16.2· 46 questions · 424 marks · 509 min · 2005–2025· Structured questions
Every Cambridge A Level Physics Paper 4 question on the first law of thermodynamics, laid out as 59 A4 pages with the mark scheme below. Nothing is left out. Free to read, no account.
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59 / 59Answers below. Sit the paper first if you are practising.
Pastlit
Physics 9702 · The first law of thermodynamics — Paper 4
A Level · topical answer key — answer key (teacher use)
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8| Question | Answer | Marks | From |
|---|---|---|---|
| 1 | see sheet | 7 | 9702/41 Oct/Nov 2005 |
| 2 | see sheet | 4 | 9702/41 Oct/Nov 2008 |
| 3 | see sheet | 11 | 9702/42 Oct/Nov 2009 |
| 4 | see sheet | 9 | 9702/42 May/June 2011 |
| 5 | see sheet | 9 | 9702/43 May/June 2011 |
| 6 | see sheet | 9 | 9702/41 May/June 2013 |
| 7 | see sheet | 9 | 9702/43 May/June 2013 |
| 8 | see sheet | 8 | 9702/41 Oct/Nov 2013 |
| 9 | see sheet | 8 | 9702/42 Oct/Nov 2013 |
| 10 | see sheet | 6 | 9702/41 May/June 2014 |
| 11 | see sheet | 9 | 9702/42 May/June 2014 |
| 12 | see sheet | 6 | 9702/43 May/June 2014 |
| 13 | see sheet | 7 | 9702/43 Oct/Nov 2014 |
| 14 | see sheet | 8 | 9702/42 Oct/Nov 2015 |
| 15 | see sheet | 8 | 9702/42 Oct/Nov 2016 |
| 16 | see sheet | 9 | 9702/43 Oct/Nov 2016 |
| 17 | see sheet | 10 | 9702/42 Feb/March 2017 |
| 18 | see sheet | 8 | 9702/42 Oct/Nov 2017 |
| 19 | see sheet | 10 | 9702/42 Feb/March 2018 |
| 20 | see sheet | 9 | 9702/41 Oct/Nov 2018 |
| 21 | see sheet | 9 | 9702/43 Oct/Nov 2018 |
| 22 | see sheet | 10 | 9702/41 May/June 2019 |
| 23 | see sheet | 11 | 9702/42 May/June 2019 |
| 24 | see sheet | 10 | 9702/43 May/June 2019 |
| 25 | see sheet | 11 | 9702/42 Oct/Nov 2019 |
| 26 | see sheet | 6 | 9702/42 May/June 2020 |
| 27 | see sheet | 9 | 9702/41 Oct/Nov 2020 |
| 28 | see sheet | 10 | 9702/42 Oct/Nov 2020 |
| 29 | see sheet | 9 | 9702/43 Oct/Nov 2020 |
| 30 | see sheet | 10 | 9702/41 May/June 2021 |
| 31 | see sheet | 9 | 9702/42 May/June 2021 |
| 32 | see sheet | 10 | 9702/43 May/June 2021 |
| 33 | see sheet | 13 | 9702/41 Oct/Nov 2021 |
| 34 | see sheet | 13 | 9702/43 Oct/Nov 2021 |
| 35 | see sheet | 10 | 9702/42 Feb/March 2022 |
| 36 | see sheet | 12 | 9702/42 May/June 2022 |
| 37 | see sheet | 7 | 9702/42 Oct/Nov 2022 |
| 38 | see sheet | 9 | 9702/42 May/June 2023 |
| 39 | see sheet | 12 | 9702/41 Oct/Nov 2023 |
| 40 | see sheet | 8 | 9702/42 Oct/Nov 2023 |
| 41 | see sheet | 12 | 9702/43 Oct/Nov 2023 |
| 42 | see sheet | 11 | 9702/42 Oct/Nov 2024 |
| 43 | see sheet | 13 | 9702/42 May/June 2025 |
| 44 | see sheet | 8 | 9702/41 Oct/Nov 2025 |
| 45 | see sheet | 10 | 9702/42 Oct/Nov 2025 |
| 46 | see sheet | 8 | 9702/43 Oct/Nov 2025 |
3 (a) State the first law of thermodynamics in terms of the increase in internal energy ∆U, the heating q of the system and the work w done on the system. … … [1] (b) The volume occupied by 1.00 mol of liquid water at 100 °C is 1.87 ×10–5m3. When the water is vaporised at an atmospheric pressure of 1.03 ×105 Pa, the water vapour has a volume of 2.96 ×10–2m3. The latent heat required to vaporise 1.00 mol of water at 100 °C and 1.03 ×105 Pa is 4.05 ×104 J. Determine, for this change of state, (i) the work w done on the system, w = ……………………………. J [2] (ii) the heating q of the system, q = ……………………………. J [1] (iii) the increase in internal energy ∆U of the system. ∆U = ……………………………. J [1] Use (c) Using your answer to (b)(iii), estimate the binding energy per molecule in liquid water. energy = ………………………………. J [2]
7 marks
Mark scheme: 3 (a) correct statement, words or symbols …..…………………………...….. B1 [1] (b) (i) w = p∆V ………………………………………………………………….. C1 = 1.03 × 105 × (2.96 × 10–2 – 1.87 × 10–5) = (–) 3050 J …………………..……………….…………..…………… A1 [2] (ii) q = 4.05 × 104 J …………………………………………………………. B1 [1] (iii) ∆U = 4.05 × 104 – 3050 = 37500 J …no e.c.f. from (a)………………… A1 [1] penalise 2 sig.fig. once only (c) number of molecules = NA ………………………………………………. C1 energy = 37500 / (6.02 × 1023) = 6.2 × 10–20 J (accept 1 sig.fig.) …………………………..…. A1 [2]
4 (a) Write down an equation to represent the first law of thermodynamics in terms of the For heating q of a system, the work w done on the system and the increase ∆U in the Examiner’s internal energy. Use … [1] (b) The pressure of an ideal gas is decreased at constant temperature. Explain what change, if any, occurs in the internal energy of the gas. … … … … [3]
4 marks
Mark scheme: 4 (a) ∆U = q + w (allow correct word equation) B1 [1] (b) either kinetic energy constant because temperature constant M1 potential energy constant because no intermolecular forces M1 so no change in internal energy A1 [3] or kinetic energy and potential energy both constant (M1) so no change in internal energy (A1) reason for either constant k.e. or constant p.e. given (A1)
2 (a) State what is meant by the internal energy of a gas. For Examiner’s … Use … … [2] (b) The first law of thermodynamics may be represented by the equation U = q + w. State what is meant by each of the following symbols. + U … +q … +w … [3] (c) An amount of 0.18 mol of an ideal gas is held in an insulated cylinder fitted with a piston, as shown in Fig. 2.1. piston gas insulated cylinder Fig. 2.1 Atmospheric pressure is 1.0 × 105 Pa. The volume of the gas is suddenly increased from 1.8 × 103 cm3 to 2.1 × 103 cm3. For the expansion of the gas, (i) calculate the work done by the gas and hence show that the internal energy changes by 30 J, [3] (ii) determine the temperature change of the gas and state whether the change is an For increase or a decrease. Examiner’s Use change = … K … [3]
11 marks
Mark scheme: 2 (a) sum of kinetic and potential energies of molecules / particles / atoms … M1 random (distribution) … A1 [2] (b) +∆U: increase in internal energy … B1 +q: heating of / heat supplied to system … B1 +w: work done on system … B1 [3] (c) (i) work done = p∆V … C1 = 1.0 × 105 × (2.1 – 1.8) × 10-3 = 30 J … M1 w = 30 J, q = 0 so ∆U = 30 J … A1 [3] (ii) these three marks were removed, as insufficient data was given in the question. [Total: 8] GCE A/AS LEVEL – October/November 2009 9702 42
4 (a) The first law of thermodynamics may be expressed in the form For Examiner’s ΔU = q + w. Use Explain the symbols in this expression. + ΔU … + q … + w … [3] (b) (i) State what is meant by specific latent heat. … … … … [3] (ii) Use the first law of thermodynamics to explain why the specific latent heat of vaporisation is greater than the specific latent heat of fusion for a particular substance. … … … … [3]
9 marks
Mark scheme: 4 (a) +∆U: increase in internal energy B1 +q: thermal energy / heat supplied to the system B1 +w: work done on the system B1 [3] (b) (i) (thermal) energy required to change the state of a substance M1 per unit mass A1 without any change of temperature A1 [3] (ii) when evaporating greater change in separation of atoms/molecules M1 greater change in volume M1 identifies each difference correctly with ∆U and w A1 [3]
4 (a) The first law of thermodynamics may be expressed in the form For Examiner’s ΔU = q + w. Use Explain the symbols in this expression. + ΔU … + q … + w … [3] (b) (i) State what is meant by specific latent heat. … … … … [3] (ii) Use the first law of thermodynamics to explain why the specific latent heat of vaporisation is greater than the specific latent heat of fusion for a particular substance. … … … … [3]
9 marks
Mark scheme: 4 (a) +∆U: increase in internal energy B1 +q: thermal energy / heat supplied to the system B1 +w: work done on the system B1 [3] (b) (i) (thermal) energy required to change the state of a substance M1 per unit mass A1 without any change of temperature A1 [3] (ii) when evaporating greater change in separation of atoms/molecules M1 greater change in volume M1 identifies each difference correctly with ∆U and w A1 [3]
2 (a) State what is meant by an ideal gas. For Examiner’s … Use … … … [3] (b) Two cylinders A and B are connected by a tube of negligible volume, as shown in Fig. 2.1. cylinder A cylinder B tap T 2.5 × 103 cm3 3.4 × 105 Pa 1.6 × 103 cm3 300 K 4.9 × 105 Pa tube Fig. 2.1 Initially, tap T is closed. The cylinders contain an ideal gas at different pressures. (i) Cylinder A has a constant volume of 2.5 × 103 cm3 and contains gas at pressure 3.4 × 105 Pa and temperature 300 K. Show that cylinder A contains 0.34 mol of gas. [1] (ii) Cylinder B has a constant volume of 1.6 × 103 cm3 and contains 0.20 mol of gas. For When tap T is opened, the pressure of the gas in both cylinders is 3.9 × 105 Pa. Examiner’s No thermal energy enters or leaves the gas. Use Determine the final temperature of the gas. temperature = … K [2] (c) By reference to work done and change in internal energy, suggest why the temperature of the gas in cylinder A has changed. … … … … [3]
9 marks
Mark scheme: 2 (a) obeys the equation pV = constant × T or pV = nRT M1 p, V and T explained A1 at all values of p, V and T/fixed mass/n is constant A1 [3] (b) (i) 3.4 × 105 × 2.5 × 103 × 10–6 = n × 8.31 × 300 M1 n = 0.34 mol A0 [1] (ii) for total mass/amount of gas 3.9 × 105 × (2.5 + 1.6) × 103 × 10–6 = (0.34 + 0.20) × 8.31 × T C1 T = 360 K A1 [2] (c) when tap opened gas passed (from cylinder B) to cylinder A B1 work done on gas in cylinder A (and no heating) M1 so internal energy and hence temperature increase A1 [3] GCE AS/A LEVEL – May/June 2013 9702 41
2 (a) State what is meant by an ideal gas. For Examiner’s … Use … … … [3] (b) Two cylinders A and B are connected by a tube of negligible volume, as shown in Fig. 2.1. cylinder A cylinder B tap T 2.5 × 103 cm3 3.4 × 105 Pa 1.6 × 103 cm3 300 K 4.9 × 105 Pa tube Fig. 2.1 Initially, tap T is closed. The cylinders contain an ideal gas at different pressures. (i) Cylinder A has a constant volume of 2.5 × 103 cm3 and contains gas at pressure 3.4 × 105 Pa and temperature 300 K. Show that cylinder A contains 0.34 mol of gas. [1] (ii) Cylinder B has a constant volume of 1.6 × 103 cm3 and contains 0.20 mol of gas. For When tap T is opened, the pressure of the gas in both cylinders is 3.9 × 105 Pa. Examiner’s No thermal energy enters or leaves the gas. Use Determine the final temperature of the gas. temperature = … K [2] (c) By reference to work done and change in internal energy, suggest why the temperature of the gas in cylinder A has changed. … … … … [3]
9 marks
Mark scheme: 2 (a) obeys the equation pV = constant × T or pV = nRT M1 p, V and T explained A1 at all values of p, V and T/fixed mass/n is constant A1 [3] (b) (i) 3.4 × 105 × 2.5 × 103 × 10–6 = n × 8.31 × 300 M1 n = 0.34 mol A0 [1] (ii) for total mass/amount of gas 3.9 × 105 × (2.5 + 1.6) × 103 × 10–6 = (0.34 + 0.20) × 8.31 × T C1 T = 360 K A1 [2] (c) when tap opened gas passed (from cylinder B) to cylinder A B1 work done on gas in cylinder A (and no heating) M1 so internal energy and hence temperature increase A1 [3] GCE AS/A LEVEL – May/June 2013 9702 43
2 The product of the pressure p and the volume V of an ideal gas is given by the expression For 1 Examiner’s Use pV = 3Nm<c 2> where m is the mass of one molecule of the gas. (a) State the meaning of the symbol (i) N, … [1] (ii) <c 2>. … [1] (b) The product pV is also given by the expression pV = NkT. Deduce an expression, in terms of the Boltzmann constant k and the thermodynamic temperature T, for the mean kinetic energy of a molecule of the ideal gas. [2] (c) A cylinder contains 1.0 mol of an ideal gas. (i) The volume of the cylinder is constant. Calculate the energy required to raise the temperature of the gas by 1.0 kelvin. energy = … J [2] (ii) The volume of the cylinder is now allowed to increase so that the gas remains at constant pressure when it is heated. Explain whether the energy required to raise the temperature of the gas by 1.0 kelvin is now different from your answer in (i). … … … [2]
8 marks
Mark scheme: 2 (a) (i) N: (total) number of molecules B1 [1] (ii) <c2>: mean square speed/velocity B1 [1] (b) pV = ⅓Nm<c2> = NkT (mean) kinetic energy = ½ m<c2> C1 algebra clear leading to ½ m<c2> = (3/2)kT A1 [2] (c) (i) either energy required = (3/2) × 1.38 × 10–23 × 1.0 × 6.02 × 1023 C1 either energy required = 12.5 J (12J if 2 s.f.) A1 [2] or energy = (3/2) × 8.31 × 1.0 (C1) or energy = 12.5 J (A1) (ii) energy is needed to push back atmosphere/do work against atmosphere M1 so total energy required is greater A1 [2]
2 The product of the pressure p and the volume V of an ideal gas is given by the expression For 1 Examiner’s Use pV = 3Nm<c 2> where m is the mass of one molecule of the gas. (a) State the meaning of the symbol (i) N, … [1] (ii) <c 2>. … [1] (b) The product pV is also given by the expression pV = NkT. Deduce an expression, in terms of the Boltzmann constant k and the thermodynamic temperature T, for the mean kinetic energy of a molecule of the ideal gas. [2] (c) A cylinder contains 1.0 mol of an ideal gas. (i) The volume of the cylinder is constant. Calculate the energy required to raise the temperature of the gas by 1.0 kelvin. energy = … J [2] (ii) The volume of the cylinder is now allowed to increase so that the gas remains at constant pressure when it is heated. Explain whether the energy required to raise the temperature of the gas by 1.0 kelvin is now different from your answer in (i). … … … [2]
8 marks
Mark scheme: 2 (a) (i) N: (total) number of molecules B1 [1] (ii) <c2>: mean square speed/velocity B1 [1] (b) pV = ⅓Nm<c2> = NkT (mean) kinetic energy = ½ m<c2> C1 algebra clear leading to ½ m<c2> = (3/2)kT A1 [2] (c) (i) either energy required = (3/2) × 1.38 × 10–23 × 1.0 × 6.02 × 1023 C1 either energy required = 12.5 J (12J if 2 s.f.) A1 [2] or energy = (3/2) × 8.31 × 1.0 (C1) or energy = 12.5 J (A1) (ii) energy is needed to push back atmosphere/do work against atmosphere M1 so total energy required is greater A1 [2]
3 The volume of 1.00 kg of water in the liquid state at 100 °C is 1.00 × 10−3 m3. The volume of 1.00 kg of water vapour at 100 °C and atmospheric pressure 1.01 × 105 Pa is 1.69 m3. (a) Show that the work done against the atmosphere when 1.00 kg of liquid water becomes water vapour is 1.71 × 105 J. [2] (b) (i) The first law of thermodynamics may be given by the expression ΔU = + q + w where ΔU is the increase in internal energy of the system. State what is meant by 1. + q, … [1] 2. + w. … [1] (ii) The specific latent heat of vaporisation of water at 100 °C is 2.26 × 106 J kg−1. A mass of 1.00 kg of liquid water becomes water vapour at 100 °C. Determine, using your answer in (a), the increase in internal energy of this mass of water during vaporisation. increase in internal energy = … J [2]
6 marks
Mark scheme: 3 (a) either change in volume = (1.69 – 1.00 × 10–3) or liquid volume << volume of vapour M1 work done = 1.01 × 105 × 1.69 = 1.71 × 105 (J) A1 [2] (b) (i) 1. heating of system/thermal energy supplied to the system B1 [1] 2. work done on the system B1 [1] (ii) ∆U = (2.26 × 106) – (1.71 × 105) C1 = 2.09 × 106 J (3 s.f. needed) A1 [2]
2 A constant mass of an ideal gas has a volume of 3.49 × 103 cm3 at a temperature of 21.0 °C. When the gas is heated, 565 J of thermal energy causes it to expand to a volume of 3.87 × 103 cm3 at 53.0 °C. This is illustrated in Fig. 2.1. 3.49 × 103 cm3 3.87 × 103 cm3 565 J 21.0 °C 53.0 °C Fig. 2.1 (a) Show that the initial and final pressures of the gas are equal. [2] (b) The pressure of the gas is 4.20 × 105 Pa. For this heating of the gas, (i) calculate the work done by the gas, work done = … J [2] (ii) use the first law of thermodynamics and your answer in (i) to determine the change in internal energy of the gas. change in internal energy = … J [2] (c) Explain why the change in kinetic energy of the molecules of this ideal gas is equal to the change in internal energy. … … … … [3]
9 marks
Mark scheme: 2 (a) use of kelvin temperatures B1 both values of (V / T) correct (11.87), V / T is constant so pressure is constant M1 [2] (allow use of n R1. Do not allow other values of n.) (b) (i) work done R p∆V R 4.2 × 105 × (3.87 – 3.49) × 103 × 10–6 C1 = = = = = R 160 J A1 [2] (do not allow use of V instead of ∆V) (ii) increase / change in internal energy R heating of system N work done on system C1 R 565 – 160 = = = = R 405 J A1 [2] (c) internal energy R sum of kinetic energy and potential energy / EK N EP B1 no intermolecular forces M1 no potential energy (so ∆U R ∆EK) A1 [3]
3 The volume of 1.00 kg of water in the liquid state at 100 °C is 1.00 × 10−3 m3. The volume of 1.00 kg of water vapour at 100 °C and atmospheric pressure 1.01 × 105 Pa is 1.69 m3. (a) Show that the work done against the atmosphere when 1.00 kg of liquid water becomes water vapour is 1.71 × 105 J. [2] (b) (i) The first law of thermodynamics may be given by the expression ΔU = + q + w where ΔU is the increase in internal energy of the system. State what is meant by 1. + q, … [1] 2. + w. … [1] (ii) The specific latent heat of vaporisation of water at 100 °C is 2.26 × 106 J kg−1. A mass of 1.00 kg of liquid water becomes water vapour at 100 °C. Determine, using your answer in (a), the increase in internal energy of this mass of water during vaporisation. increase in internal energy = … J [2]
