Year 11 Chemistry Module 4 ⏱ ~35 min Lesson 2 of 13

Calorimetry — Combustion

Jet fuel releases roughly 43,000 kJ per kilogram. Wood releases about 15,000 kJ. That 3× difference isn't guesswork — it's measured in a calorimeter. The principle is simple: burn the fuel, heat water, and watch the thermometer.

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Think First

Why does a small block of chocolate contain more kilojoules than a whole bowl of lettuce? The answer isn't just about quantity — it's about what the molecules are made of and how much energy is stored in their bonds.

If you burned both in a laboratory, you could measure exactly how much heat each released. How would you design that experiment? What would you actually be measuring, and what would you need to keep constant to make a fair comparison?

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Formula Reference — This Lesson

$q = mc\Delta T$
q = heat energy absorbed by water (J) m = mass of water in calorimeter (g) c = specific heat capacity of water = 4.18 J g⁻¹ K⁻¹ ΔT = temperature change (°C or K — same magnitude)
$\Delta H_c = \dfrac{-q}{n}$
ΔHc = molar enthalpy of combustion (kJ mol⁻¹) q = heat energy in kJ (divide J answer by 1000) n = moles of fuel burned Negative sign: combustion is exothermic — q is positive but ΔHc is negative
$n = \dfrac{m}{M}$
n = moles of fuel burned (mol) m = mass of fuel burned (g) = initial burner mass − final burner mass M = molar mass of fuel (g mol⁻¹)
Full calculation chain:   mass of fuel burned → n (using n = m/M) → q (using q = mcΔT, m = water mass) → ΔHc (using ΔHc = −q/n, with q in kJ)
📖 Know

Key Facts

  • The formulas q = mcΔT and ΔHc = −q/n
  • The components of a spirit burner calorimeter
  • Five sources of error in combustion calorimetry
💡 Understand

Concepts

  • Why 'm' in q = mcΔT is the mass of water, not fuel
  • Why the negative sign appears in ΔHc = −q/n
  • Why experimental ΔHc is always less negative than the accepted value
✅ Can Do

Skills

  • Calculate q and then ΔHc from experimental data in 5 steps
  • Calculate percentage error between experimental and accepted values
  • Identify sources of error and state their directional effect on ΔHc
Key Terms — scan these before reading
Negative signThe negative sign in ΔHc = −q/n converts a positive q into the correct negative ΔHc.
Enthalpy change (ΔH)The heat energy exchanged at constant pressure during a reaction.
ExothermicA reaction releasing heat to surroundings (ΔH < 0).
EndothermicA reaction absorbing heat from surroundings (ΔH > 0).
CalorimetryThe experimental measurement of heat changes during chemical processes.
Hess's LawThe total enthalpy change is independent of the pathway taken.
🔬

The Spirit Burner Calorimeter Setup

The spirit burner calorimeter is a simple, imperfect device — understanding its setup is inseparable from understanding why experimental ΔHc values are always lower than the true value.

Spirit Burner Calorimeter — Components Draught shield Copper calorimeter Water (m = known mass) c = 4.18 J g⁻¹ K⁻¹ Thermometer (bulb submerged) heat transfer Spirit burner + fuel Retort stand / tripod Copper walls m(fuel) = mass before − mass after Weigh burner+fuel before and after burning
Spirit burner calorimeter. The copper cup holds a known mass of water. The fuel burns below, transferring heat upward. The draught shield reduces but does not eliminate heat loss to the surroundings.

Components: spirit burner containing the fuel (e.g. ethanol, methanol), a copper calorimeter holding a known mass of water, a thermometer with its bulb fully submerged, and a draught shield around the apparatus.

Procedure (in order):

  1. Record initial mass of burner + fuel (balance reading before)
  2. Record initial water temperature
  3. Light the burner; burn fuel until a target temperature rise is reached (e.g. ΔT ≈ 10°C)
  4. Extinguish the flame; record final water temperature
  5. Record final mass of burner + fuel (balance reading after)
  6. Calculate: mass of fuel burned = initial mass − final mass

Copper is chosen for the calorimeter because it has high thermal conductivity — heat transfers quickly from the flame to the water, minimising lag between the flame and the thermometer reading.

