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Questions on measuring an enthalpy change: calorimetry
The equation q = mcΔT with the mass of water or solution and c = 4.18 J g⁻¹ K⁻¹, converting q to ΔH per mole with the correct sign, ΔH = −mcΔT ÷ n, unequal amounts of acid and alkali and the limiting reagent, why strong acids all give about −57 kJ mol⁻¹ and weak acids less, the polystyrene cup method for neutralisation and displacement, AQA required practical 2 with the cooling-curve extrapolation, the spirit burner method for combustion, and the heat losses and other errors that make measured values too small.
19 original questions · 62 marks · the measuring an enthalpy change: calorimetry notes · Energetics · Flashcards for this unit
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Describe how to determine the enthalpy change for the reaction of zinc with copper(II) sulfate solution, including how the results are processed.
Mark scheme
Indicative content
- a measured volume of copper(II) sulfate solution, for example 25.0 cm³ by pipette, in a polystyrene cup with a lid, supported in a beaker
- zinc powder weighed out in excess, so that copper(II) sulfate is the limiting reagent
- the temperature recorded at regular intervals, such as every 30 s, for a few minutes before adding the zinc, to establish the starting temperature
- the zinc added at a recorded time, with stirring, and the temperature recorded at regular intervals until it has been falling steadily for several minutes
- a graph of temperature against time, with the cooling line extrapolated back to the time of mixing to find ΔT
- q = mcΔT with m the mass of the solution, divided by the amount of copper(II) sulfate in moles, gives ΔH in kJ mol⁻¹ with a negative sign
Levels
- Level 3 (5–6 marks) the measured volume of solution in an insulated cup, zinc in excess, temperature readings before and after mixing at regular intervals, the extrapolated cooling curve to find ΔT, and the processing through q = mcΔT and the moles of the limiting reagent to a negative ΔH are all present
- Level 2 (3–4 marks) the solution, the excess zinc and the temperature rise are measured and q = mcΔT used with moles of copper(II) sulfate; there is no cooling-curve extrapolation, or no readings before mixing
- Level 1 (1–2 marks) zinc is added and the temperature rise measured; the mass in q = mcΔT is often taken as the mass of zinc, and ΔH is left positive
Calculate the enthalpy of neutralisation from the readings in the table. A student put 25.0 cm³ of 2.00 mol dm⁻³ hydrochloric acid in a polystyrene cup and, at 3.0 minutes, added 25.0 cm³ of 2.00 mol dm⁻³ sodium hydroxide solution at the same starting temperature. Use the cooling readings to find ΔT at the time of mixing. c = 4.18 J g⁻¹ K⁻¹.
Time / min Temperature / °C 0.0 19.6 1.0 19.6 2.0 19.6 3.0 alkali added; no reading 3.5 31.8 4.0 32.5 5.0 32.1 6.0 31.7 7.0 31.3 8.0 30.9 Mark scheme
- M1 the cooling line runs through the readings from 4.0 minutes, falling (32.5 − 30.9) ÷ (8.0 − 4.0) = 0.40 °C per minute
- A1 extrapolated to 3.0 minutes it reads 32.5 + 0.40 = 32.9 °C, so ΔT = 32.9 − 19.6 = 13.3 °C; accept 13.2 to 13.4 °C read from a graph
- M1 q = 50.0 × 4.18 × 13.3 = 2780 J, using the total mass of 50.0 g
- M1 amount of water formed = 0.0250 dm³ × 2.00 mol dm⁻³ = 0.0500 mol
- A1 ΔH = −2.780 ÷ 0.0500 = −55.6 kJ mol⁻¹ to three significant figures; a ΔT of 12.9 °C, from the highest reading, loses the second mark but allow error carried forward to −53.9 kJ mol⁻¹
State the equation used to calculate the heat energy transferred in a calorimetry experiment, giving the unit of each quantity, and use it to calculate the heat needed to raise the temperature of 75.0 g of water by 8.4 °C. c = 4.18 J g⁻¹ K⁻¹.
Mark scheme
- B1 q = mcΔT: heat energy = mass × specific heat capacity × temperature change
- B1 q in J, m in g, c in J g⁻¹ K⁻¹ and ΔT in K; accept °C for ΔT, since a change is the same size in both
- M1 q = 75.0 × 4.18 × 8.4
- A1 q = 2.6 × 10³ J, or 2.6 kJ, to two significant figures, matching the 8.4 °C
Calculate the enthalpy of neutralisation from the results in the table, for H₂SO₄(aq) + 2NaOH(aq) → Na₂SO₄(aq) + 2H₂O(l). Take the density of the solution as 1.00 g cm⁻³ and c = 4.18 J g⁻¹ K⁻¹.
Measurement Value Volume of 1.00 mol dm⁻³ sulfuric acid 25.0 cm³ Volume of 1.00 mol dm⁻³ sodium hydroxide 50.0 cm³ Temperature rise 9.1 °C Mark scheme
- M1 q = 75.0 × 4.18 × 9.1 = 2853 J, using the total mass of 75.0 g
- M1 amount of water formed = amount of NaOH = 0.0500 dm³ × 1.00 mol dm⁻³ = 0.0500 mol; accept 2 × n(H₂SO₄)
- M1 ΔH = −2.853 ÷ 0.0500 kJ mol⁻¹
- A1 ΔH = −57 kJ mol⁻¹ to two significant figures; −114 kJ mol⁻¹, per mole of acid, scores the first mark only
Calculate the enthalpy of combustion of propan-1-ol from the spirit burner results in the table. c = 4.18 J g⁻¹ K⁻¹.
Measurement Value Mass of propan-1-ol burned 0.720 g Mass of water in the can 150.0 g Temperature rise of the water 31.0 °C Mr of C₃H₇OH 60.0 Mark scheme
- M1 q = 150.0 × 4.18 × 31.0 = 19 437 J = 19.44 kJ, using the mass of water; reject the mass of fuel in q
- M1 amount of propan-1-ol = 0.720 ÷ 60.0 = 0.0120 mol
- M1 ΔcH = −19.44 ÷ 0.0120 kJ mol⁻¹
- A1 ΔcH = −1.62 × 10³ kJ mol⁻¹, that is −1620 kJ mol⁻¹, to three significant figures
Explain why the enthalpy of combustion of ethanol measured with a spirit burner and a copper can is less exothermic than the data-book value.
Mark scheme
- B1 heat is lost to the surroundings, the air, the can and the clamp, so not all of it warms the water and ΔT is too small
- B1 combustion is incomplete, giving carbon or carbon monoxide, which releases less energy than complete combustion to CO₂
- B1 ethanol evaporates from the wick without burning, so the mass loss overstates the amount burned
- B1 the water formed leaves as steam rather than liquid, so the heat of condensation included in ΔcH° is not collected
Calculate ΔH for Mg(s) + CuSO₄(aq) → MgSO₄(aq) + Cu(s) from the results in the table, in which magnesium powder is in excess. c = 4.18 J g⁻¹ K⁻¹.
Measurement Value Volume of copper(II) sulfate solution 50.0 cm³ Concentration of copper(II) sulfate 0.200 mol dm⁻³ Extrapolated temperature rise 22.8 °C Mark scheme
- M1 q = 50.0 × 4.18 × 22.8 = 4765 J
- M1 amount of CuSO₄, the limiting reagent = 0.0500 × 0.200 = 0.0100 mol
- A1 ΔH = −4.765 ÷ 0.0100 = −477 kJ mol⁻¹ to three significant figures
Calculate the percentage uncertainty in a temperature rise of 6.8 °C measured with a thermometer that has an uncertainty of ±0.1 °C in each reading.
Mark scheme
- M1 ΔT is the difference between two readings, so its uncertainty is 2 × 0.1 = ±0.2 °C
- M1 percentage uncertainty = 0.2 ÷ 6.8 × 100
- A1 percentage uncertainty = ±2.9% to two significant figures; 1.5%, from a single reading, scores zero
Explain why a reaction in solution is carried out in a polystyrene cup with a lid rather than in a glass beaker.
Mark scheme
- B1 polystyrene is a poor conductor of heat, so less heat is lost through the walls to the surroundings
- B1 the lid reduces heat lost from the surface of the solution, by convection and evaporation
- B1 polystyrene has a very small heat capacity, so it absorbs little of the heat released, which q = mcΔT ignores
Explain why the temperature rise in required practical 2 is found by extrapolating the cooling line back to the time of mixing rather than taken from the highest temperature recorded.
Mark scheme
- B1 the reaction takes time to finish, and heat is lost to the surroundings throughout
- B1 so by the time the highest temperature is recorded some heat has already been lost, and that reading is too low
- B1 extending the cooling line back to the time of mixing gives the temperature that would have been reached with no heat lost, so ΔT is larger and more accurate
Suggest three changes to the spirit burner method that would give an enthalpy of combustion closer to the data-book value, and explain how each one helps.