6 marks
Mark scheme: 3 (a) either change in volume = (1.69 – 1.00 × 10–3) or liquid volume << volume of vapour M1 work done = 1.01 × 105 × 1.69 = 1.71 × 105 (J) A1 [2] (b) (i) 1. heating of system/thermal energy supplied to the system B1 [1] 2. work done on the system B1 [1] (ii) ∆U = (2.26 × 106) – (1.71 × 105) C1 = 2.09 × 106 J (3 s.f. needed) A1 [2]
3 A fixed mass of gas has an initial volume of 5.00 × 10−4 m3 at a pressure of 2.40 × 105 Pa and a temperature of 288 K. It is heated at constant pressure so that, in its final state, the volume is 14.5 × 10−4 m3 at a temperature of 835 K, as illustrated in Fig. 3.1. initial state final state 5.00 × 10–4 m3 14.5 × 10–4 m3 2.40 × 105 Pa 2.40 × 105 Pa 288 K 835 K Fig. 3.1 (a) Show that these two states provide evidence that the gas behaves as an ideal gas. [3] (b) The total thermal energy supplied to the gas for this change is 569 J. Determine (i) the external work done, work done = … J [2] (ii) the change in internal energy of the gas. State whether the change is an increase or a decrease in internal energy. change in internal energy = … J … [2]
7 marks
Mark scheme: 3 (a) initially, pV / T = (2.40 × 105 × 5.00 × 10–4) / 288 = 0.417 M1 finally, pV / T = (2.40 × 105 × 14.5 × 10–4) / 835 = 0.417 M1 ideal gas because pV / T is constant A1 [3] (allow 2 marks for two determinations of V / T and then 1 mark for V / T and p constant, so ideal) (b) (i) work done = p∆V = 2.40 × 105 × (14.5 – 5.00) × 10–4 C1 = 228 J (ignore sign, not 2 s.f.) A1 [2] (ii) ∆U = q + w = 569 – 228 = 341 J M1 increase A1 [2]
3 (a) State an expression, in terms of work done and heating, that is used to calculate the increase in internal energy of a system. … … … [2] (b) State and explain, in terms of your expression in (a), the change, if any, in the internal energy (i) of the water in an ice cube when the ice melts, at atmospheric pressure, to form a liquid without any change of temperature, … … … … [3] (ii) of the gas in a tyre when the tyre bursts so that the gas suddenly increases in volume. Assume that the gas is ideal. … … … … [3]
8 marks
Mark scheme: 3 (a) heat/thermal energy gained by system or energy transferred to system by heating B1 plus work done on the system or minus work done by the system B1 [2] (b) (i) either volume decreases so work done on the system or small volume change so work done on system negligible M1 (thermal) energy absorbed to break lattice structure M1 internal energy increases A1 [3] (ii) gas expands so work done by gas (against atmosphere) M1 no time for thermal energy to enter or leave the gas M1 internal energy decreases A1 [3]
3 (a) State what is meant by the internal energy of a system. … … … [2] (b) Explain, by reference to work done and heating, whether the internal energy of the following increases, decreases or remains constant: (i) the gas in a toy balloon when the balloon bursts suddenly, … … … … [3] (ii) ice melting at constant temperature and at atmospheric pressure to form water that is more dense than the ice. … … … … [3] [Total: 8]
8 marks
Mark scheme: 3 (a) (sum of/total) potential energy and kinetic energy of (all) molecules/particles M1 reference to random (distribution) A1 [2] (b) (i) no heat enters (gas)/leaves (gas)/no heating (of gas) B1 work done by gas (against atmosphere as it expands) M1 internal energy decreases A1 [3] (ii) volume decreases so work done on ice/water B1 (allow work done negligible because ∆V small) heating of ice (to break rigid forces/bonds) M1 internal energy increases A1 [3]
2 An ideal gas initially has pressure 1.0 × 105 Pa, volume 4.0 × 10−4 m3 and temperature 300 K, as illustrated in Fig. 2.1. initial state final state 1.0 × 105 Pa 5.0 × 105 Pa 4.0 × 10–4 m3 4.0 × 10–4 m3 300 K T Fig. 2.1 A change in energy of the gas of 240 J results in an increase of pressure to a final value of 5.0 × 105 Pa at constant volume. The thermodynamic temperature becomes T. (a) Calculate (i) the temperature T, T = … K [2] (ii) the amount of gas. amount = … mol [2] (b) The increase in internal energy ΔU of a system may be represented by the expression ΔU = q + w. (i) State what is meant by the symbol 1. +q, … 2. +w. … [2] (ii) State, for the gas in (a), the value of 1. ΔU, ΔU = … J 2. +q, +q = … J 3. +w. +w = … J [3] [Total: 9]
9 marks
Mark scheme: 2 (a) (i) p ∝ T or pV / T = constant or pV = nRT C1 T (= 5 × 300 =) 1500 K A1 [2] (ii) pV = nRT 1.0 × 105 × 4.0 × 10–4 = n × 8.31 × 300 or 5.0 × 105 × 4.0 × 10–4 = n × 8.31 × 1500 C1 n = 0.016 mol A1 [2] (b) (i) 1. heating/thermal energy supplied B1 2. work done on/to system B1 [2] (ii) 1. 240 J A1 2. same value as given in 1. (= 240 J) and zero given for 3. A1 3. zero A1 [3] 2
2 (a) The first law of thermodynamics can be represented by the expression ΔU = q + w. State what is meant by the symbols in the expression. +DU … +q … +w … [2] (b) A fixed mass of an ideal gas undergoes a cycle ABCA of changes, as shown in Fig. 2.1. 6.0 pressure / 105 Pa A B 5.0 4.0 3.0 2.0 1.0 C 0 0 2.0 4.0 6.0 volume / 10–4 m3 Fig. 2.1 (i) During the change from A to B, the energy supplied to the gas by heating is 442 J. Use the first law of thermodynamics to show that the internal energy of the gas increases by 265 J. [2] (ii) During the change from B to C, the internal energy of the gas decreases by 313 J. By considering molecular energy, state and explain qualitatively the change, if any, in the temperature of the gas. … … … … … [3] (iii) For the change from C to A, use the data in (b)(i) and (b)(ii) to calculate the change in internal energy. change in internal energy = … J [1] (iv) The temperature of the gas at point A is 227 °C. Calculate the number of molecules in the fixed mass of the gas. number = … [2] [Total: 10]
10 marks
Mark scheme: 2(a) +q heat (energy) transferred to the system / heating of system +w work done on system B2 2(b)(i) W = p∆V = 5.2 × 105 × (5.0 – 1.6) × 10–4 (=177 J) B1 ∆U = q + w = 442 – 177 = 265 J A1 2(b)(ii) no (molecular) potential energy B1 internal energy decreases so (total molecular) kinetic energy decreases B1 (mean molecular) kinetic energy decreases so temperature decreases B1 Question Answer Marks 2(b)(iii) ∆U + 265 – 313 = 0 ∆U = 48 J A1 2(b)(iv) pV = NkT or pV = nRT and N = nNA C1 5.2 × 105 × 1.6 × 10–4 = N × 1.38 × 10–23 × (273 + 227) or 5.2 × 105 × 1.6 × 10–4 = n × 8.31 × (273 + 227) and n = N / 6.02 × 1023 N = 1.2 × 1022 A1
2 (a) State what is meant by specific latent heat. … … … [2] (b) A beaker of boiling water is placed on the pan of a balance, as illustrated in Fig. 2.1. A V d.c. supply heater balance pan boiling water Fig. 2.1 The water is maintained at its boiling point by means of a heater. The change M in the balance reading in 300 s is determined for two different input powers to the heater. The results are shown in Fig. 2.2. voltmeter reading ammeter reading M / g / V / A 11.5 5.2 5.0 14.2 6.4 9.1 Fig. 2.2 (i) Energy is supplied continuously by the heater. State where, in this experiment, 1. external work is done, … … 2. internal energy increases. Explain your answer. … … … [3] (ii) Use data in Fig. 2.2 to determine the specific latent heat of vaporisation of water. specific latent heat = … J g–1 [3] [Total: 8]
8 marks
Mark scheme: 2(a) (thermal) energy per (unit) mass (to cause change of state) B1 (energy required to cause/released in) change of state at constant temperature B1 2(b)(i) 1. (work done on/against) the atmosphere B1 2. water as it turns from liquid to vapour M1 as potential energy of molecules increases A1 or surroundings as its temperature rises (M1) as energy is lost/transferred to surroundings (A1) 2(b)(ii) VI – h = M / t × L (where h = power loss) or L = (VIt – Q) / M (where Q = energy loss) C1 (14.2 × 6.4) – (11.5 × 5.2) = (9.1 – 5.0) × L / 300 or L = [(14.2 × 6.4) – (11.5 × 5.2)] × 300 / (9.1 – 5.0) C1 L = 2300 J g–1 A1
2 A cylinder contains 5.12 mol of an ideal gas at pressure of 5.60 × 105 Pa and volume 3.80 × 104 cm3. (a) Determine the temperature of the gas. temperature = … K [2] (b) The average kinetic energy EK of a molecule of the gas is given by the expression 3 EK = kT 2 where k is the Boltzmann constant and T is the thermodynamic temperature. The gas is heated at constant pressure so that its temperature rises by 125 K. (i) Use your answer in (a) to determine the new volume of the gas. volume = … cm3 [2] (ii) Calculate the increase in internal energy of the gas. Explain your working. increase in internal energy = … J [3] (c) (i) Use your answer in (b)(i) to determine the external work done during the expansion of the gas. work done = … J [2] (ii) Calculate the total thermal energy required to heat the gas in (b). energy = … J [1] [Total: 10]
10 marks
Mark scheme: 2(a) pV = nRT T = (5.60 × 105 × 3.80 × 10–2) / (5.12 × 8.31) C1 T = 500 K A1 2(b)(i) V / T is constant V = (3.80 × 104) × (500 + 125) / 500 C1 V = 4.75 × 104 cm3 A1 2(b)(ii) (for ideal gas,) change in internal energy is change in (total) kinetic energy (of molecules) B1 ∆U = 3 / 2 × 1.38 × 10–23 × 125 × 5.12 × 6.02 × 1023 C1 = 7980 J A1 2(c)(i) w = p∆V = 5.60 × 105 × (4.75 – 3.80) × 10–2 C1 = 5320 J A1 2(c)(ii) total = 7980 + 5320 = 13300 J A1
2 (a) State what is meant by the internal energy of a system. … … … … [2] (b) An ideal gas undergoes a cycle of changes as shown in Fig. 2.1. 3.00 2.80 Q 372 K pressure / 105 Pa 2.60 97.0 J 2.40 2.20 280 K P R 332 K 2.00 900 950 1000 1050 1100 1150 volume / cm3 Fig. 2.1 At point P, the gas has volume 950 cm3, pressure 2.10 × 105 Pa and temperature 280 K. The gas is heated at constant volume and 97.0 J of thermal energy is transferred to the gas. Its pressure and temperature change so that the gas is at point Q on Fig. 2.1. The gas then undergoes the change from point Q to point R and then from point R back to point P, as shown on Fig. 2.1. Some energy changes that take place during the cycle PQRP are shown in Fig. 2.2. change P → Q change Q → R change R → P thermal energy transferred to gas / J +97.0 0 … work done on gas / J … –42.5 +37.0 increase in internal energy of gas / J … … … Fig. 2.2 (i) State the total change in internal energy of the gas during the complete cycle PQRP. Explain your answer. … … … [2] (ii) On Fig. 2.2, complete the energy changes for the gas during 1. the change P → Q, 2. the change Q → R, 3. the change R → P. [5] [Total: 9]
9 marks
Mark scheme: 2(a) sum of potential and kinetic energies (of molecules/atoms/particles) B1 (energy of) molecules/atoms/particles in random motion B1 2(b)(i) final temperature = initial temperature B1 no change in internal energy B1 2(b)(ii) 1. work done on gas (P→Q): 0 A1 increase in internal energy (P→Q): (+)97.0 J A1 2. increase in internal energy (Q→R): –42.5 J A1 3. increase in internal energy (R→P): –54.5 J A1 thermal energy supplied (R→P): –91.5 J A1
2 (a) State what is meant by the internal energy of a system. … … … … [2] (b) An ideal gas undergoes a cycle of changes as shown in Fig. 2.1. 3.00 2.80 Q 372 K pressure / 105 Pa 2.60 97.0 J 2.40 2.20 280 K P R 332 K 2.00 900 950 1000 1050 1100 1150 volume / cm3 Fig. 2.1 At point P, the gas has volume 950 cm3, pressure 2.10 × 105 Pa and temperature 280 K. The gas is heated at constant volume and 97.0 J of thermal energy is transferred to the gas. Its pressure and temperature change so that the gas is at point Q on Fig. 2.1. The gas then undergoes the change from point Q to point R and then from point R back to point P, as shown on Fig. 2.1. Some energy changes that take place during the cycle PQRP are shown in Fig. 2.2. change P → Q change Q → R change R → P thermal energy transferred to gas / J +97.0 0 … work done on gas / J … –42.5 +37.0 increase in internal energy of gas / J … … … Fig. 2.2 (i) State the total change in internal energy of the gas during the complete cycle PQRP. Explain your answer. … … … [2] (ii) On Fig. 2.2, complete the energy changes for the gas during 1. the change P → Q, 2. the change Q → R, 3. the change R → P. [5] [Total: 9]
9 marks
Mark scheme: 2(a) sum of potential and kinetic energies (of molecules/atoms/particles) B1 (energy of) molecules/atoms/particles in random motion B1 2(b)(i) final temperature = initial temperature B1 no change in internal energy B1 2(b)(ii) 1. work done on gas (P→Q): 0 A1 increase in internal energy (P→Q): (+)97.0 J A1 2. increase in internal energy (Q→R): –42.5 J A1 3. increase in internal energy (R→P): –54.5 J A1 thermal energy supplied (R→P): –91.5 J A1
2 A fixed mass of an ideal gas has volume 210 cm3 at pressure 3.0 × 105 Pa and temperature 270 K. The volume of the gas is reduced at constant pressure to 140 cm3, as shown in Fig. 2.1. 210 cm3 140 cm3 3.0 × 105 Pa 3.0 × 105 Pa 270 K T Fig. 2.1 The final temperature of the gas is T. (a) Determine: (i) the amount of gas amount = … mol [3] (ii) the final temperature T of the gas T = … K [2] (iii) the external work done on the gas. work done = … J [2] (b) For this change in volume and temperature of the gas, the thermal energy transferred is 53 J. Determine ΔU, the change in internal energy of the gas. ΔU = … J [3] [Total: 10]
10 marks
Mark scheme: 2(a)(i) pV = nRT C1 n = (3.0 × 105 × 210 × 10–6) / (8.31 × 270) C1 = 0.028 mol A1 2(a)(ii) V ∝ T or T = pV / nR with value of n from (i) C1 T = (140 / 210) × 270 or T = (3.0 × 105 × 140 ×10–6) / (8.31 × 0.028) = 180 K A1 2(a)(iii) W = p∆V = 3.0 × 105 × (210 – 140) × 10–6 C1 = 21 J A1 Question Answer Marks 2(b) ∆U = w + q C1 = 21 – 53 C1 or ∆U = (nNA) × (3 / 2)k∆T (C1) = (0.0281 × 6.02 × 1023) × (3 / 2) × 1.38 × 10–23 × (180 – 270) (C1) or ∆U = (3 / 2)nR∆T (C1) = (3 / 2) × 0.0281 × 8.31 × (180 – 270) (C1) ∆U = (–)32 J A1
2 (a) The first law of thermodynamics may be expressed in the form ΔU = q + w. (i) State, for a system, what is meant by: 1. +q … … 2. +w. … … [2] (ii) State what is represented by a negative value of ΔU. … … [1] (b) An ideal gas, sealed in a container, undergoes the cycle of changes shown in Fig. 2.1. 7.0 8.7 × 10–4 m3 B 6.6 × 105 Pa 450 K 6.0 pressure / 105 Pa 5.0 4.0 2.4 × 10–3 m3 3.0 1.6 × 105 Pa 8.7 × 10–4 m3 300 K 1.6 × 105 Pa 110 K 2.0 C A 1.0 0.75 1.00 1.25 1.50 1.75 2.00 2.25 2.50 volume / 10–3 m3 Fig. 2.1 At point A, the gas has volume 2.4 × 10–3 m3, pressure 1.6 × 105 Pa and temperature 300 K. The gas is compressed suddenly so that no thermal energy enters or leaves the gas during the compression. The amount of work done is 480 J so that, at point B, the gas has volume 8.7 × 10–4 m3, pressure 6.6 × 105 Pa and temperature 450 K. The gas is now cooled at constant volume so that, between points B and C, 1100 J of thermal energy is transferred. At point C, the gas has pressure 1.6 × 105 Pa and temperature 110 K. Finally, the gas is returned to point A. (i) State and explain the total change in internal energy of the gas for one complete cycle ABCA. … … … [2] (ii) Calculate the external work done on the gas during the expansion from point C to point A. work done = … J [2] (iii) Complete Fig. 2.2 for the changes from: 1. point A to point B 2. point B to point C 3. point C to point A. change +q / J +w / J ΔU / J A B … … … B C … … … C A … … … Fig. 2.2 [4] [Total: 11]
11 marks
Mark scheme: 2(a)(i) 1. energy transfer to the system by heating B1 2. (external) work done on the system B1 2(a)(ii) decrease in internal energy B1 2(b)(i) no change (in internal energy) B1 (because) no change in temperature B1 2(b)(ii) work done = p∆V = (–)1.6 × 105 × (2.4 – 0.87) × 10–3 C1 = (–)240 J A1 2(b)(iii) first row all correct (0, 480, 480) A1 second row all correct (–1100, 0, –1100) A1 final column of third row calculated correctly from the two values above it, so that the final column adds up to 0 A1 second column in final row correct, with correct negative sign and first column in final row calculated correctly so that it adds to the second column to give the third column (fully correct table is: 0 480 480 –1100 0 –1100 860 –240 620 ) A1
2 A fixed mass of an ideal gas has volume 210 cm3 at pressure 3.0 × 105 Pa and temperature 270 K. The volume of the gas is reduced at constant pressure to 140 cm3, as shown in Fig. 2.1. 210 cm3 140 cm3 3.0 × 105 Pa 3.0 × 105 Pa 270 K T Fig. 2.1 The final temperature of the gas is T. (a) Determine: (i) the amount of gas amount = … mol [3] (ii) the final temperature T of the gas T = … K [2] (iii) the external work done on the gas. work done = … J [2] (b) For this change in volume and temperature of the gas, the thermal energy transferred is 53 J. Determine ΔU, the change in internal energy of the gas. ΔU = … J [3] [Total: 10]
10 marks
Mark scheme: 2(a)(i) pV = nRT C1 n = (3.0 × 105 × 210 × 10–6) / (8.31 × 270) C1 = 0.028 mol A1 2(a)(ii) V ∝ T or T = pV / nR with value of n from (i) C1 T = (140 / 210) × 270 or T = (3.0 × 105 × 140 ×10–6) / (8.31 × 0.028) = 180 K A1 2(a)(iii) W = p∆V = 3.0 × 105 × (210 – 140) × 10–6 C1 = 21 J A1 Question Answer Marks 2(b) ∆U = w + q C1 = 21 – 53 C1 or ∆U = (nNA) × (3 / 2)k∆T (C1) = (0.0281 × 6.02 × 1023) × (3 / 2) × 1.38 × 10–23 × (180 – 270) (C1) or ∆U = (3 / 2)nR∆T (C1) = (3 / 2) × 0.0281 × 8.31 × (180 – 270) (C1) ∆U = (–)32 J A1
2 (a) Smoke particles are suspended in still air. Brownian motion of the smoke particles is seen through a microscope. Describe: (i) what is seen through the microscope … … [1] (ii) how Brownian motion provides evidence for the nature of the movement of gas molecules. … … … [2] (b) A fixed mass of an ideal gas has volume 2.40 × 103 cm3 at pressure 3.51 × 105 Pa and temperature 290 K. The gas is heated at constant volume until the temperature is 310 K at pressure 3.75 × 105 Pa, as illustrated in Fig. 2.1. 2.40 × 103 cm3 2.40 × 103 cm3 3.51 × 105 Pa 3.75 × 105 Pa 290 K 310 K Fig. 2.1 The quantity of thermal energy required to raise the temperature of 1.00 mol of the gas by 1.00 K at constant volume is 12.5 J. Calculate, to three significant figures: (i) the amount, in mol, of the gas amount = … mol [3] (ii) the thermal energy transfer during the change. energy transfer = … J [2] (c) For the change in the gas in (b), state: (i) the quantity of external work done on the gas work done = … J [1] (ii) the change in internal energy, with the direction of this change. change = … J direction … [2] [Total: 11]
11 marks
Mark scheme: 2(a)(i) specks of light moving haphazardly B1 2(a)(ii) (gas) molecules collide with (smoke) particles or random motion of the (gas) molecules M1 causes the (haphazard) motion of the smoke particles or causes the smoke particles to change direction A1 2(b)(i) pV = nRT C1 n = (3.51 × 105 × 2.40 × 10–3) / (8.31 × 290) or n = (3.75 × 105 × 2.40 × 10–3) / (8.31 × 310) C1 or pV = NkT (C1) n = (3.51 × 105 × 2.40 × 10–3) / (1.38 × 10–23 × 6.02 × 1023 × 290) or n = (3.75 × 105 × 2.40 × 10–3) / (1.38 × 10–23 × 6.02 × 1023 × 310) (C1) n = 0.350 mol or 0.349 mol A1 2(b)(ii) energy transfer = (0.349 or 0.35) × 12.5 × (310 – 290) C1 = 87.3 J or 87.5 J A1 2(c)(i) zero A1 2(c)(ii) 87.3 J or 87.5 J A1 increase B1
3 By reference to the first law of thermodynamics, state and explain the change, if any, in the internal energy of: (a) a lump of solid lead as it melts at constant temperature … … … … … [3] (b) some gas in a toy balloon when the balloon bursts and no thermal energy enters or leaves the gas. … … … … … [3] [Total: 6]
6 marks
Mark scheme: 3(a) (little/no volume change so) little/no external work done B1 thermal energy supplied to provide latent heat M1 internal energy increases A1 3(b) (rapid) increase in volume B1 gas does work against the atmosphere M1 internal energy decreases A1
2 (a) The first law of thermodynamics may be expressed as ΔU = (+q) + (+w) where ΔU is the increase in internal energy of the system. State the meaning of: +q … … +w. … … [2] (b) The variation with pressure p of the volume V of a fixed mass of an ideal gas is shown in Fig. 2.1. 4.0 BV / 10–3 m3 3.6 3.2 2.8 2.4 C A 2.0 2.2 2.6 3.0 3.4 3.8 4.2 4.6 5.0 5.4 p / 105 Pa Fig. 2.1 The gas undergoes a cycle of changes A to B to C to A. During the change A to B, the volume of the gas increases from 2.3 × 10–3 m3 to 3.8 × 10–3 m3. (i) Show that the magnitude of the work done during the change A to B is 390 J. [1] (ii) State and explain the total change, if any, in the internal energy of the gas during one complete cycle. … … … [2] (c) During the change A to B, 1370 J of thermal energy is transferred to the gas. During the change B to C, no thermal energy enters or leaves the gas. The work done on the gas during this change is 550 J. Use these data and the information in (b) to complete Table 2.1. Table 2.1 change q / J w / J ΔU / J A to B … … … B to C … … … C to A … … … [4] [Total: 9]
9 marks
Mark scheme: 2(a) +q: thermal energy transfer to system B1 +w: work done on system B1 2(b)(i) (W =) 2.6 ×105 × (3.8 – 2.3) × 10–3 = 390 J A1 2(b)(ii) no (total) change (in internal energy) B1 gas returns to its original temperature B1 2(c) A to B row all correct (1370, – 390, 980) B1 B to C row all correct (0, 550, 550) B1 C to A row: ΔU adds to the other two ΔU values to give zero B1 C to A row: w = 0 and q adds to w to give ΔU value complete correct answer: change q / J w / J ΔU / J A to B B to C C to A (+)1370 0 –1530 –390 (+)550 0 (+)980 (+)550 –1530 B1
2 (a) State what is meant by the internal energy of a system. … … … [2] (b) The atoms of an ideal gas occupy a container of volume 2.30 × 10–3 m3 at pressure 2.60 × 105 Pa and temperature 180 K, as illustrated in Fig. 2.1. 2.30 × 10–3 m3 3.80 × 10–3 m3 2.60 × 105 Pa 2.60 × 105 Pa 180 K T 980 J Fig. 2.1 The gas is heated at constant pressure so that its volume becomes 3.80 × 10–3 m3 at a temperature T. For the fixed mass of gas, calculate: (i) the amount of substance, in mol amount = … mol [2] (ii) the temperature T, in K. T = … K [2] (c) During the change in (b), the thermal energy supplied to the gas is 980 J. (i) Determine the work done on the gas during this change. Explain your working. work done = … J [3] (ii) Determine the change ΔU in internal energy of the gas. ΔU = … J [1] [Total: 10]
10 marks
Mark scheme: 2(a) sum of potential energy and kinetic energy (of particles) B1 (total) energy of random motion of particles B1 2(b)(i) pV = nRT C1 2.60 × 105 × 2.30 × 10–3 = n × 8.31 × 180 n = 0.400 mol A1 2(b)(ii) (2.30 × 10–3) / 180 = (3.80 × 10–3) / T or 2.60 × 105 × 3.80 × 10–3 = 0.400 × 8.31 × T C1 T = 297 K A1 2(c)(i) ΔW = pΔV = 2.60 × 105 × (2.30 – 3.80) × 10–3 C1 = (–)390 J A1 negative because work is done by gas or negative because work is done against atmospheric pressure or negative because volume of gas increases B1 2(c)(ii) ΔU = (980 – 390) = 590 J A1
2 (a) The first law of thermodynamics may be expressed as ΔU = (+q) + (+w) where ΔU is the increase in internal energy of the system. State the meaning of: +q … … +w. … … [2] (b) The variation with pressure p of the volume V of a fixed mass of an ideal gas is shown in Fig. 2.1. 4.0 BV / 10–3 m3 3.6 3.2 2.8 2.4 C A 2.0 2.2 2.6 3.0 3.4 3.8 4.2 4.6 5.0 5.4 p / 105 Pa Fig. 2.1 The gas undergoes a cycle of changes A to B to C to A. During the change A to B, the volume of the gas increases from 2.3 × 10–3 m3 to 3.8 × 10–3 m3. (i) Show that the magnitude of the work done during the change A to B is 390 J. [1] (ii) State and explain the total change, if any, in the internal energy of the gas during one complete cycle. … … … [2] (c) During the change A to B, 1370 J of thermal energy is transferred to the gas. During the change B to C, no thermal energy enters or leaves the gas. The work done on the gas during this change is 550 J. Use these data and the information in (b) to complete Table 2.1. Table 2.1 change q / J w / J ΔU / J A to B … … … B to C … … … C to A … … … [4] [Total: 9]
9 marks
Mark scheme: 2(a) +q: thermal energy transfer to system B1 +w: work done on system B1 2(b)(i) (W =) 2.6 ×105 × (3.8 – 2.3) × 10–3 = 390 J A1 2(b)(ii) no (total) change (in internal energy) B1 gas returns to its original temperature B1 2(c) A to B row all correct (1370, – 390, 980) B1 B to C row all correct (0, 550, 550) B1 C to A row: ΔU adds to the other two ΔU values to give zero B1 C to A row: w = 0 and q adds to w to give ΔU value complete correct answer: change q / J w / J ΔU / J A to B B to C C to A (+)1370 0 –1530 –390 (+)550 0 (+)980 (+)550 –1530 B1
2 An ideal gas is contained in a cylinder by means of a movable frictionless piston, as illustrated in Fig. 2.1. cylinder movement of piston piston gas molecule Fig. 2.1 Initially, the gas has a volume of 1.8 × 10−3 m3 at a pressure of 3.3 × 105 Pa and a temperature of 310 K. (a) Show that the number of gas molecules in the cylinder is 1.4 × 1023. [2] (b) Use kinetic theory to explain why, when the piston is moved so that the gas expands, this causes a decrease in the temperature of the gas. … … … … [3] (c) The gas expands so that its volume increases to 2.4 × 10−3 m3 at a pressure of 2.3 × 105 Pa and a temperature of 288 K, as shown in Fig. 2.2. 1.8 × 10−3 m3 2.4 × 10−3 m3 3.3 × 105 Pa 2.3 × 105 Pa 310 K 288 K Fig. 2.2 (i) The average translational kinetic energy EK of a molecule of an ideal gas is given by 3 EK = kT 2 where k is the Boltzmann constant and T is the thermodynamic temperature. Calculate the increase in internal energy ΔU of the gas during the expansion. ΔU = … J [3] (ii) The work done by the gas during the expansion is 76 J. Use your answer in (i) to explain whether thermal energy is transferred to or from the gas during the expansion. … … … [2] [Total: 10]
10 marks
Mark scheme: 2(a) pV = NkT C1 N = (1.8 × 10–3 × 3.3 × 105) / (1.38 × 10–23 × 310) = 1.4 × 1023 A1 or pV = nRT and nNA = N (C1) N = (1.8 × 10–3 × 3.3 × 105 × 6.02 × 1023) / (8.31 × 310) = 1.4 × 1023 (A1) 2(b) speed of molecule decreases on impact with moving piston B1 mean square speed (directly) proportional to (thermodynamic) temperature or mean square speed (directly) proportional to kinetic energy (of molecules) or kinetic energy (of molecules) (directly) proportional to (thermodynamic) temperature B1 kinetic energy (of molecules) decreases (so temperature decreases) B1 2(c)(i) ΔU = 3/2 × k × ΔT × N C1 = 3/2 × 1.38 × 10–23 × (288 – 310) × 1.4 × 1023 C1 = – 64 J A1 2(c)(ii) decrease in internal energy is less than work done by gas M1 (thermal energy is) transferred to the gas (during the expansion) A1
2 An ideal gas has a volume of 3.1 × 10−3 m3 at a pressure of 8.5 × 105 Pa and a temperature of 290 K, as shown in Fig. 2.1. volume 3.1 × 10−3 m3 volume 6.3 × 10−3 m3 pressure 8.5 × 105 Pa pressure 2.7 × 105 Pa temperature 290 K temperature TF Fig. 2.1 The gas suddenly expands to a volume of 6.3 × 10−3 m3. During the expansion, no thermal energy is transferred. The final pressure of the gas is 2.7 × 105 Pa at temperature TF, as shown in Fig. 2.1. (a) Show that the number of gas molecules is 6.6 × 1023. [3] (b) (i) Show that the final temperature TF of the gas is 190 K. [1] (ii) The average translational kinetic energy EK of a molecule of an ideal gas is given by 3 EK = kT 2 where T is the thermodynamic temperature and k is the Boltzmann constant. Calculate the increase in internal energy ΔU of the gas. ΔU = … J [3] (c) Use the first law of thermodynamics to explain why the external work w done on the gas during the expansion is equal to the increase in internal energy in (b)(ii). … … … [2] [Total: 9]
9 marks
Mark scheme: 2(a) pV = nRT C1 pV = nRT and N = nNA or pV = NkT C1 3.1 × 10–3 × 8.5 × 105 = (N × 290 × 8.31) / (6.02 × 1023) so N = 6.6 × 1023 or 3.1 × 10–3 × 8.5 × 105 = N × 1.38 × 10–23 × 290 so N = 6.6 × 1023 A1 2(b)(i) (3.1 × 10–3 × 8.5 × 105) / 290 = (6.3 × 10–3 × 2.7 × 105) / T so T = 190 K or 6.3 × 10–3 × 2.7 × 105 = 6.6 × 1023 × 1.38 × 10–23 × T so T = 190 K A1 2(b)(ii) ΔU = 3/2 × k × ΔT × N C1 = 3/2 × 1.38 × 10–23 × (190 – 290) × 6.6 × 1023 C1 = –1400 J A1 2(c) ΔU = q + w M1 q = 0 so ΔU = w A1
2 An ideal gas is contained in a cylinder by means of a movable frictionless piston, as illustrated in Fig. 2.1. cylinder movement of piston piston gas molecule Fig. 2.1 Initially, the gas has a volume of 1.8 × 10−3 m3 at a pressure of 3.3 × 105 Pa and a temperature of 310 K. (a) Show that the number of gas molecules in the cylinder is 1.4 × 1023. [2] (b) Use kinetic theory to explain why, when the piston is moved so that the gas expands, this causes a decrease in the temperature of the gas. … … … … [3] (c) The gas expands so that its volume increases to 2.4 × 10−3 m3 at a pressure of 2.3 × 105 Pa and a temperature of 288 K, as shown in Fig. 2.2. 1.8 × 10−3 m3 2.4 × 10−3 m3 3.3 × 105 Pa 2.3 × 105 Pa 310 K 288 K Fig. 2.2 (i) The average translational kinetic energy EK of a molecule of an ideal gas is given by 3 EK = kT 2 where k is the Boltzmann constant and T is the thermodynamic temperature. Calculate the increase in internal energy ΔU of the gas during the expansion. ΔU = … J [3] (ii) The work done by the gas during the expansion is 76 J. Use your answer in (i) to explain whether thermal energy is transferred to or from the gas during the expansion. … … … [2] [Total: 10]
10 marks
Mark scheme: 2(a) pV = NkT C1 N = (1.8 × 10–3 × 3.3 × 105) / (1.38 × 10–23 × 310) = 1.4 × 1023 A1 or pV = nRT and nNA = N (C1) N = (1.8 × 10–3 × 3.3 × 105 × 6.02 × 1023) / (8.31 × 310) = 1.4 × 1023 (A1) 2(b) speed of molecule decreases on impact with moving piston B1 mean square speed (directly) proportional to (thermodynamic) temperature or mean square speed (directly) proportional to kinetic energy (of molecules) or kinetic energy (of molecules) (directly) proportional to (thermodynamic) temperature B1 kinetic energy (of molecules) decreases (so temperature decreases) B1 2(c)(i) ΔU = 3/2 × k × ΔT × N C1 = 3/2 × 1.38 × 10–23 × (288 – 310) × 1.4 × 1023 C1 = – 64 J A1 2(c)(ii) decrease in internal energy is less than work done by gas M1 (thermal energy is) transferred to the gas (during the expansion) A1
3 (a) Define specific heat capacity. … … … [2] (b) A sealed container of fixed volume V contains N molecules, each of mass m, of an ideal gas at pressure p. (i) State an expression, in terms of V, N, p and the Boltzmann constant k, for the thermodynamic temperature T of the gas. … [1] (ii) Show that the mean translational kinetic energy EK of a molecule of the gas is given by 3 EK = kT. 2 [2] (iii) Explain why the internal energy of the gas is equal to the total kinetic energy of the molecules. … … … [2] (c) The gas in (b) is supplied with thermal energy Q. (i) Explain, with reference to the first law of thermodynamics, why the increase in internal energy of the gas is Q. … … … [2] (ii) Use the expression in (b)(ii) and the information in (c)(i) to show that the specific heat capacity c of the gas is given by 3k c = . 2m [2] (d) The container in (b) is now replaced with one that does not have a fixed volume. Instead, the gas is able to expand, so that the pressure of the gas remains constant as thermal energy is supplied. Suggest, with a reason, how the specific heat capacity of the gas would now compare with the value in (c)(ii). … … … … [2] [Total: 13]
13 marks
Mark scheme: 3(a) (thermal) energy per unit mass (to cause temperature change) B1 (thermal) energy per unit change in temperature B1 3(b)(i) (T =) pV / Nk B1 3(b)(ii) (pV =) NkT = ⅓Nm<c2> or pV = NkT and pV = ⅓Nm<c2> M1 leading to ½m<c2> = (3/2)kT and ½m<c2> = EK A1 3(b)(iii) internal energy = ΣEK (of molecules) + ΣEP (of molecules) or no forces between molecules B1 potential energy of molecules is zero B1 3(c)(i) increase in internal energy = Q + work done B1 constant volume so no work done B1 3(c)(ii) c = Q / NmΔT C1 = [N × (3/2)kΔT] / (NmΔT) = 3k / 2m A1 3(d) (as it expands) gas does work (against the atmosphere/external pressure) B1 for same temperature rise) more (thermal) energy needed, so larger specific heat capacity B1
3 (a) Define specific heat capacity. … … … [2] (b) A sealed container of fixed volume V contains N molecules, each of mass m, of an ideal gas at pressure p. (i) State an expression, in terms of V, N, p and the Boltzmann constant k, for the thermodynamic temperature T of the gas. … [1] (ii) Show that the mean translational kinetic energy EK of a molecule of the gas is given by 3 EK = kT. 2 [2] (iii) Explain why the internal energy of the gas is equal to the total kinetic energy of the molecules. … … … [2] (c) The gas in (b) is supplied with thermal energy Q. (i) Explain, with reference to the first law of thermodynamics, why the increase in internal energy of the gas is Q. … … … [2] (ii) Use the expression in (b)(ii) and the information in (c)(i) to show that the specific heat capacity c of the gas is given by 3k c = . 2m [2] (d) The container in (b) is now replaced with one that does not have a fixed volume. Instead, the gas is able to expand, so that the pressure of the gas remains constant as thermal energy is supplied. Suggest, with a reason, how the specific heat capacity of the gas would now compare with the value in (c)(ii). … … … … [2] [Total: 13]
13 marks
Mark scheme: 3(a) (thermal) energy per unit mass (to cause temperature change) B1 (thermal) energy per unit change in temperature B1 3(b)(i) (T =) pV / Nk B1 3(b)(ii) (pV =) NkT = ⅓Nm<c2> or pV = NkT and pV = ⅓Nm<c2> M1 leading to ½m<c2> = (3/2)kT and ½m<c2> = EK A1 3(b)(iii) internal energy = ΣEK (of molecules) + ΣEP (of molecules) or no forces between molecules B1 potential energy of molecules is zero B1 3(c)(i) increase in internal energy = Q + work done B1 constant volume so no work done B1 3(c)(ii) c = Q / NmΔT C1 = [N × (3/2)kΔT] / (NmΔT) = 3k / 2m A1 3(d) (as it expands) gas does work (against the atmosphere/external pressure) B1 for same temperature rise) more (thermal) energy needed, so larger specific heat capacity B1
2 A fixed mass of an ideal gas has a volume V and a pressure p. The gas undergoes a cycle of changes, X to Y to Z to X, as shown in Fig. 2.1. Z p Y X 0 0 V Fig. 2.1 Table 2.1 shows data for p, V and temperature T for the gas at points X, Y and Z. Table 2.1 p / 105 Pa V / 10–3 m3 T / K X 1.5 4.2 540 Y 230 Z 5.1 782 (a) State the change in internal energy ΔU for one complete cycle, XYZX. ΔU = … J [1] (b) Calculate the amount n of gas. n = … mol [2] (c) Complete Table 2.1. Use the space below for any working. [2] (d) (i) The first law of thermodynamics for a system may be represented by the equation ΔU = q + W. State, with reference to the system, what is meant by: ΔU : … q : … W : … [3] (ii) Explain how the first law of thermodynamics applies to the change Z to X. … … … … [2] [Total: 10]
10 marks
Mark scheme: 2(a) 0 B1 2(b) pV = nRT (n =) 1.5 × 105 × 4.2 × 10–3 / 8.31 × 540 C1 = 0.14 mol A1 2(c) missing pressure 1.5 (× 105) B1 both missing volumes 1.8 (× 10–3) B1 2(d)(i) (ΔU:) increase in internal energy (of the system) B1 (q:) thermal energy supplied to the system B1 (W:) work done on system B1 Question Answer Marks 2(d)(ii) volume increases and work is done by the gas B1 temperature decreases and internal energy decreases B1
3 (a) Define specific latent heat of vaporisation. … … … [2] (b) The specific latent heat of vaporisation of water at atmospheric pressure of 1.0 × 105 Pa is 2.3 × 106 J kg–1. A mass of 0.37 kg of liquid water at 100 °C is provided with the thermal energy needed to vaporise all of the water at atmospheric pressure. (i) Calculate the thermal energy q supplied to the water. q = … J [1] (ii) The mass of 1.0 mol of water is 18 g. Assume that water vapour can be considered to behave as an ideal gas. Show that the volume of water vapour produced is 0.64 m3. [3] (iii) Assume that the initial volume of the liquid water is negligible compared with the volume of water vapour produced. Determine the magnitude of the work done by the water in expanding against the atmosphere when it vaporises. work done = … J [2] (iv) Use your answers in (b)(i) and (b)(iii) to determine the increase in internal energy of the water when it vaporises at 100 °C. Explain your reasoning. increase in internal energy = … J [2] (c) Use the first law of thermodynamics to suggest, with a reason, how the specific latent heat of vaporisation of water at a pressure greater than atmospheric pressure compares with its value at atmospheric pressure. … … … [2] [Total: 12]
12 marks
Mark scheme: 3(a) (thermal) energy per unit mass B1 energy to change state between liquid and gas at constant temperature B1 3(b)(i) q = mL = 0.37 2.3 106 = 8.5 105 J A1 3(b)(ii) pV = nRT and T = 373 K C1 n = 370 / 18 C1 V = [(370 / 18) 8.31 373] / (1.0 105) = 0.64 m3 A1 3(b)(iii) w = pV C1 = 1.0 105 0.64 = 6.4 104 J A1 3(b)(iv) (water does work against atmosphere so) work done on water is negative B1 increase in internal energy = (8.5 – 0.64) 105 = 7.9 105 J A1 3(c) valid reasoning of how work done by water is affected M1 correct use of first law to draw conclusion about effect on specific latent heat that is consistent with work done A1
2 (a) Define specific heat capacity. … … … [2] (b) A fixed mass of water in a beaker is at atmospheric pressure. (i) The initial temperature of the water is 0 °C. The water is supplied with thermal energy E, so that its temperature increases to 8 °C. There is no net change in the volume of the water. Use the first law of thermodynamics to complete Table 2.1 for this process. Table 2.1 thermal energy increase in internal work done on water supplied to water energy of water + E [2] (ii) The water is now heated so that its temperature increases by a further 8 °C to a final temperature of 16 °C. This process causes the volume of the water to increase so that work W is done. Assume that the change in internal energy is the same as in (b)(i). Use the first law of thermodynamics to complete Table 2.2 for this process. Table 2.2 thermal energy increase in internal work done on water supplied to water energy of water [2] (c) Use the information in (b) to suggest, with a reason, how the average specific heat capacity of water between 8 °C and 16 °C compares with its average value between 0 °C and 8 °C. … … [1] [Total: 7]
7 marks
Mark scheme: 2(a) (thermal) energy per unit mass (to cause temperature change) B1 (thermal) energy per unit change in temperature B1 2(b)(i) work done correct (0) B1 increase in internal energy correct (+E) B1 2(b)(ii) work done correct (–W) and increase in internal energy same as (b)(i) B1 thermal energy correct so that it adds to work done to give increase in internal energy B1 2(c) more thermal energy needed so specific heat capacity is greater B1
3 (a) State the first law of thermodynamics. Identify the meaning of any symbols that you use. … … … [2] (b) The state of an ideal gas is continuously changed according to the cycle ABCDA shown in Fig. 3.1. C D pressure B A volume Fig. 3.1 (i) Complete Table 3.1 for the changes A to B and B to C by placing two ticks (3) in each row. Table 3.1 change in internal energy work done on gas change decrease no change increase negative zero positive A to B B to C [4] (ii) Use the first law of thermodynamics to describe and explain the energy transfers associated with one complete cycle ABCDA. … … … … … [3] [Total: 9]
9 marks
Mark scheme: 3(a) C1 increase in internal energy = work done on system + energy transferred to the system by heating A1 3(b)(i) AB change in internal energy: decrease B1 AB work done on gas: positive B1 BC change in internal energy: increase B1 BC work done on gas: zero B1 3(b)(ii) more work done by gas in CD than is done on gas in AB or (no work done on gas in BC and DA so) (overall) gas does work B1 (overall) change in internal energy is zero B1 (must be an overall) input of thermal energy B1
2 (a) Define specific heat capacity. … … … [2] (b) An ideal gas of mass 0.35 kg is heated at a constant pressure of 2.0 × 105 Pa so that its internal energy increases by 7600 J. During this process, the volume of the gas increases from 0.038 m3 to 0.063 m3 and the temperature increases by 56 °C. (i) Show that the magnitude of the work done on the gas is 5000 J. [1] (ii) Explain whether the work done on the gas is positive or negative. … … … [2] (iii) Determine the magnitude of the thermal energy q transferred to the gas. q = … J [2] (iv) Calculate the specific heat capacity of the gas for this process. Give a unit with your answer. specific heat capacity = … unit … [2] (c) The gas in (b) is now heated at constant volume rather than at constant pressure. The increase in internal energy of the gas is the same as in (b). Use the first law of thermodynamics to explain whether the specific heat capacity of the gas for this process is less than, the same as, or greater than the answer in (b)(iv). … … … … … [3] [Total: 12]
12 marks
Mark scheme: 2(a) (thermal) energy per unit mass (to change temperature) B1 (thermal) energy per unit change in temperature B1 2(b)(i) work done = pV A1 = (2.0 105) (0.063 – 0.038) = 5000 J 2(b)(ii) gas is expanding (against external pressure) B1 gas does work / work is done by gas, so (work done on gas is) negative B1 2(b)(iii) U = q + W C1 7600 = q + (–5000) A1 q = 12 600 J 2(b)(iv) specific heat capacity = q / mT C1 = 12600 / (0.35 56) = 640 J kg–1 K–1 A1 2(c) same gain in internal energy so same temperature rise B1 no change in volume so no work done B1 or no work done so less thermal energy needed (for same change in internal energy) less thermal energy needed (for same temperature change) so lower specific heat capacity B1
3 (a) State what is meant by the internal energy of a system. … … … [2] (b) Use the first law of thermodynamics to explain what happens to the internal energy: (i) of a spring when it is stretched at constant temperature within its elastic limit … … … … … [3] (ii) of a sample of water when it evaporates from a rain puddle on a hot day. … … … … … [3] [Total: 8]
8 marks
Mark scheme: 3(a) sum of potential energy and kinetic energy (of particles) B1 (total) energy of random motion of particles B1 3(b)(i) no thermal energy transferred B1 work is done on the spring (increasing the potential energy of particles) M1 so internal energy increases A1 3(b)(ii) thermal energy transferred to water B1 work is done by water (expanding against atmosphere as it vaporises) B1 more thermal energy transferred than work done so internal energy increases B1