Weigh the burner before AND after burning. Never estimate or assume the mass of fuel consumed. Evaporation from the wick between weighings adds to the apparent mass lost — always cap the burner immediately after extinguishing the flame to minimise this error.
Common error — not capping the burner: If the burner is left uncapped after the experiment, fuel evaporates from the wick. This makes the recorded mass of fuel burned appear larger than it actually was, giving a falsely small value of n, and therefore a falsely low (less negative) ΔHc.
Bomb calorimeter vs spirit burner: The NESA data sheet gives standard ΔHc values measured in a sealed bomb calorimeter at constant volume under high-pressure oxygen — a far more controlled system. Spirit burner experiments are open-air and always lose significant heat, giving values well below the accepted figure.
COMBUSTION CALORIMETRY — CALCULATION FLOWCHART Measure Δm mass of fuel burned (g) Measure ΔT temperature rise of water (°C) q = mcΔT heat absorbed by water (J) n = m/M moles of fuel burned ΔHc = −q/n molar enthalpy of combustion
CALORIMETRY CALCULATOR — INTERACTIVE Interactive
Adjust mass, specific heat capacity, and ΔT sliders — see q and ΔH update in real time.
02

Sources of Error in Combustion Calorimetry

Every spirit burner experiment gives a ΔHc that is less negative than the true value — the key skill is identifying exactly why, and stating the direction of each error's effect.

The experimental ΔHc is always less negative (lower in magnitude) than the accepted value because heat is lost before it can be transferred to the water. In HSC questions, you must name the specific physical source of error and state its directional effect on the result.

Effect on ΔHc
q too small → |ΔHc| too low
Less energy released → |ΔHc| too low
m(fuel) overestimated → n too large → |ΔHc| too low
q underestimated (not all heat goes to water) → |ΔHc| too low
ΔT underestimated → q too small → |ΔHc| too low
How to Minimise
Draught shield; insulation around calorimeter
Adequate air supply; clean wick
Cap burner immediately after extinguishing
Use thin-walled calorimeter; correct for calorimeter heat capacity
Ensure thermometer bulb is fully submerged in water
Real-World Anchor — Fuel Energy Density: Aviation kerosene (jet fuel) is used instead of petrol in aircraft partly because of its higher molar enthalpy of combustion per unit mass. Calorimetry at industrial scale is how fuel engineers compare and certify fuel grades before use. The spirit burner experiment you're running in class is conceptually identical — just less precise. You'll compare fuel energy densities in Short Answer Q3.
Never write "human error" or "inaccurate measurements" in an HSC answer. These phrases earn zero marks. Always name the specific physical process causing the error (e.g. "heat loss to the surrounding air through the walls of the apparatus") and state its directional effect on ΔHc.

🔧 Worked Examples

Worked Example 1 Calculating q and ΔHc

Problem

A student burns ethanol (C₂H₅OH, M = 46.07 g mol⁻¹) in a spirit burner. The mass of the burner decreases from 152.34 g to 151.62 g. The calorimeter contains 200.0 g of water. The water temperature rises from 19.5°C to 31.2°C. Calculate the molar enthalpy of combustion of ethanol.

Solution

  1. 1
    Mass of fuel burned
    m(fuel) = 152.34 − 151.62 = 0.72 g
    Subtract final burner mass from initial. This is the mass of ethanol consumed.
  2. 2
    Moles of ethanol burned
    $n = \dfrac{m}{M} = \dfrac{0.72}{46.07} = 0.01562 \text{ mol}$
    Use n = m/M with the molar mass of ethanol.
  3. 3
    Temperature change
    ΔT = 31.2 − 19.5 = 11.7°C = 11.7 K
    A change of 1°C equals a change of 1 K — the magnitude is the same.
  4. 4
    Heat absorbed by water
    $q = mc\Delta T = 200.0 \times 4.18 \times 11.7 = 9781 \text{ J} = \mathbf{9.781 \text{ kJ}}$
    Use the mass of water (200.0 g), not the fuel. Divide by 1000 to convert J → kJ.
  5. 5
    Molar enthalpy of combustion
    $\Delta H_c = \dfrac{-q}{n} = \dfrac{-9.781}{0.01562} = \mathbf{-626 \text{ kJ mol}^{-1}}$
    The accepted value is −1367 kJ mol⁻¹. The experimental value is less than half — showing very significant heat loss, typical of spirit burner experiments.
✓ Answer ΔHc(ethanol) = −626 kJ mol⁻¹ (experimental). Accepted: −1367 kJ mol⁻¹.
Worked Example 2 Percentage error & sources of discrepancy

Problem

The accepted molar enthalpy of combustion of methanol (CH₃OH) is −726 kJ mol⁻¹. A student's experiment gave −412 kJ mol⁻¹. (a) Calculate the percentage error. (b) Suggest two specific sources of error that would explain why the experimental value is less negative.

Solution

  1. 1
    Set up percentage error formula
    $\% \text{ error} = \dfrac{|\text{experimental} - \text{accepted}|}{|\text{accepted}|} \times 100$
    Use absolute values — the sign of ΔH does not affect percentage difference.
  2. 2
    Calculate
    $= \dfrac{|-412 - (-726)|}{|-726|} \times 100 = \dfrac{314}{726} \times 100 = \mathbf{43.3\%}$
    A 43% error is large but typical for an open spirit burner experiment — most of the combustion energy escapes to the surroundings before heating the water.
  3. 3
    Two specific sources of error
    (1) Heat loss to surroundings: A large proportion of combustion energy heats the surrounding air and copper walls rather than the water, making q smaller than the true heat released — giving a ΔHc less negative than the accepted value.
    (2) Incomplete combustion: Insufficient oxygen at the flame produces CO instead of CO₂ for some of the combustion. CO releases less energy per mole than complete combustion to CO₂, reducing the total heat released and making ΔHc less negative.
✓ Answer (a) 43.3% error. (b) Heat loss to surroundings; incomplete combustion. Both make ΔHc less negative than the accepted value.

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🧪 Activities

🔬 Activity 1 — Calculate + Interpret

Calorimetry Data Processing

A student burns propan-1-ol (C₃H₇OH, M = 60.10 g mol⁻¹) in a spirit burner. Use the data below to complete the calculation chain.

Value
Column B
  1. a Calculate the mass of propan-1-ol burned and convert to moles.

    m(fuel) = 188.45 − 187.81 = 0.64 g
    n = 0.64 ÷ 60.10 = 0.01065 mol
  2. b Calculate the heat absorbed by the water (q in kJ).

    ΔT = 32.6 − 18.2 = 14.4°C = 14.4 K
    q = mcΔT = 250.0 × 4.18 × 14.4 = 15,048 J = 15.048 kJ
  3. c Calculate the experimental ΔHc and the percentage error compared to the accepted value.

    ΔHc = −q/n = −15.048 ÷ 0.01065 = −1413 kJ mol⁻¹
    % error = |−1413 − (−2021)| ÷ 2021 × 100 = 608 ÷ 2021 × 100 = 30.1%
    The experimental value is about 30% below the accepted value — typical heat loss for a spirit burner setup.

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📊 Activity 2 — Calculate + Interpret

Error Analysis — Which Error Has the Biggest Effect?

A student performs a combustion calorimetry experiment on butanol (C₄H₉OH, M = 74.12 g mol⁻¹). Examine each scenario and determine how the error affects the final ΔHc value.

Scenario: Correct data: 0.80 g butanol burned, 200.0 g water, ΔT = 15.0°C. The student made one error in each case below. For each, calculate the incorrect ΔHc and compare it to the correct value.
  1. 1 The student used m = 0.80 g (mass of fuel) instead of m = 200.0 g in the q = mcΔT step. What ΔHc do they calculate, and is it more or less negative than the correct value?

    Correct calculation:
    n = 0.80/74.12 = 0.01079 mol
    q(correct) = 200.0 × 4.18 × 15.0 = 12,540 J = 12.54 kJ
    ΔHc(correct) = −12.54/0.01079 = −1162 kJ mol⁻¹

    Student's error (m = 0.80 g in q formula):
    q(wrong) = 0.80 × 4.18 × 15.0 = 50.2 J = 0.0502 kJ
    ΔHc(wrong) = −0.0502/0.01079 = −4.65 kJ mol⁻¹

    The student's answer is 250× less negative than the correct value — a massive underestimate caused by using the wrong mass in q = mcΔT.
  2. 2 Due to forgetting to cap the burner, an extra 0.10 g of butanol evaporated after the flame was extinguished. The student records mass of fuel burned as 0.90 g (instead of 0.80 g). How does this affect ΔHc?

    n(wrong) = 0.90/74.12 = 0.01214 mol (overestimated)
    q is unchanged = 12.54 kJ (the water still gained the same heat)
    ΔHc(wrong) = −12.54/0.01214 = −1033 kJ mol⁻¹

    This is less negative than the correct −1162 kJ mol⁻¹. By overestimating n (more moles in the denominator), the ΔHc magnitude is reduced. Evaporation always makes the result less negative — consistent with all errors in combustion calorimetry.

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Interactive — Calorimetry Calculation Stepper
Revisit Your Initial Thinking

Look back at what you wrote in the Think First section. What has changed? What did you get right? What surprised you?

Misconceptions to Fix

Wrong: Incomplete combustion is safer than complete combustion because it produces less CO₂.

Right: Incomplete combustion produces toxic carbon monoxide (CO) and particulate carbon (soot), which are deadly. Complete combustion produces CO₂ and H₂O, which are non-toxic. The goal is always complete combustion for safety and efficiency.

MC

Multiple Choice

5 random questions from a replayable lesson bank — feedback shown immediately

✍️ Short Answer

03

Extended Questions

UnderstandBand 3

6. Explain why, in combustion calorimetry using a spirit burner, the value of 'm' in the formula q = mcΔT must be the mass of water and not the mass of fuel. In your answer, state what q represents and why the specific heat capacity of water is used. 3 MARKS

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ApplyBand 4

7. A student burns 0.85 g of methanol (CH₃OH, M = 32.04 g mol⁻¹) and heats 180.0 g of water from 21.0°C to 34.5°C. (a) Calculate q in kJ. (b) Calculate ΔHc. (c) The accepted value is −726 kJ mol⁻¹. Calculate the percentage error and identify one specific source of error that explains why the experimental value is less negative. 5 MARKS

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EvaluateBand 5

8. Real-World Application: Fuel engineers compare fuels by their molar enthalpy of combustion (ΔHc) per gram (energy density). The table below shows data for three fuels.

FuelFormulaM (g mol⁻¹)ΔHc (kJ mol⁻¹)Energy per gram (kJ g⁻¹)
MethanolCH₃OH32.04−726Calculate
EthanolC₂H₅OH46.07−1367Calculate
Octane (petrol proxy)C₈H₁₈114.23−5471Calculate

(a) Complete the energy per gram column (kJ g⁻¹ = |ΔHc| ÷ M). (3 marks)
(b) Using your calculated values, explain which fuel is most efficient per gram and suggest why octane is preferred in internal combustion engines over methanol. (2 marks) 5 MARKS

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04

Revisit Your Thinking

Go back to your Think First response. Now that you've studied combustion calorimetry:

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✅ Comprehensive Answers

🔬 Activity 1 — Propan-1-ol Calorimetry

(a) m(fuel) = 188.45 − 187.81 = 0.64 g; n = 0.64 ÷ 60.10 = 0.01065 mol

(b) ΔT = 32.6 − 18.2 = 14.4°C = 14.4 K; q = 250.0 × 4.18 × 14.4 = 15,048 J = 15.048 kJ