Mark scheme
- B1 a draught screen around the burner and can, which keeps the flame under the can and reduces heat lost to moving air
- B1 a shorter gap between the flame and the base of the can, so less heat warms the air between them
- B1 keeping the cap on the burner except while it burns, so ethanol does not evaporate and the mass loss is only fuel that burned; accept insulating the can, with a lid
Compare the polystyrene cup method with the spirit burner method in terms of heat loss and how close their results come to data-book values.
Mark scheme
- B1 in the cup the heat is released directly into the solution, whereas from a burner it must cross an air gap and the can
- B1 so the burner loses a much larger fraction of the heat, and also suffers incomplete combustion and evaporation
- B1 cup results for neutralisation and displacement are usually within about 10% of the data book, whereas burner results are often much further from it
Explain why the enthalpy of neutralisation of hydrocyanic acid, HCN, by sodium hydroxide is much less exothermic than that of hydrochloric acid.
Mark scheme
- B1 hydrochloric acid is a strong acid, fully dissociated, so its neutralisation is only H⁺(aq) + OH⁻(aq) → H₂O(l)
- B1 hydrocyanic acid is a weak acid, mostly undissociated, so more HCN molecules dissociate as OH⁻ removes the H⁺ ions
- B1 that dissociation takes in energy, so less heat is released overall per mole of water formed; 'weak acids release less energy' alone is not enough
Calculate the enthalpy of neutralisation of nitric acid by potassium hydroxide from the results in the table. Take the density of the solution as 1.00 g cm⁻³ and c = 4.18 J g⁻¹ K⁻¹.
Measurement Value Volume of 1.50 mol dm⁻³ nitric acid 20.0 cm³ Volume of 1.00 mol dm⁻³ potassium hydroxide 40.0 cm³ Temperature rise 6.8 °C Mark scheme
- M1 q = 60.0 × 4.18 × 6.8 = 1705 J, using the total mass of 60.0 g
- M1 n(HNO₃) = 0.0300 mol and n(KOH) = 0.0400 mol, so the acid is limiting and 0.0300 mol of water forms
- A1 ΔH = −1.705 ÷ 0.0300 = −57 kJ mol⁻¹ to two significant figures; dividing by 0.0400 mol gives −43 kJ mol⁻¹ and scores the first mark only
Suggest how the temperature change should be found when ammonium nitrate is dissolved in water in a polystyrene cup, an endothermic change, with readings taken every 30 s.
Mark scheme
- B1 after mixing the temperature falls to a minimum and then rises slowly as heat flows in from the warmer surroundings
- B1 the warming line after the minimum is extrapolated back to the time of mixing
- B1 ΔT is the fall from the starting temperature to that extrapolated value, and ΔH is positive
Give two assumptions made when q = mcΔT is applied to a solution in a polystyrene cup.
Mark scheme
- B1 the density of the solution is 1.00 g cm⁻³, so the mass in grams equals the volume in cm³
- B1 the specific heat capacity of the solution equals that of water, 4.18 J g⁻¹ K⁻¹; allow 'the cup absorbs no heat' as the second assumption
Identify the limiting reagent when 3.00 g of zinc is added to 25.0 cm³ of 0.500 mol dm⁻³ copper(II) sulfate, and justify the answer. Ar of Zn = 65.4.
Mark scheme
- B1 amount of zinc = 3.00 ÷ 65.4 = 0.0459 mol and amount of CuSO₄ = 0.0250 × 0.500 = 0.0125 mol
- B1 the reacting ratio is 1:1, so copper(II) sulfate is the limiting reagent and zinc is in excess
Suggest why, in a displacement reaction, the mass of the zinc is not added to the mass of the solution when q = mcΔT is used.
Mark scheme
- B1 the heat is absorbed almost entirely by the water of the solution, which is the substance whose temperature is measured
- B1 the zinc is a small mass of solid with a much smaller specific heat capacity than water, so the heat it absorbs is negligible
Suggest why the temperature continues to rise for about a minute after zinc powder is added to copper(II) sulfate solution.
Mark scheme
- B1 the reaction is not instantaneous; the zinc takes time to mix through the solution and react
- B1 heat is still being released during that time faster than it is lost, so the temperature keeps rising until the reaction is nearly complete
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