = 0 °C + 58.5 °C = 58.5 °C · answer B

A skipped the ice leg: 6625 ÷ 104.6 = 63.3. C skipped the melt: 14,492.5 ÷ 104.6 = 139, past the boiling point. D started the water at −10.0 °C: −10.0 + 58.5 = 48.5. E warmed the ice with water's c: 5579 ÷ 104.6 = 53.3.

Melting takes over half the heat. The water warms from 0 °C, not from the ice's start. ✓
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?

Drop a hot metal into cool water and heat leaves the metal and enters the water until both settle at one shared temperature. Mixing two bodies and reading the thermometer is calorimetry: the heat lost equals the heat gained.

Dr. Karmach

8 · Calorimetry

Use an insulated cup to make energy conservation visible (the heat one body loses equals the heat another gains) and solve for a final temperature or a reaction's enthalpy, with the answer's final temperature landing between the two starting temperatures.

Dr. Karmach

How a Calorie gets measured

A food label's Calorie number is not estimated. The food is burned in a sealed chamber, water around it absorbs the heat, and the temperature rise gives the count.

Dr. Karmach

Heat lost equals heat gained

Nest two foam cups, add a lid and a thermometer, and almost no heat escapes. Whatever heat the hot object loses, the water gains. The two settle at one shared temperature.

Dr. Karmach

Energy is conserved in the cup

Inside the insulated cup, the energy that leaves one body enters the other. Energy is conserved: none is created or destroyed.

qA + qB = 0 → qA = −qB
each body: q = m·c·ΔT with ΔT = Tf − Ti · one q comes out negative: that body released the heat
Dr. Karmach

The final temperature sits between

Both bodies end at the same temperature. It lands between the two starting temperatures, pulled toward whichever body carries the larger m·c: usually the water.

Dr. Karmach

The method

  1. Set the balance: qA = −qB, ΔT = Tf − Ti each.
  2. Solve without expanding: Tf = the m·c-weighted average.
  3. Check: Tf between the starts; heat lost = heat gained.
Dr. Karmach

Two routes on the map

Top row: with Tf unknown, the m·c-weighted average gives it in one move. Bottom row: the solution's q = m·c·ΔT, one sign flip for the reaction's heat, then ÷ moles for ΔH.

Dr. Karmach

Worked example 1: mixing hot and cold water

qhot = −qcold · ΔT = Tf − Ti on both sides
given: 150 g water at 70 °C · 100 g water at 20 °C · wanted: Tf

Pour 150 g of water at 70 °C into 100 g at 20 °C. Both are water, so both specific heats are 4.184. Find the final temperature.

Dr. Karmach

Worked example 1: solution

qhot = −qcold · ΔT = Tf − Ti on both sides
150 g water at 70 °C · 100 g water at 20 °C · same c = 4.184, cancels

Step 1 · Set the balance

Each body keeps its own ΔT = Tf − Ti: 150 · (Tf − 70) = −100 · (Tf − 20). The hot side's ΔT will come out negative; the minus sign hands its released heat to the cold side.

Dr. Karmach

Worked example 1: solution

qhot = −qcold · ΔT = Tf − Ti on both sides
150 g water at 70 °C · 100 g water at 20 °C · same c = 4.184, cancels
Step 1 · Set the balance Step 2 · Solve without expanding
Tf = 150 × 70 + 100 × 20150 + 100 = 12,500250 = 50.0 °C

The balance point is the mass-weighted average of the two starting temperatures. No distributing, no collecting terms: the masses weight the two starts directly.

Dr. Karmach

Worked example 1: solution

qhot = −qcold · ΔT = Tf − Ti on both sides
150 g water at 70 °C · 100 g water at 20 °C · same c = 4.184, cancels
Step 1 · Set the balance Step 2 · Solve without expanding
Tf = 150 × 70 + 100 × 20150 + 100 = 12,500250 = 50.0 °C
Step 3 · Check
50.0 °C lands between 20 and 70, closer to 70 because the hotter sample is heavier. And the books balance: the hot water released 150 × 4.184 × 20.0 = 12,552 J, the cold water absorbed 100 × 4.184 × 30.0 = 12,552 J. Heat lost = heat gained. ✓
Dr. Karmach

Worked example 1: the route on the map

qhot = −qcold
given: 150 g water at 70 °C · 100 g water at 20 °C · found: Tf = 50.0 °C

With Tf unknown, neither q can come first. One move, the m·c-weighted average, gives Tf directly. ✓
Dr. Karmach

Worked example 2: a hot bolt in water

qiron = −qwater · ΔT = Tf − Ti on both sides
given: 100 g iron at 90 °C · 150 g water at 20 °C · c: iron 0.449, water 4.184 · wanted: Tf

A 100 g iron bolt at 90 °C drops into 150 g of water at 20 °C.

A common first attempt: add the two heats. Test the result against the thermometer.

Dr. Karmach

Worked example 2: solution

qiron = −qwater · ΔT = Tf − Ti on both sides
100 g iron at 90 °C · 150 g water at 20 °C

A common first attempt

adding the heats: Tf = 14.6 °C ✗
14.6 °C is below both 20 °C and 90 °C: no shared temperature sits outside the pair

Same signs on both heats is the slip. One body loses, the other gains.

Dr. Karmach

Worked example 2: solution

qiron = −qwater · ΔT = Tf − Ti on both sides
100 g iron at 90 °C · 150 g water at 20 °C
A common first attempt
adding the heats: Tf = 14.6 °C ✗
14.6 °C is below both 20 °C and 90 °C: no shared temperature sits outside the pair
Step 1 · Set the balance
44.9 × (Tf − 90) = −627.6 × (Tf − 20)
The two m·c terms are set: iron's 100 × 0.449 = 44.9 against the water's 150 × 4.184 = 627.6, each with its own Tf − Ti. The iron's ΔT will come out negative. ✓
Dr. Karmach

Worked example 2: the final temperature

qiron = −qwater · ΔT = Tf − Ti on both sides
m·c: iron 44.9, water 627.6 · start 90 °C and 20 °C

Step 2 · Solve without expanding

Tf = 44.9 × 90 + 627.6 × 2044.9 + 627.6 = 24.7 °C
24.7 °C sits between 20 and 90, close to the water: its m·c of 627.6 dwarfs the iron's 44.9. ✓
Dr. Karmach

Worked example 2: the route on the map

qiron = −qwater
given: 100 g iron at 90 °C · 150 g water at 20 °C · found: Tf = 24.7 °C

The same one move as two water samples. Only the m·c weights changed. ✓
Dr. Karmach

Take-home: one loses, the other gains

heat lost by the hot body = heat gained by the cold body
Tf always lands between the two starting temperatures

Never add the two heats. One body releases, the other absorbs. Set the loss equal to the gain, and a final temperature outside the starting pair means a dropped sign.

Dr. Karmach

Your turn: aluminum into water

Drop 80 g aluminum (c = 0.897) at 100 °C into 200 g water at 22 °C. Fill the m·c terms into the weighted average that solves qAl = −qwater.

Tf = × 100 + × 22 + = °C
Dr. Karmach

Your turn: aluminum into water

Drop 80 g aluminum (c = 0.897) at 100 °C into 200 g water at 22 °C. Fill the m·c terms into the weighted average that solves qAl = −qwater.

Tf = × 100 + × 22 + = °C
Tf = 71.76 × 100 + 836.8 × 2271.76 + 836.8 = 28.2 °C
Between 22 and 100, and close to 22: the water's m·c of 836.8 far outweighs the aluminum's 71.76. ✓
Dr. Karmach

Worked example 3: enthalpy from a temperature rise

q = m·c·ΔT, then ΔH = −q / moles
given: 100.0 g solution · 20.0 → 26.8 °C · 0.0500 mol reacted · wanted: ΔH per mole

An acid and a base neutralize in a cup holding 100.0 g of solution. The temperature climbs from 20.0 to 26.8 °C, and 0.0500 mol of water forms. Find ΔH per mole.

Dr. Karmach

Worked example 3: solution

q = m·c·ΔT, then ΔH = −q / moles
100.0 g solution · ΔT = +6.8 °C · 0.0500 mol

Two moves are needed.

Step 1 · Heat gained by the solution

q = 100.0 g × 4.184 J/g·°C × 6.8 °C = 2845 J
Dr. Karmach

Worked example 3: solution

q = m·c·ΔT, then ΔH = −q / moles
100.0 g solution · ΔT = +6.8 °C · 0.0500 mol
Two moves are needed. Step 1 · Heat gained by the solution
q = 100.0 g × 4.184 J/g·°C × 6.8 °C = 2845 J
Step 2 · Heat per mole of reaction
ΔH = −2845 J0.0500 mol = −56,900 J/mol = −56.9 kJ/mol
The solution warmed, so the reaction released heat: ΔH is negative, exothermic. ✓
Dr. Karmach

Worked example 3: the route on the map

qreaction = −qsolution · ΔH = qreaction ÷ moles
given: 100.0 g solution, 20.0 → 26.8 °C · 0.0500 mol · found: ΔH = −56.9 kJ/mol

Step 1 of the solution is arrow 1: the solution's q. Step 2 is arrows 2 and 3: flip the sign, then divide by the moles. ✓
Dr. Karmach

Two calorimeters, two jobs

bomb calorimeter: sealed steel, constant volume
combustion and food Calories · the whole rig warms: q = Ccal · ΔT
coffee-cup calorimeter: open cup, constant pressure
neutralization, dissolving, mixing · the heat measured here equals ΔH · a dissolving salt's heat, cold pack or hot pack, gets its number this way

Combustion runs in the sealed bomb at constant volume. Solution chemistry runs in the open cup at constant pressure, where q equals ΔH. Burn it in the bomb; mix it in the cup.

