Specific heat capacity and latent heat (QCE Physics Unit 1)
“Solve problems involving specific heat capacity () and specific latent heat () of fusion and vaporisation, including state changes”
Within a single phase, heat is related to temperature change by (specific heat capacity), and at a phase change heat is absorbed or released at constant temperature according to (latent heat of fusion or vaporisation), with energy conserved in insulated heat exchanges so the heat lost by hotter bodies equals the heat gained by colder bodies.
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What this dot point is asking
QCAA wants you to apply to temperature changes within a single phase, and to the energy absorbed or released when a substance changes phase at constant temperature. Both equations together solve the standard multi-stage heating problem.
Specific heat capacity
The specific heat capacity () of a substance is the energy required to raise the temperature of kg by K:
where is heat (J), is mass (kg), is specific heat capacity (J kg K) and is temperature change (K or °C; the size of the unit is identical).
Typical values to know: J kg K, , , . Water has an unusually high specific heat, which is why coastal climates are mild.
A positive means heat absorbed and temperature rises. A negative (or negative ) means heat released and temperature falls.
Latent heat
When a substance changes phase, energy is absorbed or released without a temperature change. