Physics
Thermal physics and ideal gases
- 1.
A 0.250 kg aluminium block warms from 20.0 to 60.0 degrees C. Specific heat capacity is 900 J kg^-1 K^-1. Find energy transferred, assuming no losses, to 3 significant figures.
[3 marks]Answer explanation
Draft walkthroughs are based on marking guidance, not independently verified derivations.
- Temperature differences have the same numerical size in kelvin and Celsius.
- Only the difference belongs in mc delta T; multiplying by the final temperature would overestimate energy.
Marking points
- Temperature change is 40.0 K.
- Q = mc delta T.
- Q = 9.00e3 J.
Examiner tip: Do not add 273 to a temperature change.
- 2.
A fixed amount of ideal gas in a sealed rigid container is initially at 100 kPa and 300 K. It is heated at fixed volume to 450 K with no gas entering or leaving. Find final pressure and explain the molecular reason.
[3 marks]Answer explanation
Draft walkthroughs are based on marking guidance, not independently verified derivations.
- From pV = nRT, all factors except p and T remain fixed.
- Both more frequent impacts and greater momentum changes contribute to greater pressure in the ideal kinetic model.
Marking points
- At fixed amount and volume, p/T is constant.
- Final pressure is 150 kPa.
- Higher mean molecular kinetic energy increases momentum transfer to walls per unit time.
Examiner tip: Use absolute temperature in gas ratios.
- 3.
Mix 0.200 kg water at 80.0 degrees C with 0.300 kg water at 20.0 degrees C. Find equilibrium temperature. Neglect heat loss and container heat capacity; specific heat is identical and constant.
[3 marks]Answer explanation
Draft walkthroughs are based on marking guidance, not independently verified derivations.
- The final temperature is a mass-weighted average, not an arithmetic mean of the temperatures.
- More cold water shifts the result below 50 degrees C; both samples reach the same final temperature.
Marking points
- Heat lost equals heat gained: 0.200c(80.0 - T) = 0.300c(T - 20.0).
- Cancel c and solve 22.0 = 0.500T.
- T = 44.0 degrees C.
Examiner tip: Container heat capacity would change the balance unless it were negligible as stated.
- 4.
Find rms molecular speed for an ideal gas at 300 K with molar mass 0.0280 kg mol^-1, using R = 8.31 J mol^-1 K^-1. Explain why this is not the mean velocity. Give 3 significant figures.
[3 marks]Answer explanation
Draft walkthroughs are based on marking guidance, not independently verified derivations.
- The molar form pairs R with mass per mole, not mass per molecule.
- Squaring speed before averaging prevents cancellation of opposite directions.
Marking points
- v_rms = sqrt(3RT/M).
- v_rms = 517 m s^-1.
- In equilibrium random directions make mean velocity zero, while mean squared speed is positive.
Examiner tip: Convert grams per mole to kilograms per mole before using SI R.
- 5.
Place 0.0500 kg ice at 0 degrees C in 0.200 kg water at 30.0 degrees C in an insulated container of negligible heat capacity. Use c_water = 4200 J kg^-1 K^-1 and L_f = 3.34e5 J kg^-1. Decide whether all ice melts and find final temperature.
[3 marks]Answer explanation
Draft walkthroughs are based on marking guidance, not independently verified derivations.
- Test the melting energy first; if the warm water could not supply it the final state would contain ice at zero degrees C.
- After melting, the original water and melted ice share the surplus 8500 J over a combined mass 0.250 kg.
Marking points
- Water can release 25200 J cooling to 0 degrees C; melting needs 16700 J, so all ice melts.
- 0.200c(30.0 - T) = 0.0500L_f + 0.0500cT.
- Final temperature is 8.10 degrees C (3 significant figures).
Examiner tip: Include both latent heat and warming of the melted water.
- 6.
Exactly 0.500 mol ideal gas expands reversibly and isothermally at 300 K from 0.0100 to 0.0200 m^3. Given work by gas W = nRT ln(V2/V1), use R = 8.31 J mol^-1 K^-1 to find work and heat supplied. State internal energy change and the sign convention.
[3 marks]Answer explanation
Draft walkthroughs are based on marking guidance, not independently verified derivations.
- The logarithmic work follows from integrating p = nRT/V during quasistatic expansion.
- Heat must replace the energy leaving as work to keep the ideal gas temperature constant.
Marking points
- W = 0.500*8.31*300*ln(2) = 864 J (3 significant figures), positive for expansion.
- Ideal-gas internal energy depends only on temperature, so delta U = 0 J.
- Using delta U = Q - W with Q into gas positive, heat supplied Q = 864 J.
Examiner tip: Isothermal does not mean no heat transfer; it means constant temperature.
Marking points are indicative, not an official mark scheme. Accept equivalent valid methods and supported interpretations that address the task; award each mark once without requiring the model wording.