Dr. Karmach

Worked example 4: a bomb calorimeter run

qreleased = Ccal · ΔT
given: 1.0 g fructose burned · Ccal = 9.90 kJ/°C · ΔT = +1.58 °C · wanted: heat released

1.0 g of fructose burns in a bomb calorimeter whose heat capacity is Ccal = 9.90 kJ/°C. The temperature climbs 1.58 °C. How much heat did the combustion release?

Dr. Karmach

Worked example 4: solution

qreleased = Ccal · ΔT
1.0 g fructose · Ccal = 9.90 kJ/°C · ΔT = +1.58 °C

One heat capacity for the whole rig

The bomb, the water, the walls: Ccal covers all of it at once, 9.90 kJ per degree. No mass and no specific heat are needed; Ccal already contains them.

Dr. Karmach

Worked example 4: solution

qreleased = Ccal · ΔT
1.0 g fructose · Ccal = 9.90 kJ/°C · ΔT = +1.58 °C
One heat capacity for the whole rig Multiply by the temperature rise
q = 9.90 kJ1 °C × 1.58 °C = 15.6 kJ
Dr. Karmach

Worked example 4: solution

qreleased = Ccal · ΔT
1.0 g fructose · Ccal = 9.90 kJ/°C · ΔT = +1.58 °C
One heat capacity for the whole rig Multiply by the temperature rise
q = 9.90 kJ1 °C × 1.58 °C = 15.6 kJ
Set the direction
The calorimeter warmed, so the combustion released the heat: qrxn = −15.6 kJ for one gram of fructose. That is 15.6 ÷ 4.184 = 3.74, nearly 4 food Calories per gram: the carbohydrate number on every label, measured. ✓
Dr. Karmach

Where this goes wrong

100 g iron at 90 °C into 150 g water at 20 °C → Tf = 24.7 °C
the correct final temperature both bodies reach
Ignoring the water's share. Assuming the metal just cools to the water's temperature gives Tf = 20 °C. The water warms too; its gain is part of the balance.
Adding the two heats. Same sign on both sides gives Tf = 14.6 °C, below both starting temperatures. One body loses heat, the other gains it: heat lost = heat gained.
Swapping the masses onto the wrong specific heats. Pairing 150 with the iron and 100 with the water gives Tf = 29.7 °C. Each mass keeps its own substance's c.
Dr. Karmach

Practice 1

heat lost = heat gained
given: 60.0 g copper at 120.0 °C · 125 g water at 25.0 °C · c: copper 0.385, water 4.184 · wanted: Tf

A 60.0 g copper block at 120.0 °C drops into 125 g of water at 25.0 °C. What final temperature, in °C, do they reach?

  1. 29.0
  2. 40.3
  3. 55.8
  4. 72.5
Dr. Karmach

Practice 1 · answer: A

heat lost = heat gained
m·c: copper 60.0 × 0.385 = 23.1 · water 125 × 4.184 = 523 · start 120.0 °C and 25.0 °C
Tf = 23.1 × 120.0 + 523 × 25.023.1 + 523 = 29.0 °C (answer A)

B swapped the masses onto the wrong specific heats: 40.3 °C. C dropped the specific heats and weighted by mass alone: (60.0 × 120.0 + 125 × 25.0) ÷ 185 = 55.8 °C, a shortcut that works only when both bodies are water. D took the plain average of the starts: (120.0 + 25.0) ÷ 2 = 72.5 °C, as if the two bodies weighed the same and shared one c.

29.0 °C sits between 25 and 120, close to the water: its m·c of 523 outweighs the copper's 23.1. ✓
Dr. Karmach

Practice 2

qmetal = −qwater · ΔT = Tf − Ti on both sides
given: 95.0 g metal at 99.0 °C · 40.0 g water at 18.0 °C · measured: Tf = 34.5 °C · wanted: c of the metal

A 95.0 g sample of an unknown metal at 99.0 °C drops into 40.0 g of water at 18.0 °C. Both settle at 34.5 °C. What is the metal's specific heat, in J/g·°C?

  1. −0.451
  2. 2.76 × 10³
  3. 0.843
  4. 0.451
  5. 2.54
Dr. Karmach

Practice 2 · answer: D

qmetal = −qwater · ΔT = Tf − Ti on both sides
water: 40.0 g · ΔT = 34.5 − 18.0 = +16.5 °C · metal: 95.0 g · ΔT = 34.5 − 99.0 = −64.5 °C
qwater = 40.0 g × 4.184 J/g·°C × 16.5 °C = 2761 J → c = −2761 J95.0 g × (−64.5 °C) = 0.451 J/g·°C (answer D)

A dropped the minus in qmetal = −qwater: 2761 ÷ (95.0 × (−64.5)) = −0.451, a negative specific heat. B stopped at qwater: 2761 J, before dividing by the metal's m·ΔT. C used the final temperature as the metal's ΔT: 2761 ÷ (95.0 × 34.5) = 0.843. E swapped the two masses: −(95.0 × 4.184 × 16.5) ÷ (40.0 × (−64.5)) = 2.54.

The metal fell 64.5 °C while the water rose only 16.5 °C: the metal's m·c, 95.0 × 0.451 = 42.8, is about a quarter of the water's 167. A c near 0.45, like iron's, fits. ✓
Dr. Karmach

Practice 3

qreleased = n × |ΔH|, then the calorimeter constant Ccal = q / ΔT
given: 0.562 g carbon burns · C + O₂ → CO₂ · ΔH = −393.5 kJ/mol · 26.74 °C → 27.93 °C · wanted: Ccal

0.562 g of carbon burns in a bomb calorimeter: C + O₂ → CO₂, ΔH = −393.5 kJ/mol. The temperature climbs from 26.74 °C to 27.93 °C. What is the calorimeter constant, in kJ per °C?

  1. 15.5
  2. 18.4
  3. 186
  4. 0.659
Dr. Karmach

Practice 3 · answer: A

C + O₂ → CO₂ · ΔH = −393.5 kJ/mol
0.562 g C burned · ΔT = 27.93 − 26.74 = +1.19 °C
q = 0.562 g × 1 mol12.01 g × 393.5 kJ1 mol = 18.4 kJ → Ccal = 18.4 kJ1.19 °C = 15.5 kJ/°C (answer A)

B stopped at the heat: 18.4 kJ is q, not a calorimeter constant. C skipped the mole conversion: 0.562 × 393.5 ÷ 1.19 = 186 treats the grams as moles. D divided by the final temperature: 18.4 ÷ 27.93 = 0.659; the divisor is ΔT = 1.19 °C.

A reaction with a known ΔH calibrates the rig: 18.4 kJ went in and the temperature rose 1.19 °C, so the calorimeter soaks up 15.5 kJ per degree. That one number is the calorimeter constant; run the same calibration on a coffee cup and it goes by the cup constant, Kcup. ✓
Dr. Karmach

Check yourself

  1. A hot metal is dropped into cool water in an insulated cup. Write the conservation law that relates the heat the metal loses to the heat the water gains.
  2. A final temperature comes out below both starting temperatures. What went wrong, and what does the correct answer always sit between?

A reaction releases a fixed amount of heat per mole, and the calorimeter is how that number gets measured. Written beside its balanced equation as ΔH, it becomes a conversion factor as real as any molar mass.

Dr. Karmach

9 · Thermochemical Equations

Treat ΔH as tied to the equation as written: reverse the equation and flip its sign, scale the coefficients and scale ΔH in step, and use ΔH as a conversion factor to find the heat released or absorbed by a given amount of substance.

Dr. Karmach

The gas bill charges for heat

The utility charges for energy delivered, not the gas itself. Burning a set amount of fuel releases a set amount of heat, and the bill counts that heat.

Dr. Karmach

ΔH is tied to the equation as written

A thermochemical equation pairs a balanced equation with its ΔH. That ΔH belongs to those exact coefficients and states. Change the equation, and ΔH changes with it.

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · ΔH = −890 kJ
−890 kJ is released when 1 mol CH₄ burns exactly as written
Dr. Karmach

Reverse the equation, flip the sign

Running a reaction backward reverses its heat flow. A release becomes an equal absorption. The magnitude is unchanged; only the sign flips.

H₂O(l) → H₂(g) + ½ O₂(g) · ΔH = +286 kJ
forward, ΔH = −286 kJ (released) · reversed, ΔH = +286 kJ (absorbed)
Dr. Karmach

Scale the coefficients, scale ΔH

ΔH is proportional to the amount reacting. Double every coefficient and twice as much reacts, so ΔH doubles. Halve them and ΔH halves.

2 H₂(g) + O₂(g) → 2 H₂O(l) · ΔH = −572 kJ
from H₂ + ½ O₂ → H₂O, ΔH = −286 kJ, scaled ×2
Dr. Karmach

ΔH is a conversion factor

The coefficients turn ΔH into a factor: kJ per mole of any species in the equation. Chain it with molar mass to move between grams of fuel and kilojoules of heat.

Dr. Karmach

The method

  1. Match the target to the given. Reverse the equation if the target runs backward.
  2. Flip the sign for a reversal; scale ΔH by the factor that scales the coefficients.
  3. For heat, use ΔH as kJ per mole and cancel units.
Dr. Karmach

Worked example 1: reversing an equation

C(s) + O₂(g) → CO₂(g) · ΔH = −394 kJ
given: this equation and ΔH · wanted: ΔH for the reverse

Carbon burns to carbon dioxide, releasing 394 kJ. What is ΔH for the reverse, CO₂(g) → C(s) + O₂(g)?

Dr. Karmach

Worked example 1: solution

C(s) + O₂(g) → CO₂(g) · ΔH = −394 kJ
forward: 394 kJ released

Step 1 · Match the target to the given

The target runs the other way: CO₂ breaks apart into C and O₂. It is the reverse.

Dr. Karmach

Worked example 1: solution

C(s) + O₂(g) → CO₂(g) · ΔH = −394 kJ
forward: 394 kJ released
Step 1 · Match the target to the given Step 2 · Flip the sign
CO₂(g) → C(s) + O₂(g) · ΔH = +394 kJ
−394 kJ released → +394 kJ absorbed · same magnitude, opposite sign
Splitting CO₂ must cost exactly the energy its formation released. ✓
Dr. Karmach

Worked example 2: reverse and scale

H₂(g) + ½ O₂(g) → H₂O(l) · ΔH = −286 kJ
given: this equation and ΔH · wanted: ΔH for 2 H₂O(l) → 2 H₂(g) + O₂(g)

Find ΔH for 2 H₂O(l) → 2 H₂(g) + O₂(g).

A common first attempt: flip the sign but leave the coefficients' change out of ΔH. Test it.

Dr. Karmach

Worked example 2: solution

H₂(g) + ½ O₂(g) → H₂O(l) · ΔH = −286 kJ
target: 2 H₂O(l) → 2 H₂(g) + O₂(g)

Step 1 · Match the target to the given

The target is reversed and every coefficient is doubled. Two changes, so ΔH takes two steps.

Dr. Karmach

Worked example 2: solution

H₂(g) + ½ O₂(g) → H₂O(l) · ΔH = −286 kJ
target: 2 H₂O(l) → 2 H₂(g) + O₂(g)
Step 1 · Match the target to the given Step 2 · Flip the sign, then scale ΔH
ΔH = −(2 × −286 kJ) = +572 kJ
Flip only: +286 kJ ✗. Scale only: −572 kJ ✗. Both moves give +572 kJ: forming 2 mol water released 572 kJ, so splitting it absorbs 572 kJ. ✓
Dr. Karmach

Take-home: reverse flips, scale multiplies

flip the arrow, flip the sign · scale the equation, scale the ΔH
reversed: ΔH × (−1) · scaled by n: ΔH × n · do both when both apply

Each change to the equation changes ΔH. Reversing flips the sign. Scaling multiplies. A target that is both reversed and doubled needs both moves. Say the rule until it is automatic.

Dr. Karmach

Your turn: reverse and scale

Given 2 SO₂(g) + O₂(g) → 2 SO₃(g), ΔH = −198.2 kJ, find ΔH for 4 SO₃(g) → 4 SO₂(g) + 2 O₂(g) (reversed and doubled).

ΔH = ( × −198.2 kJ) = kJ
Dr. Karmach

Your turn: reverse and scale

Given 2 SO₂(g) + O₂(g) → 2 SO₃(g), ΔH = −198.2 kJ, find ΔH for 4 SO₃(g) → 4 SO₂(g) + 2 O₂(g) (reversed and doubled).

ΔH = ( × −198.2 kJ) = kJ
ΔH = −(2 × −198.2 kJ) = +396.4 kJ
Reversed, so the sign flips; doubled, so ×2. Forming 4 mol SO₃ released 396.4 kJ, so the reverse absorbs it. ✓
Dr. Karmach

Worked example 3: grams of fuel to kilojoules

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · ΔH = −890 kJ
given: 40.0 g CH₄ burned · molar mass CH₄ = 16.04 g/mol · wanted: ΔH

Burn 40.0 g of methane completely. What is ΔH for this amount of fuel?

Two conversion factors are needed: grams to moles, then moles to kilojoules.

Dr. Karmach

Worked example 3: solution

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · ΔH = −890 kJ
40.0 g CH₄ · 16.04 g/mol · −890 kJ per 1 mol CH₄

Two conversion factors are needed.

Step 1 · Pick the ΔH orientation

Two orientations exist. Only the one canceling mol CH₄ is used: −890 kJ / 1 mol CH₄, not 1 mol CH₄ / −890 kJ.

Dr. Karmach

Worked example 3: solution

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · ΔH = −890 kJ
40.0 g CH₄ · 16.04 g/mol · −890 kJ per 1 mol CH₄
Two conversion factors are needed. Step 1 · Pick the ΔH orientation Step 2 · Chain grams → moles → kilojoules
40.0 g × 1 mol16.04 g × −890 kJ1 mol = −2220 kJ
40.0 g is about 2.5 mol, each releasing 890 kJ: ΔH ≈ −2220 kJ, about 2200 kJ given off. ✓
Dr. Karmach

Worked example 3: the route on the map

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · ΔH = −890 kJ
given: 40.0 g CH₄ · found: −2220 kJ

Grams in hand: two arrows, two conversion factors. Molar mass first, then ΔH per mole of CH₄. ✓
Dr. Karmach

Worked example 4: when the coefficient is 2

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH = −198.2 kJ
given: 87.9 g SO₂ · molar mass SO₂ = 64.07 g/mol · wanted: heat evolved in kJ

Calculate the heat evolved when 87.9 g of sulfur dioxide is converted to sulfur trioxide.

Same chain as the methane problem, with one difference: −198.2 kJ does not belong to 1 mol of SO₂. Tempting: use it per mole anyway. Test it.

Dr. Karmach

Worked example 4: solution

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH = −198.2 kJ
87.9 g SO₂ · 64.07 g/mol · −198.2 kJ per 2 mol SO₂

Step 1 · Write ΔH per mole of SO₂

−198.2 kJ is the heat for the equation as written, which burns 2 mol of SO₂. Per mole of SO₂ that is −198.2/2 = −99.1 kJ. Keeping −198.2 per mole doubles the answer to −272 kJ: wrong.

Dr. Karmach

Worked example 4: solution

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH = −198.2 kJ
87.9 g SO₂ · 64.07 g/mol · −198.2 kJ per 2 mol SO₂
Step 1 · Write ΔH per mole of SO₂ Step 2 · Chain grams → moles → kilojoules
87.9 g × 1 mol SO₂64.07 g × −198.2 kJ2 mol SO₂ = −136 kJ
87.9 g is about 1.4 mol of SO₂, each releasing about 99 kJ: near −140 kJ. ✓
Dr. Karmach

Worked example 4: the route on the map

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH = −198.2 kJ
given: 87.9 g SO₂ · found: −136 kJ

The same two arrows as the methane route. Only the ΔH factor changes: −198.2 kJ per 2 mol SO₂. ✓
Dr. Karmach

Take-home: divide by the coefficient

−198.2 kJ per 2 mol SO₂ = −99.1 kJ per 1 mol SO₂
the kJ-per-mole factor for any species: ΔH over that species' coefficient

ΔH belongs to the whole equation, not to any one substance. The conversion factor puts the species' coefficient under ΔH. A coefficient of 1 hides the division; a 2 does not.

Dr. Karmach

Where this goes wrong

from H₂ + ½ O₂ → H₂O(l), ΔH = −286 kJ, find 2 H₂O(l) → 2 H₂ + O₂
correct: reverse and double → ΔH = +572 kJ
Forgetting to flip the sign. Scaling but keeping the original sign gives −572 kJ. The target is the reverse, so the sign must flip: +572 kJ.
Forgetting to scale. Flipping the sign but leaving the coefficients out gives +286 kJ. Every coefficient doubled, so ΔH doubles: +572 kJ.
Leaving ΔH unchanged. Copying −286 kJ ignores both moves. The equation was reversed and doubled; ΔH must be too.
Dr. Karmach

Practice 1

N₂(g) + O₂(g) → 2 NO(g) · ΔH = +180 kJ
given: this equation and ΔH · wanted: ΔH for 4 NO(g) → 2 N₂(g) + 2 O₂(g)

What is ΔH, in kJ, for 4 NO(g) → 2 N₂(g) + 2 O₂(g)?

  1. +360
  2. −360
  3. −180
  4. +180
Dr. Karmach

Practice 1 · answer: B

N₂(g) + O₂(g) → 2 NO(g) · ΔH = +180 kJ
target: 4 NO → 2 N₂ + 2 O₂ · reversed and ×2
ΔH = −(2 × 180 kJ) = −360 kJ (answer B)

A scaled but kept the sign: 2 × 180 = +360 kJ. C flipped the sign but did not scale: −180 kJ. D left ΔH untouched at +180 kJ.

Forming 2 mol NO absorbed 180 kJ, so making 4 mol the reverse way releases twice that: −360 kJ. ✓
Dr. Karmach

Practice 2

2 Mg(s) + O₂(g) → 2 MgO(s) · ΔH = −1203 kJ
given: 2.50 × 10² kJ released · molar mass Mg 24.31 g/mol · wanted: g Mg

A magnesium flare burns white-hot. What mass of magnesium, in grams, must burn to release 2.50 × 10² kJ?

  1. 10.1
  2. 5.05
  3. 0.416
  4. 0.0171
Dr. Karmach

Practice 2 · answer: A

2 Mg(s) + O₂(g) → 2 MgO(s) · ΔH = −1203 kJ
2.50 × 10² kJ released · 1203 kJ per 2 mol Mg · Mg = 24.31 g/mol
2.50 × 10² kJ × 2 mol Mg1203 kJ × 24.31 g Mg1 mol Mg = 10.1 g Mg (answer A)

B kept 1203 kJ per 1 mol Mg: 2.50 × 10² ÷ 1203 × 24.31 = 5.05 g, half the true mass, because the equation burns 2 mol. C stopped at moles: 2.50 × 10² × 2/1203 = 0.416 mol Mg, one factor short of grams. D divided by the molar mass instead of multiplying: 0.416 ÷ 24.31 = 0.0171 g.

One mole of Mg releases about 600 kJ, so 250 kJ takes about 0.4 mol, near 10 g at 24 g each. ✓
Dr. Karmach

Practice 3

2 C₈H₁₈(l) + 25 O₂(g) → 16 CO₂(g) + 18 H₂O(l) · ΔH = −10,941 kJ
given: 35.0 g octane burned · molar mass C₈H₁₈ = 114.22 g/mol · wanted: ΔH in kJ, sign included

A lawn-mower engine burns 35.0 g of octane. What is ΔH, in kJ, for burning this amount?

  1. −5.60 × 10⁻⁵
  2. 0.306
  3. +1.68 × 10³
  4. −1.68 × 10³
  5. −3.35 × 10³
Dr. Karmach

Practice 3 · answer: D

2 C₈H₁₈(l) + 25 O₂(g) → 16 CO₂(g) + 18 H₂O(l) · ΔH = −10,941 kJ
35.0 g C₈H₁₈ · 114.22 g/mol · −10,941 kJ per 2 mol C₈H₁₈
35.0 g × 1 mol C₈H₁₈114.22 g × −10,941 kJ2 mol C₈H₁₈ = −1.68 × 10³ kJ (answer D)

A flipped the ΔH factor: 0.306 mol × (2 mol / −10,941 kJ) = −5.60 × 10⁻⁵, and mol never cancels. B stopped at moles: 35.0 ÷ 114.22 = 0.306 mol, one factor short of kilojoules. C dropped the sign: combustion releases heat, so ΔH is negative. E used −10,941 kJ per 1 mol: 0.306 × (−10,941) = −3.35 × 10³ kJ, double the answer, because the equation burns 2 mol.

Per mole of octane the heat is −10,941 ÷ 2 = −5470.5 kJ, and 0.306 mol is under a third of a mole: about 1680 kJ released. ✓
Dr. Karmach

Check yourself

  1. An equation is reversed and its coefficients tripled. What two changes apply to ΔH?
  2. A reaction releases 500 kJ per mole. Write the conversion factor that turns moles of it into kilojoules, and state which unit cancels.

A single reaction's ΔH can be reversed and scaled. Adding several such equations, each reversed or scaled to line up, builds the ΔH of a reaction never measured directly: Hess's law.

Dr. Karmach

10 · Hess's Law

Use Hess's law to find the enthalpy of an overall reaction, rearranging the given thermochemical equations, reversing and scaling each ΔH in step, then adding so that everything cancels except the target.

Dr. Karmach

Two trails, one altitude gain

Two trails climb from the same trailhead to the same summit. The altitude gained is identical for both. Enthalpy changes work the same way.

Dr. Karmach

Enthalpy is a state function

A state function depends only on the start and the end, never on the route. Burning carbon to CO₂ releases 393.5 kJ whether it takes one step or two.

Dr. Karmach

Hess's law: the steps' ΔH values add

C(s) + ½ O₂(g) → CO(g) · −110.5 kJ, then CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ
sum: C(s) + O₂(g) → CO₂(g) · ΔH = −110.5 + (−283.0) = −393.5 kJ

When equations add up to a target reaction, their ΔH values add up to its ΔH. This gives ΔH for reactions no calorimeter can isolate.

Dr. Karmach

Rearrange each given before adding

flip the arrow, flip the sign · scale the equation, scale the ΔH
reversed: ΔH × (−1) · scaled by n: ΔH × n · a reversed and doubled equation needs both moves

Given equations rarely line up as printed. Reverse or scale each one until its species sit where the target needs them, and change its ΔH in step. Say the rule as you work.

Dr. Karmach

The method

C(s) + ½ O₂(g) → CO(g): burning carbon always makes CO₂ too · 2 C(s) + H₂(g) → C₂H₂(g): will not run at all
the indirect route: no calorimeter sees these, so their ΔH is built from combustions that measure cleanly
  1. Match each given to the target. Note the side and coefficient each needs.
  2. Reverse and scale. Flip the sign for a reversal; multiply ΔH with the coefficients.
  3. Add and cancel. Sum equations and ΔH values; shared species cancel.
Dr. Karmach

The method on the map

Thermochemical equations already reversed and scaled one equation at a time. Hess's law asks both questions of every given, then adds the adjusted equations and their ΔH values.

Dr. Karmach

Worked example 1: combining two equations

target: C(s) + ½ O₂(g) → CO(g)
given (1): C(s) + O₂(g) → CO₂(g) · ΔH = −393.5 kJ · given (2): CO(g) + ½ O₂(g) → CO₂(g) · ΔH = −283.0 kJ

Burning carbon always makes some CO₂ alongside the CO, so ΔH for this reaction cannot be measured directly. Find it from the two given equations.

Dr. Karmach

Worked example 1: solution

target: C(s) + ½ O₂(g) → CO(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ

Step 1 · Match each given to the target

C(s) is a reactant in (1): keep (1) as written. CO(g) must end up a product, but (2) consumes it: reverse (2).

Dr. Karmach

Worked example 1: solution

target: C(s) + ½ O₂(g) → CO(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
reversed (2): CO₂(g) → CO(g) + ½ O₂(g) · ΔH = +283.0 kJ
sign flips: −283.0 becomes +283.0 · coefficients unchanged, so no scaling
Dr. Karmach

Worked example 1: solution

target: C(s) + ½ O₂(g) → CO(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
reversed (2): CO₂(g) → CO(g) + ½ O₂(g) · ΔH = +283.0 kJ
sign flips: −283.0 becomes +283.0 · coefficients unchanged, so no scaling
Step 3 · Add and cancel
ΔH = −393.5 kJ + 283.0 kJ = −110.5 kJ
CO₂ and ½ O₂ appear on both sides of the sum and cancel, leaving exactly the target. A −110.5 step then a −283.0 step totals −393.5, the one-step value. ✓
Dr. Karmach

Worked example 1: the route on the map

target: C(s) + ½ O₂(g) → CO(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ

Match on the map

(1) has C(s) on the reactant side, one mole: it passes both questions. (2) has CO(g) on the wrong side: it reverses.

Dr. Karmach

Worked example 1: the route on the map

target: C(s) + ½ O₂(g) → CO(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ
Match on the map Reverse and scale on the map

Only (2) is reversed: −283.0 kJ becomes +283.0 kJ. Every coefficient already matches, so nothing is scaled.

Dr. Karmach

Worked example 1: the route on the map

target: C(s) + ½ O₂(g) → CO(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ
Match on the map Reverse and scale on the map

Only (2) is reversed: −283.0 kJ becomes +283.0 kJ. Every coefficient already matches, so nothing is scaled.

Step 3 adds −393.5 kJ and +283.0 kJ: −110.5 kJ. Scale stays grey, since no given needed it. ✓
Dr. Karmach

Worked example 2: reversing and scaling a given

target: 2 CO(g) + O₂(g) → 2 CO₂(g)
given (1): C(s) + O₂(g) → CO₂(g) · ΔH = −393.5 kJ · given (2): C(s) + ½ O₂(g) → CO(g) · ΔH = −110.5 kJ

Both givens are written per mole of carbon, and the target contains no carbon at all. Find ΔH for the target.

Dr. Karmach

Worked example 2: solution

target: 2 CO(g) + O₂(g) → 2 CO₂(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) C(s) + ½ O₂(g) → CO(g) · −110.5 kJ

Step 1 · Match each given to the target

The target needs 2 CO as reactants: (2) makes CO, so reverse it and double it. The target needs 2 CO₂ as products: double (1).

Dr. Karmach

Worked example 2: solution

target: 2 CO(g) + O₂(g) → 2 CO₂(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) C(s) + ½ O₂(g) → CO(g) · −110.5 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
2 CO(g) → 2 C(s) + O₂(g) · ΔH = −2 × (−110.5) = +221.0 kJ
2 C(s) + 2 O₂(g) → 2 CO₂(g) · ΔH = 2 × (−393.5) = −787.0 kJ
Dr. Karmach

Worked example 2: solution

target: 2 CO(g) + O₂(g) → 2 CO₂(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) C(s) + ½ O₂(g) → CO(g) · −110.5 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
2 CO(g) → 2 C(s) + O₂(g) · ΔH = −2 × (−110.5) = +221.0 kJ
2 C(s) + 2 O₂(g) → 2 CO₂(g) · ΔH = 2 × (−393.5) = −787.0 kJ
Step 3 · Add and cancel
ΔH = 221.0 kJ + (−787.0 kJ) = −566.0 kJ
2 C and one O₂ cancel in the sum, leaving the target. Burning CO to CO₂ releases 283.0 kJ per mole, and 2 × 283.0 = 566.0. ✓
Dr. Karmach

Worked example 2: the route on the map

target: 2 CO(g) + O₂(g) → 2 CO₂(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) C(s) + ½ O₂(g) → CO(g) · −110.5 kJ

(2) takes both moves: CO sits on the wrong side, and the target needs 2 of it. (1) skips the reversal but still doubles. Both givens light up the scale box. ✓
Dr. Karmach

Your turn: sulfur dioxide to sulfur trioxide

target: 2 SO₂(g) + O₂(g) → 2 SO₃(g)
given (1): S(s) + O₂(g) → SO₂(g) · ΔH = −296.8 kJ · given (2): S(s) + 3/2 O₂(g) → SO₃(g) · ΔH = −395.7 kJ

Reverse and double (1), double (2), then add.

ΔH = −(2 × ( kJ)) + 2 × ( kJ) = kJ
Dr. Karmach

Your turn: sulfur dioxide to sulfur trioxide

target: 2 SO₂(g) + O₂(g) → 2 SO₃(g)
given (1): S(s) + O₂(g) → SO₂(g) · ΔH = −296.8 kJ · given (2): S(s) + 3/2 O₂(g) → SO₃(g) · ΔH = −395.7 kJ

Reverse and double (1), double (2), then add.

ΔH = −(2 × ( kJ)) + 2 × ( kJ) = kJ
ΔH = −(2 × (−296.8 kJ)) + 2 × (−395.7 kJ) = 593.6 kJ − 791.4 kJ = −197.8 kJ
Both routes start from sulfur: forming 2 SO₃ directly releases 791.4 kJ, forming 2 SO₂ releases 593.6 kJ, and the target is the step between them. ✓

Dr. Karmach

Where this goes wrong

target: C(s) + ½ O₂(g) → CO(g) · correct: reverse (2), add · ΔH = −110.5 kJ
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) CO(g) + ½ O₂(g) → CO₂(g) · −283.0 kJ
Reversing without flipping the sign. Adding −393.5 and −283.0 unchanged gives −676.5 kJ, the heat of two combustions, not the target. Reversed, (2) contributes +283.0 kJ.
Scaling the equation but not ΔH. A given doubled to fit the target doubles its ΔH too. A reversed and doubled given needs both the flip and the ×2.
Adding before the species line up. If anything besides the target species survives the sum, a given still needs reversing or scaling. Fix the equations first; the ΔH values follow.
Dr. Karmach

Practice 1

target: N₂(g) + 2 O₂(g) → 2 NO₂(g)
given (1): N₂(g) + O₂(g) → 2 NO(g) · ΔH = +180.5 kJ · given (2): 2 NO(g) + O₂(g) → 2 NO₂(g) · ΔH = −114.1 kJ

What is ΔH, in kJ, for the target reaction?

  1. +294.6
  2. +66.4
  3. +180.5
  4. −294.6
Dr. Karmach

Practice 1 · answer: B

target: N₂(g) + 2 O₂(g) → 2 NO₂(g)
(1) +180.5 kJ · (2) −114.1 kJ · 2 NO cancels when the givens are added as written
ΔH = 180.5 kJ + (−114.1 kJ) = +66.4 kJ (answer B)

Neither given needs reversing or scaling. A dropped the minus on (2): 180.5 + 114.1 = +294.6. C stopped at the first given: +180.5 kJ never adds step (2). D flipped (1) instead: −180.5 − 114.1 = −294.6.

Forming NO absorbs more heat than the NO-to-NO₂ step releases, so the overall ΔH stays positive. ✓

Dr. Karmach

Worked example 3: three given equations

target: C(s) + 2 H₂(g) → CH₄(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) H₂(g) + ½ O₂(g) → H₂O(l) · −285.8 kJ · (3) CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · −890.3 kJ

Carbon and hydrogen do not combine cleanly to methane in any calorimeter, but all three combustions are easy to measure. Find ΔH for the target.

Dr. Karmach

Worked example 3: rearranging the givens

target: C(s) + 2 H₂(g) → CH₄(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) H₂(g) + ½ O₂(g) → H₂O(l) · −285.8 kJ · (3) CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · −890.3 kJ

Step 1 · Match each given to the target

C(s): reactant in (1), keep it. 2 H₂: double (2). CH₄ must end up a product: reverse (3).

Dr. Karmach

Worked example 3: rearranging the givens

target: C(s) + 2 H₂(g) → CH₄(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) H₂(g) + ½ O₂(g) → H₂O(l) · −285.8 kJ · (3) CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · −890.3 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
2 H₂(g) + O₂(g) → 2 H₂O(l) · ΔH = 2 × (−285.8) = −571.6 kJ
CO₂(g) + 2 H₂O(l) → CH₄(g) + 2 O₂(g) · ΔH = +890.3 kJ · (1) stays −393.5 kJ
Each ΔH moved with its equation: ×2 for the doubling, a sign flip for the reversal, no change for the equation kept as written. ✓
Dr. Karmach

Worked example 3: adding the three equations

C(s) + O₂ + 2 H₂ + O₂ + CO₂ + 2 H₂O → CO₂ + 2 H₂O + CH₄ + 2 O₂
CO₂, 2 H₂O, and 2 O₂ cancel · left: C(s) + 2 H₂(g) → CH₄(g)

Step 3 · Add and cancel

Dr. Karmach

Worked example 3: adding the three equations

C(s) + O₂ + 2 H₂ + O₂ + CO₂ + 2 H₂O → CO₂ + 2 H₂O + CH₄ + 2 O₂
CO₂, 2 H₂O, and 2 O₂ cancel · left: C(s) + 2 H₂(g) → CH₄(g)

Step 3 · Add and cancel

ΔH = −393.5 kJ + (−571.6 kJ) + 890.3 kJ = −74.8 kJ
Burning the elements releases 965.1 kJ; unburning methane costs 890.3 kJ. The difference, 74.8 kJ, is released. ✓

Dr. Karmach

Worked example 4: halving a given equation

target: 2 C(s, graphite) + H₂(g) → C₂H₂(g)
(1) C(s) + O₂(g) → CO₂(g) · −393.5 kJ · (2) H₂(g) + ½ O₂(g) → H₂O(l) · −285.8 kJ · (3) 2 C₂H₂(g) + 5 O₂(g) → 4 CO₂(g) + 2 H₂O(l) · −2598.8 kJ

Carbon and hydrogen will not combine directly to acetylene, so its formation enthalpy comes from three combustions. Read (3) closely: its −2598.8 kJ belongs to two moles of acetylene, and the target makes one.

Dr. Karmach

Worked example 4: solution

target: 2 C(s, graphite) + H₂(g) → C₂H₂(g)
(1) C + O₂ → CO₂ · −393.5 kJ · (2) H₂ + ½ O₂ → H₂O(l) · −285.8 kJ · (3) 2 C₂H₂ + 5 O₂ → 4 CO₂ + 2 H₂O(l) · −2598.8 kJ

Step 1 · Match each given to the target

The target needs 2 C as reactants: double (1). One H₂: keep (2). C₂H₂ must end up a product, one mole of it: reverse (3) and halve it.

Dr. Karmach

Worked example 4: solution

target: 2 C(s, graphite) + H₂(g) → C₂H₂(g)
(1) C + O₂ → CO₂ · −393.5 kJ · (2) H₂ + ½ O₂ → H₂O(l) · −285.8 kJ · (3) 2 C₂H₂ + 5 O₂ → 4 CO₂ + 2 H₂O(l) · −2598.8 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
2 CO₂(g) + H₂O(l) → C₂H₂(g) + 5/2 O₂(g) · ΔH = +2598.8/2 = +1299.4 kJ
reversed: the sign flips · halved: ΔH halves · flipping without halving carries +2598.8 kJ and lands at +1526.0 kJ, the answer for two moles
Dr. Karmach

Worked example 4: solution

target: 2 C(s, graphite) + H₂(g) → C₂H₂(g)
(1) C + O₂ → CO₂ · −393.5 kJ · (2) H₂ + ½ O₂ → H₂O(l) · −285.8 kJ · (3) 2 C₂H₂ + 5 O₂ → 4 CO₂ + 2 H₂O(l) · −2598.8 kJ
Step 1 · Match each given to the target Step 2 · Reverse and scale
2 CO₂(g) + H₂O(l) → C₂H₂(g) + 5/2 O₂(g) · ΔH = +2598.8/2 = +1299.4 kJ
reversed: the sign flips · halved: ΔH halves · flipping without halving carries +2598.8 kJ and lands at +1526.0 kJ, the answer for two moles
Step 3 · Add and cancel
ΔH = 2 × (−393.5) + (−285.8) + 1299.4 = +226.6 kJ
2 CO₂, H₂O, and 5/2 O₂ cancel, leaving exactly the target. Positive: acetylene sits 226.6 kJ above its elements, and a welding torch gets that stored energy back. ✓
Dr. Karmach

Worked example 4: the route on the map

target: 2 C(s, graphite) + H₂(g) → C₂H₂(g)
(1) C + O₂ → CO₂ · −393.5 kJ · (2) H₂ + ½ O₂ → H₂O(l) · −285.8 kJ · (3) 2 C₂H₂ + 5 O₂ → 4 CO₂ + 2 H₂O(l) · −2598.8 kJ

A scale factor can be less than 1. (3) is written for 2 mol acetylene, so it reverses and halves; (1) doubles; (2) passes straight to the sum. ✓
Dr. Karmach

Practice 2

target: N₂(g) + 2 H₂(g) → N₂H₄(l)
given (1): 2 N₂H₄(l) + 2 O₂(g) → 2 N₂(g) + 4 H₂O(g) · ΔH = −1068.4 kJ · given (2): H₂(g) + ½ O₂(g) → H₂O(g) · ΔH = −241.8 kJ

Hydrazine, a rocket fuel, cannot be made directly from its elements. What is ΔH, in kJ, for the target reaction?

  1. +50.6
  2. +534.2
  3. +584.8
  4. −1017.8
  5. +292.4
Dr. Karmach

Practice 2 · answer: A

reverse, halve (1): N₂(g) + 2 H₂O(g) → N₂H₄(l) + O₂(g) · ΔH = 1068.4/2 = +534.2 kJ
double (2): 2 H₂(g) + O₂(g) → 2 H₂O(g) · ΔH = 2 × (−241.8) = −483.6 kJ · O₂ and 2 H₂O cancel, leaving N₂(g) + 2 H₂(g) → N₂H₄(l)
ΔH = 534.2 kJ + (−483.6 kJ) = +50.6 kJ (answer A)

B stopped after (1): +534.2 kJ never brings in the hydrogen. C reversed (1) but never halved it: 1068.4 − 483.6 = +584.8, and 2 H₂O and O₂ are left over. D halved (1) but never flipped its sign: −534.2 + (−483.6) = −1017.8. E never doubled (2): 534.2 − 241.8 = +292.4.

Dr. Karmach

Practice 2 · answer: A

reverse, halve (1): N₂(g) + 2 H₂O(g) → N₂H₄(l) + O₂(g) · ΔH = 1068.4/2 = +534.2 kJ
double (2): 2 H₂(g) + O₂(g) → 2 H₂O(g) · ΔH = 2 × (−241.8) = −483.6 kJ · O₂ and 2 H₂O cancel, leaving N₂(g) + 2 H₂(g) → N₂H₄(l)
ΔH = 534.2 kJ + (−483.6 kJ) = +50.6 kJ (answer A)
Unburning hydrazine costs more heat than burning the hydrogen returns, so ΔH is positive: N₂H₄ stores energy above its elements. ✓

Dr. Karmach

Practice 3

target: C₃H₆(g) + H₂(g) → C₃H₈(g)
given (1): 2 C₃H₆(g) + 9 O₂(g) → 6 CO₂(g) + 6 H₂O(l) · ΔH = −4116.0 kJ · given (2): C₃H₈(g) + 5 O₂(g) → 3 CO₂(g) + 4 H₂O(l) · ΔH = −2219.9 kJ · given (3): H₂(g) + ½ O₂(g) → H₂O(l) · ΔH = −285.8 kJ

A refinery adds hydrogen to propene to make propane. What is ΔH, in kJ, for the target reaction?

  1. −2181.9
  2. −4563.7
  3. −123.9
  4. −447.7
  5. +161.9
Dr. Karmach

Practice 3 · answer: C

halve (1): C₃H₆(g) + 9/2 O₂(g) → 3 CO₂(g) + 3 H₂O(l) · ΔH = −4116.0/2 = −2058.0 kJ
reverse (2): 3 CO₂(g) + 4 H₂O(l) → C₃H₈(g) + 5 O₂(g) · ΔH = +2219.9 kJ · keep (3): −285.8 kJ · 3 CO₂, 4 H₂O, and 5 O₂ cancel
ΔH = −2058.0 kJ + 2219.9 kJ + (−285.8 kJ) = −123.9 kJ (answer C)

A never halved (1): −4116.0 + 2219.9 − 285.8 = −2181.9. B reversed (2) but kept its sign: −2058.0 − 2219.9 − 285.8 = −4563.7. D reversed the propene equation instead of the propane one: +2058.0 − 2219.9 − 285.8 = −447.7. E stopped before equation (3): −2058.0 + 2219.9 = +161.9, and H₂ never enters.

Dr. Karmach

Practice 3 · answer: C

halve (1): C₃H₆(g) + 9/2 O₂(g) → 3 CO₂(g) + 3 H₂O(l) · ΔH = −4116.0/2 = −2058.0 kJ
reverse (2): 3 CO₂(g) + 4 H₂O(l) → C₃H₈(g) + 5 O₂(g) · ΔH = +2219.9 kJ · keep (3): −285.8 kJ · 3 CO₂, 4 H₂O, and 5 O₂ cancel
ΔH = −2058.0 kJ + 2219.9 kJ + (−285.8 kJ) = −123.9 kJ (answer C)
Propene and hydrogen burn to release 2343.8 kJ; propane burns to release 2219.9 kJ. The difference, 123.9 kJ, is released when the two combine. ✓

Dr. Karmach

Practice 4

(1) 4 NH₃(g) + 5 O₂(g) → 4 NO(g) + 6 H₂O(g) · ΔH = −907 kJ
(2) 2 NO(g) + O₂(g) → 2 NO₂(g) · ΔH = −113 kJ · (3) 3 NO₂(g) + H₂O(l) → 2 HNO₃(aq) + NO(g) · ΔH = −139 kJ

Nitric acid is made industrially in these three steps, with all NO and NO₂ recycled. What is ΔH per mole of HNO₃ produced, in kJ/mol?

  1. −290.
  2. −381
  3. −762
  4. −1,520
Dr. Karmach

Practice 4 · answer: B

(1) + 3 × (2) + 2 × (3) · givens: −907 · −113 · −139 (kJ)
NO: 4 + 2 made, 6 used · NO₂: 6 made, 6 used · both cancel · 4 HNO₃ produced
ΔH = −907 + 3 × (−113) + 2 × (−139) = −1524 kJ −1524 kJ4 mol HNO₃ = −381 kJ/mol (answer B)

A added the givens unscaled, then divided: −907 − 113 − 139 = −1159 kJ, and −1159 kJ ÷ 4 = −290. kJ/mol. C divided by the 2 in equation (3) instead of the 4 in the sum: −762 kJ/mol. D never divided: −1524 kJ, or −1,520 to three figures, is ΔH for four moles.

Tripling (2) makes the 6 NO₂ that (3), doubled, consumes. Every step is exothermic, so the per-mole answer must come out negative. ✓
Dr. Karmach

Check yourself

  1. A given equation must be reversed and tripled before adding. State the two changes to its ΔH.
  2. Two givens sum to the target only if a species cancels. On which sides of the two equations must that species appear?

Methane, acetylene, and hydrazine were each built from their elements. Tabulating one ΔH value per compound turns Hess's law into a single formula: standard enthalpies of formation.

Dr. Karmach

11 · Standard Enthalpies of Formation

Write the thermochemical equation behind a standard enthalpy of formation, assign zero to elements in their standard states, and calculate ΔH°rxn as Σ n·ΔH°f(products) − Σ n·ΔH°f(reactants), in either direction.

Dr. Karmach

One short table, thousands of reactions

Nobody measures the heat of every reaction. Each compound's formation enthalpy is measured once and tabulated, and the table then predicts ΔH for any reaction built from its rows.

Dr. Karmach

Hess's law, run through the elements

(1) H₂(g) + ½ O₂(g) → H₂O(l) · ΔH = −285.8 kJ
(2) H₂(g) + ½ O₂(g) → H₂O(g) · ΔH = −241.8 kJ
target: H₂O(l) → H₂O(g) at 25 °C · reverse (1): +285.8 kJ · add (2): +285.8 + (−241.8) = +44.0 kJ

Both equations build water from the same elements. Reverse one, add the other: the elements cancel. Evaporation absorbs heat, +44.0 kJ. Tabulate each compound's equation from its elements once, and every reaction's ΔH follows.

Dr. Karmach

Standard enthalpy of formation, ΔH°f

H₂(g) + ½ O₂(g) → H₂O(l) · ΔH°f = −285.8 kJ/mol
exactly 1 mol of product · from elements in their most stable forms · at standard conditions: 25 °C, 1 atm

ΔH°f is the enthalpy change when one mole of a compound forms from its elements in their most stable forms at standard conditions. The product's coefficient stays 1; fractions on elements are allowed.

Dr. Karmach

Elements in their standard states: ΔH°f = 0

zero: O₂(g) · N₂(g) · H₂(g) · Cl₂(g) · Br₂(l) · Hg(l) · C(s, graphite) · Fe(s)
not zero: O(g) · O₃(g) · Br₂(g) · Fe(l) · C(s, diamond) · every compound

An element already in its most stable form has nothing to form, so its ΔH°f is zero. The stable form matters: liquid bromine, not gaseous; graphite, not diamond.

Dr. Karmach

One formula replaces the cycle

ΔH°rxn = Σ n·ΔH°f(products) − Σ n·ΔH°f(reactants)
n: the balanced-equation coefficients · Δ = final − initial, so products come first

Every reaction can run through the elements: unbuild the reactants, rebuild the products. Adding the two legs gives products minus reactants.

Dr. Karmach

The method

  1. Balance the equation with states. The state picks the table row.
  2. Look up every ΔH°f. Elements in their standard states count as zero.
  3. Multiply each value by its coefficient.
  4. Subtract: products minus reactants.

Dr. Karmach

Worked example 1: writing a formation equation

wanted: the thermochemical equation for ΔH°f of ammonia · ΔH°f NH₃(g) = −46.1 kJ/mol
reactants: elements in their most stable forms · product coefficient: 1

Write the thermochemical equation whose ΔH is the standard enthalpy of formation of NH₃(g).

Dr. Karmach

Worked example 1: solution

wanted: the formation equation of NH₃(g) · ΔH°f = −46.1 kJ/mol
nitrogen's stable form: N₂(g) · hydrogen's stable form: H₂(g)

Elements in their most stable forms

The reactants are N₂(g) and H₂(g), never lone N or H atoms.

Dr. Karmach

Worked example 1: solution

wanted: the formation equation of NH₃(g) · ΔH°f = −46.1 kJ/mol
nitrogen's stable form: N₂(g) · hydrogen's stable form: H₂(g)
Elements in their most stable forms Exactly one mole of product
½ N₂(g) + 3/2 H₂(g) → NH₃(g) · ΔH = −46.1 kJ
N: 1 = 1 · H: 3 = 3 · NH₃ keeps coefficient 1, so fractions land on the elements
Clearing the fractions gives N₂ + 3 H₂ → 2 NH₃ with ΔH = −92.2 kJ: a valid equation, but for 2 mol, so its ΔH is no longer the per-mole ΔH°f. ✓

Dr. Karmach

Guided example: aluminum burns

4 Al(s) + 3 O₂(g) → 2 Al₂O₃(s)
table: Al(s) 0 · O₂(g) 0 · Al₂O₃(s) −1669.8 (kJ/mol)

Sparklers burn aluminum powder in air. Calculate ΔH°rxn from the table. Run all four steps, even where a value is zero.

Dr. Karmach

Guided example: solution

4 Al(s) + 3 O₂(g) → 2 Al₂O₃(s)
Al: 4 = 4 · O: 6 = 6 · table: Al(s) 0 · O₂(g) 0 · Al₂O₃(s) −1669.8 (kJ/mol)

Step 1 · Balance the equation with states

Four Al and six O on each side. The (s) on Al₂O₃ picks its row.

Dr. Karmach

Guided example: solution

4 Al(s) + 3 O₂(g) → 2 Al₂O₃(s)
Al: 4 = 4 · O: 6 = 6 · table: Al(s) 0 · O₂(g) 0 · Al₂O₃(s) −1669.8 (kJ/mol)
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f

Al(s) and O₂(g) are elements in their standard states: zero. Only Al₂O₃(s) carries a value.

Dr. Karmach

Guided example: solution

4 Al(s) + 3 O₂(g) → 2 Al₂O₃(s)
Al: 4 = 4 · O: 6 = 6 · table: Al(s) 0 · O₂(g) 0 · Al₂O₃(s) −1669.8 (kJ/mol)
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f Step 3 · Multiply each value by its coefficient
products: 2 × (−1669.8 kJ) = −3339.6 kJ · reactants: 4 × 0 + 3 × 0 = 0 kJ
Dr. Karmach

Guided example: solution

4 Al(s) + 3 O₂(g) → 2 Al₂O₃(s)
Al: 4 = 4 · O: 6 = 6 · table: Al(s) 0 · O₂(g) 0 · Al₂O₃(s) −1669.8 (kJ/mol)
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f Step 3 · Multiply each value by its coefficient
products: 2 × (−1669.8 kJ) = −3339.6 kJ · reactants: 4 × 0 + 3 × 0 = 0 kJ
Step 4 · Subtract: products minus reactants
ΔH°rxn = −3339.6 kJ − 0 kJ = −3339.6 kJ
Only the product carries a value, so ΔH°rxn is 2 × ΔH°f of Al₂O₃: its formation equation, doubled. ✓

Dr. Karmach

Worked example 2: ΔH°rxn from the table

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l)
table: CH₄(g) −74.8 · O₂(g) 0 · CO₂(g) −393.5 · H₂O(l) −285.8 (kJ/mol)

Calculate ΔH°rxn for burning one mole of methane, using only the table values.

Dr. Karmach

Worked example 2: solution

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l)
table: CH₄(g) −74.8 · O₂(g) 0 · CO₂(g) −393.5 · H₂O(l) −285.8 (kJ/mol)

Step 1 · Balance the equation with states
Step 2 · Look up every ΔH°f

The equation is balanced, and liquid water picks the −285.8 row. O₂ is an element in its standard state: zero.

Dr. Karmach

Worked example 2: solution

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l)
table: CH₄(g) −74.8 · O₂(g) 0 · CO₂(g) −393.5 · H₂O(l) −285.8 (kJ/mol)
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f Step 3 · Multiply each value by its coefficient
products: −393.5 + 2 × (−285.8) = −965.1 kJ
reactants: −74.8 + 2 × 0 = −74.8 kJ
Dr. Karmach

Worked example 2: solution

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l)
table: CH₄(g) −74.8 · O₂(g) 0 · CO₂(g) −393.5 · H₂O(l) −285.8 (kJ/mol)
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f Step 3 · Multiply each value by its coefficient
products: −393.5 + 2 × (−285.8) = −965.1 kJ
reactants: −74.8 + 2 × 0 = −74.8 kJ
Step 4 · Subtract: products minus reactants
ΔH°rxn = −965.1 kJ − (−74.8 kJ) = −890.3 kJ
Combustion is strongly exothermic. The small negative reactant sum only trims the total. ✓

Dr. Karmach

Your turn: carbon monoxide burns

2 CO(g) + O₂(g) → 2 CO₂(g)
table: CO(g) −110.5 · O₂(g) 0 · CO₂(g) −393.5 (kJ/mol)

Multiply each table value by its coefficient, then subtract.

ΔH°rxn = 2 × ( kJ) − [2 × ( kJ) + 0] = kJ
Dr. Karmach

Your turn: carbon monoxide burns

2 CO(g) + O₂(g) → 2 CO₂(g)
table: CO(g) −110.5 · O₂(g) 0 · CO₂(g) −393.5 (kJ/mol)

Multiply each table value by its coefficient, then subtract.

ΔH°rxn = 2 × ( kJ) − [2 × ( kJ) + 0] = kJ
ΔH°rxn = 2 × (−393.5 kJ) − [2 × (−110.5 kJ) + 0] = −787.0 kJ + 221.0 kJ = −566.0 kJ
Adding carbon's two combustion steps by Hess's law gives the same −566.0 kJ: the table method is Hess's law, pre-packaged. ✓

Dr. Karmach

Where this goes wrong

CH₄(g) + 2 O₂(g) → CO₂(g) + 2 H₂O(l) · correct: ΔH°rxn = −890.3 kJ
table: CH₄ −74.8 · CO₂ −393.5 · H₂O(l) −285.8 · H₂O(g) −241.8 · O₂ 0
Reactants minus products. The reversed subtraction gives +890.3 kJ, a combustion that absorbs heat. Products minus reactants: −890.3 kJ.
Skipping a coefficient. Counting H₂O once gives −393.5 − 285.8 + 74.8 = −604.5 kJ. The 2 multiplies its value: 2 × (−285.8).
Using the wrong state. With the H₂O(g) value the sum is −877.1 + 74.8 = −802.3 kJ, the answer to a different reaction. The equation says liquid: −285.8.
Giving an element a value. O₂(g) is an element in its standard state: it contributes 0 to either sum.
Dr. Karmach

Practice 1

CH₃OH(l): methanol · ΔH°f = −238.7 kJ/mol
elements: C · H · O

Methanol fuels drag racers. Which thermochemical equation has ΔH equal to ΔH°f of CH₃OH(l)?

  1. C(g) + 4 H(g) + O(g) → CH₃OH(l)
  2. CO(g) + 2 H₂(g) → CH₃OH(l)
  3. 2 C(s, graphite) + 4 H₂(g) + O₂(g) → 2 CH₃OH(l)
  4. C(s, graphite) + 2 H₂(g) + ½ O₂(g) → CH₃OH(l)
  5. C(s, diamond) + 2 H₂(g) + ½ O₂(g) → CH₃OH(l)
Dr. Karmach

Practice 1 · answer: D

C(s, graphite) + 2 H₂(g) + ½ O₂(g) → CH₃OH(l) · ΔH = −238.7 kJ (answer D)
C: 1 = 1 · H: 4 = 4 · O: 1 = 1 · reactants: elements in their most stable forms · product: exactly 1 mol

A starts from free gaseous atoms, not C(s, graphite), H₂(g) and O₂(g). B starts from CO, a compound: industry makes methanol this way, but its ΔH is not ΔH°f. C makes 2 mol, so its ΔH is 2 × (−238.7) = −477.4 kJ. E uses diamond, not carbon's most stable form.