(c) ΔHc = −15.048 ÷ 0.01065 = −1413 kJ mol⁻¹; % error = |−1413 − (−2021)| ÷ 2021 × 100 = 608/2021 × 100 = 30.1%

📊 Activity 2 — Error Analysis (Butanol)

Correct values: n = 0.80/74.12 = 0.01079 mol; q = 200.0 × 4.18 × 15.0 = 12,540 J = 12.54 kJ; ΔHc(correct) = −12.54/0.01079 = −1162 kJ mol⁻¹

Scenario 1 (wrong m): q(wrong) = 0.80 × 4.18 × 15.0 = 50.16 J = 0.05016 kJ; ΔHc = −0.05016/0.01079 = −4.65 kJ mol⁻¹. Massively underestimated — 250× too small.

Scenario 2 (evaporation): n(wrong) = 0.90/74.12 = 0.01214 mol; q unchanged = 12.54 kJ; ΔHc(wrong) = −12.54/0.01214 = −1033 kJ mol⁻¹. Less negative than correct −1162 — overestimated n means smaller |ΔHc|.

❓ Multiple Choice

1. B — q = mcΔT calculates heat absorbed by the water. 'm' is the mass of water, not fuel.

2. C — Spirit burner calorimeters are open systems; significant heat escapes to the surrounding air before reaching the water, making q (and therefore |ΔHc|) smaller than the true value.

3. B — n = 0.500/100 = 0.00500 mol; q = 150.0 × 4.18 × 8.4 = 5267 J = 5.267 kJ; ΔHc = −5.267/0.00500 = −1053 kJ mol⁻¹.

4. A — Water absorbs heat (q > 0, positive), but the reaction releasing that heat is exothermic (ΔH < 0, negative). The negative sign converts the positive q into the correct negative ΔH.

5. D — Balance imprecision would produce random scatter (some too high, some too low), not a systematic 50% shortfall always in the same direction. The consistent direction of the error — always less negative — points to a systematic source: heat loss. This is the dominant error in spirit burner experiments, far exceeding any contribution from balance precision.

📝 Short Answer Model Answers

Q6 (3 marks): q represents the heat energy absorbed by the water during combustion [1]. 'm' must be the mass of water because q = mcΔT calculates the thermal energy transferred to the water — not to the fuel or the calorimeter [1]. The specific heat capacity of water (c = 4.18 J g⁻¹ K⁻¹) is used because water is the substance being heated, and c tells us how many joules are needed to raise 1 g by 1 K [1].

Q7 (5 marks): (a) ΔT = 34.5 − 21.0 = 13.5°C; q = 180.0 × 4.18 × 13.5 = 10,157 J = 10.157 kJ [1]. (b) n = 0.85/32.04 = 0.02653 mol; ΔHc = −10.157/0.02653 = −383 kJ mol⁻¹ [2 — 1 for n, 1 for ΔHc]. (c) % error = |−383 − (−726)| / 726 × 100 = 343/726 × 100 = 47.2% [1]. Source: heat loss to surroundings — a large proportion of the combustion energy heats the surrounding air rather than the water, making q smaller than the true heat released and ΔHc less negative [1].

Q8 (5 marks): (a) Methanol: 726/32.04 = 22.7 kJ g⁻¹ [1]; Ethanol: 1367/46.07 = 29.7 kJ g⁻¹ [1]; Octane: 5471/114.23 = 47.9 kJ g⁻¹ [1]. (b) Octane is most efficient per gram at 47.9 kJ g⁻¹ — more than twice methanol's 22.7 kJ g⁻¹ [1]. Octane (petrol) is preferred in internal combustion engines because it releases more energy per gram of fuel, allowing vehicles to travel further on the same tank mass — this is the same reason jet fuel (kerosene) is denser in energy than wood or alcohol [1].

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Speed Race

Calorimetry — Combustion

Answer questions on Calorimetry — Combustion before your opponents cross the line. Fast answers = faster car. Pool: lessons 1–2.

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