2 (a) Define specific heat capacity. … … … [2] (b) An ideal gas of mass 0.35 kg is heated at a constant pressure of 2.0 × 105 Pa so that its internal energy increases by 7600 J. During this process, the volume of the gas increases from 0.038 m3 to 0.063 m3 and the temperature increases by 56 °C. (i) Show that the magnitude of the work done on the gas is 5000 J. [1] (ii) Explain whether the work done on the gas is positive or negative. … … … [2] (iii) Determine the magnitude of the thermal energy q transferred to the gas. q = … J [2] (iv) Calculate the specific heat capacity of the gas for this process. Give a unit with your answer. specific heat capacity = … unit … [2] (c) The gas in (b) is now heated at constant volume rather than at constant pressure. The increase in internal energy of the gas is the same as in (b). Use the first law of thermodynamics to explain whether the specific heat capacity of the gas for this process is less than, the same as, or greater than the answer in (b)(iv). … … … … … [3] [Total: 12]
12 marks
Mark scheme: 2(a) (thermal) energy per unit mass (to change temperature) B1 (thermal) energy per unit change in temperature B1 2(b)(i) work done = pV A1 = (2.0 105) (0.063 – 0.038) = 5000 J 2(b)(ii) gas is expanding (against external pressure) B1 gas does work / work is done by gas, so (work done on gas is) negative B1 2(b)(iii) U = q + W C1 7600 = q + (–5000) A1 q = 12 600 J 2(b)(iv) specific heat capacity = q / mT C1 = 12600 / (0.35 56) = 640 J kg–1 K–1 A1 2(c) same gain in internal energy so same temperature rise B1 no change in volume so no work done B1 or no work done so less thermal energy needed (for same change in internal energy) less thermal energy needed (for same temperature change) so lower specific heat capacity B1
3 (a) Define specific latent heat. … … … [2] (b) A dish containing 7.2 × 10–5 m3 of a substance rests on a laboratory bench. The substance is initially a liquid of density 710 kg m–3. Atmospheric pressure is 1.0 × 105 Pa. The liquid is heated at its boiling point so that it completely vaporises. The increase in the internal energy of the substance during this process is 17.6 kJ. The final volume of the vapour is 0.017 m3. (i) Show that the magnitude of the work done on the substance when it vaporises is 1.7 kJ. [2] (ii) Use the information in (b)(i) to calculate the thermal energy Q, in kJ, supplied to the substance to cause it to vaporise. Q = … kJ [2] (iii) Use your answer in (b)(ii) to determine a value for the specific latent heat of vaporisation LV, in kJ kg–1, of the substance. LV = … kJ kg–1 [2] (c) The substance in (b) has a specific latent heat of fusion LF. Suggest and explain whether LF is likely to be less than, the same as, or greater than the answer in (b)(iii). … … … … … [3] [Total: 11]
11 marks
Mark scheme: 3(a) (thermal) energy per unit mass (to cause change of state) B1 (thermal) energy to change state at constant temperature B1 3(b)(i) W = pV C1 = 1.0 105 0.017 = 1700 J = 1.7 kJ A1 3(b)(ii) U = Q + W C1 Q = 17.6 + 1.7 A1 = 19.3 kJ 3(b)(iii) mass = 710 7.2 10–5 C1 ( = 0.051 kg) L = 19.3 / 0.051 A1 = 380 kJ kg–1 3(c) fusion involves (much) smaller volume change (than vaporisation) B1 smaller change in intermolecular spacing so smaller change in internal energy B1 negligible work done (by substance during fusion) so LF is less (than LV) B1
3 (a) Define specific heat capacity. … … … [2] (b) A block of aluminium has a volume of 3.612 × 10–3 m3 at a temperature of 0 °C. Aluminium has a density of 2.700 × 103 kg m–3 at 0 °C. It has a density of 2.620 × 103 kg m–3 at 500 °C. The block is heated so that its temperature increases from 0 °C to 500 °C at an atmospheric pressure of 1.01 × 105 Pa. The increase in internal energy of the block is 4.38 MJ. (i) Calculate the mass of the block. mass = … kg [2] (ii) Show that the volume of the block at a temperature of 500 °C is 3.722 × 10–3 m3. [1] (iii) Use the information in (b)(ii) to determine the magnitude of the work done on the block when its temperature is raised from 0 °C to 500 °C. work done = … J [2] (iv) Explain whether the work done on the block is positive or negative. … … … [2] (v) Use the first law of thermodynamics to determine, to three significant figures, a value for the specific heat capacity of aluminium. Explain your reasoning. Give a unit with your answer. specific heat capacity = … unit … [3] (c) Without further calculation, suggest with a reason how doubling the pressure in (b) is likely to affect the answer in (b)(v). … … … [1] [Total: 13]
13 marks
Mark scheme: 3(a) (thermal) energy per unit mass (to cause temperature change) B1 (thermal) energy per unit change in temperature B1 3(b)(i) density = mass / volume C1 mass = 2.700 × 103 × 3.612 × 10–3 A1 = 9.752 kg 3(b)(ii) volume = 3.612 × 10–3 × (2.700 / 2.620) = 3.722 × 10–3 m3 A1 or volume = 9.752 / (2.620 × 103) = 3.722 × 10–3 m3 3(b)(iii) W = pV C1 = 1.01 × 105 × (3.722 – 3.612) × 10–3 A1 = 11.1 J 3(b)(iv) volume (of block) increases B1 work is done against the atmosphere so work done (on block) is negative B1 3(b)(v) thermal energy = (4.38 × 106) + 11.1 B1 specific heat capacity = (4.38 × 106) / (9.75 × 500) C1 = 898 J kg–1 °C–1 A1 3(c) work done is negligible compared with (change in) internal energy so (answer in (b)(v) would be) unchanged B1
2 (a) State two ways in which the first law of thermodynamics describes that the internal energy of a system may be changed. 1 … … 2 … … [2] (b) (i) Use the first law of thermodynamics to explain why a bicycle pump gets hot when it is used to pump up a tyre quickly. … … … … … [3] (ii) With reference to molecular energies, explain why the temperature of water remains at 100 °C when it vaporises in a kettle, even though it is being heated. … … … … … [3] [Total: 8]
8 marks
Mark scheme: 2(a) work done on / by system B1 thermal energy supplied to / removed from system B1 2(b)(i) no thermal energy transferred to / from system (due to lack of time) B1 work is done on the gas to compress it / to decrease its volume B1 internal energy increases so temperature increases B1 2(b)(ii) (during vaporisation) molecular separation increases B1 (heating causes) potential energy of molecules to increase B1 kinetic energy of molecules unchanged so temperature unchanged B1
4 A cylinder contains a fixed mass of an ideal gas at pressure 2Y and volume 6X. The gas undergoes a sequence of changes from its initial state A, through states B, C and D, then finally back to its initial state A, as shown in Fig. 4.1. 6Y pressure C D 4Y 2Y B A 0 0 2X 4X 6X 8X volume Fig. 4.1 Fig. 4.2 shows the variation with time of the internal energy of the gas. 60XY internal energy D 40XY 20XY A A C B 0 time Fig. 4.2 (a) State the first law of thermodynamics. … … … [2] (b) (i) Use Fig. 4.1 and Fig. 4.2 to determine the general expression for the internal energy U of the gas when it has pressure p and volume V. U = … [1] (ii) An ideal gas at thermodynamic temperature T contains N molecules. Use your answer in (b)(i) and the equation of state for an ideal gas to deduce an expression for U in terms of N and T. Identify any other symbols you use. U = … [2] (c) Determine expressions, in terms of X and Y, for the work W done on the gas during: (i) change AB W = … [1] (ii) change CD. W = … [1] (d) Use your answers in (c) and the first law of thermodynamics to determine an expression, in terms of X and Y, for the net thermal energy Q supplied to the gas during one full cycle ABCDA. Explain your reasoning. Q = … [3] [Total: 10]
10 marks
Mark scheme: 4(a) change in internal energy = work done + energy transfer by heating C1 increase in internal energy = work done on system + energy transferred to the system by heating A1 4(b)(i) U = (3 / 2) pV A1 4(b)(ii) pV = NkT and k identified as Boltzmann constant B1 U = (3 / 2) NkT A1 4(c)(i) W = (+)8XY A1 4(c)(ii) W = –20XY A1 4(d) work done during stages BC and DA = 0 B1 change in internal energy (over complete cycle) = 0 C1 thermal energy supplied = 20XY – 8XY A1 = (+)12XY
2 (a) State two ways in which the first law of thermodynamics describes that the internal energy of a system may be changed. 1 … … 2 … … [2] (b) (i) Use the first law of thermodynamics to explain why a bicycle pump gets hot when it is used to pump up a tyre quickly. … … … … … [3] (ii) With reference to molecular energies, explain why the temperature of water remains at 100 °C when it vaporises in a kettle, even though it is being heated. … … … … … [3] [Total: 8]
8 marks
Mark scheme: 2(a) work done on / by system B1 thermal energy supplied to / removed from system B1 2(b)(i) no thermal energy transferred to / from system (due to lack of time) B1 work is done on the gas to compress it / to decrease its volume B1 internal energy increases so temperature increases B1 2(b)(ii) (during vaporisation) molecular separation increases B1 (heating causes) potential energy of molecules to increase B1 kinetic energy of molecules unchanged so temperature unchanged B1