One mole of product from elements in their standard states. The ½ on O₂ is allowed. ✓

Dr. Karmach

Practice 2

2 NaHCO₃(s) → Na₂CO₃(s) + H₂O(g) + CO₂(g)
table: NaHCO₃(s) −950.8 · Na₂CO₃(s) −1130.7 · H₂O(g) −241.8 · CO₂(g) −393.5 (kJ/mol)

Using the table values, what is ΔH°rxn, in kJ, for the decomposition of baking soda?

  1. −815.2
  2. −1766.0
  3. +135.6
  4. −135.6
Dr. Karmach

Practice 2 · answer: C

2 NaHCO₃(s) → Na₂CO₃(s) + H₂O(g) + CO₂(g)
products: −1130.7 + (−241.8) + (−393.5) = −1766.0 kJ · reactants: 2 × (−950.8) = −1901.6 kJ
ΔH°rxn = −1766.0 kJ − (−1901.6 kJ) = +135.6 kJ (answer C)

A dropped the coefficient 2 on NaHCO₃: −1766.0 − (−950.8) = −815.2. B stopped at the products' sum: −1766.0, before subtracting the reactants. D subtracted reactants minus products: −135.6.

The oven must keep supplying heat for the powder to break down, so ΔH°rxn is positive: a formation table predicts endothermic reactions too. ✓

Dr. Karmach

Worked example 3: solving for an unknown ΔH°f

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH°rxn = −197.8 kJ
table: SO₂(g) −296.8 · O₂(g) 0 · SO₃(g): not listed

The reaction's ΔH°rxn was measured, but the table has no row for SO₃(g). Find ΔH°f of SO₃(g).

Dr. Karmach

Worked example 3: solution

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH°rxn = −197.8 kJ
table: SO₂(g) −296.8 · O₂(g) 0 · x = ΔH°f of SO₃(g)

Write the formula with x

−197.8 = 2x − [2 × (−296.8) + 0]
products: 2x · reactants: 2 × (−296.8) = −593.6 kJ
Dr. Karmach

Worked example 3: solution

2 SO₂(g) + O₂(g) → 2 SO₃(g) · ΔH°rxn = −197.8 kJ
table: SO₂(g) −296.8 · O₂(g) 0 · x = ΔH°f of SO₃(g)
Write the formula with x
−197.8 = 2x − [2 × (−296.8) + 0]
products: 2x · reactants: 2 × (−296.8) = −593.6 kJ
Solve for x
2x = −197.8 kJ + (−593.6 kJ) = −791.4 kJ x = −395.7 kJ/mol
Run it forward as a check: 2 × (−395.7) − 2 × (−296.8) = −197.8 kJ. ✓

Dr. Karmach

Worked example 4: the thermite reaction

2 Al(s) + Fe₂O₃(s) → Al₂O₃(s) + 2 Fe(l)
table: Al(s) 0 · Fe₂O₃(s) −822.2 · Al₂O₃(s) −1669.8 · Fe(l) +12.40 (kJ/mol) · Al = 26.98 g/mol

Aluminum powder strips the oxygen from iron oxide, leaving molten iron. Calculate the heat released in kJ per gram of aluminum reacted.

Two species here are elements. Tempting: write two zeros. Check each state first.

Dr. Karmach

Worked example 4: solution

2 Al(s) + Fe₂O₃(s) → Al₂O₃(s) + 2 Fe(l)
Al(s) 0 · Fe₂O₃(s) −822.2 · Al₂O₃(s) −1669.8 · Fe(l) +12.40 (kJ/mol) · Al = 26.98 g/mol

Step 1 · Balance the equation with states
Step 2 · Look up every ΔH°f

The states pick the rows. Al(s) is aluminum's standard state: zero. Fe(l) is not iron's: melting costs energy, so it carries +12.40. Calling it zero gives −847.6 kJ, wrong.

Dr. Karmach

Worked example 4: solution

2 Al(s) + Fe₂O₃(s) → Al₂O₃(s) + 2 Fe(l)
Al(s) 0 · Fe₂O₃(s) −822.2 · Al₂O₃(s) −1669.8 · Fe(l) +12.40 (kJ/mol) · Al = 26.98 g/mol
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f Step 3 · Multiply each value by its coefficient
products: −1669.8 + 2 × (+12.40) = −1645.0 kJ
reactants: 2 × 0 + (−822.2) = −822.2 kJ
Dr. Karmach

Worked example 4: solution

2 Al(s) + Fe₂O₃(s) → Al₂O₃(s) + 2 Fe(l)
Al(s) 0 · Fe₂O₃(s) −822.2 · Al₂O₃(s) −1669.8 · Fe(l) +12.40 (kJ/mol) · Al = 26.98 g/mol
Step 1 · Balance the equation with states Step 2 · Look up every ΔH°f Step 3 · Multiply each value by its coefficient
products: −1669.8 + 2 × (+12.40) = −1645.0 kJ
reactants: 2 × 0 + (−822.2) = −822.2 kJ
Step 4 · Subtract: products minus reactants
ΔH°rxn = −1645.0 kJ − (−822.2 kJ) = −822.8 kJ
Strongly exothermic, as anything that leaves its iron molten must be. ✓

Dr. Karmach

Worked example 4: per gram of aluminum

2 Al(s) + Fe₂O₃(s) → Al₂O₃(s) + 2 Fe(l) · ΔH°rxn = −822.8 kJ
−822.8 kJ per 2 mol Al reacted · Al = 26.98 g/mol

Convert the reaction total to a per-gram figure

−822.8 kJ2 mol Al × 1 mol Al26.98 g Al = −822.8 kJ53.96 g Al = −15.25 kJ/g Al
Hot enough that the iron comes out molten. Run that liquid iron into a mold between two rail ends and it cools into a weld: rails are joined this way. ✓

Dr. Karmach

Practice 3

2 C₂H₆(g) + 7 O₂(g) → 4 CO₂(g) + 6 H₂O(l) · ΔH°rxn = −3119.4 kJ
table: CO₂(g) −393.5 · H₂O(l) −285.8 (kJ/mol) · C₂H₆(g): not listed

A burner test measures ethane's combustion enthalpy above. What is ΔH°f of C₂H₆(g), in kJ/mol?

  1. −3204.1
  2. −84.7
  3. −169.4
  4. −338.8
Dr. Karmach

Practice 3 · answer: B

−3119.4 = [4 × (−393.5) + 6 × (−285.8)] − [2x + 7 × 0]
O₂(g) is an element in its standard state: 0 · products: −1574.0 + (−1714.8) = −3288.8 kJ · x = ΔH°f of C₂H₆(g)
2x = −3288.8 kJ − (−3119.4 kJ) = −169.4 kJ x = −84.7 kJ/mol (answer B)

A wrote reactants minus products: −3119.4 = 2x − (−3288.8) gives x = −3204.1. C stopped at 2x: −169.4 kJ belongs to 2 mol of ethane. D multiplied by the 2 instead of dividing: 2 × (−169.4) = −338.8.

Run it forward: 4 × (−393.5) + 6 × (−285.8) − 2 × (−84.7) = −3119.4 kJ. ✓

Dr. Karmach

Practice 4

C₅H₁₂(l) + 8 O₂(g) → 5 CO₂(g) + 6 H₂O(g)
table: C₅H₁₂(l) −146.8 · CO₂(g) −393.5 · H₂O(g) −241.8 · H₂O(l) −285.8 · O₂(g) 0 (kJ/mol)

Pentane burns in a camp stove. What is ΔH°rxn, in kJ?

  1. −3535.5
  2. −3418.3
  3. −3271.5
  4. +3271.5
Dr. Karmach

Practice 4 · answer: C

C₅H₁₂(l) + 8 O₂(g) → 5 CO₂(g) + 6 H₂O(g)
products: 5 × (−393.5) + 6 × (−241.8) = −3418.3 kJ · reactants: −146.8 + 8 × 0 = −146.8 kJ
ΔH°rxn = −3418.3 kJ − (−146.8 kJ) = −3271.5 kJ (answer C)

A took the liquid-water row against the equation's (g): −3535.5. B stopped at the products' sum: 5 × (−393.5) + 6 × (−241.8) = −3418.3, before subtracting the reactant. D subtracted reactants minus products: +3271.5.

Five carbons of fuel against methane's one, so several times methane's 890 kJ, and negative as every combustion must be. ✓

Dr. Karmach

Check yourself

  1. State the two conditions a species must meet for its ΔH°f to equal zero.
  2. A reaction's ΔH°rxn and every ΔH°f except one are known. Outline how to find the missing value.

The table predicts ΔH from tabulated wholes; bond energies tell the same story from inside the molecule, where breaking and making individual bonds sets the size and sign of ΔH.

Dr. Karmach

Can you…?

  • ☐ distinguish heat from work and convert among joules, calories, and Calories?
  • ☐ identify exothermic and endothermic processes from equations, energy diagrams, and the sign of ΔH?
  • ☐ apply q = m·c·ΔT to find heat, mass, specific heat, or temperature change?
  • ☐ compare how specific heats set different substances' temperature response to the same heat?
  • ☐ use calorimetry data to determine the heat of a process or reaction?
  • ☐ reverse and scale thermochemical equations and use ΔH as a conversion factor?
  • ☐ combine reversed and scaled equations with Hess's law to find an overall reaction's enthalpy?
  • ☐ write formation equations and use standard formation enthalpies to find any reaction's enthalpy?
  • ☐ compute heat for melting, vaporizing, or a full heating curve?

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

Dr. Karmach

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip

lecture: skip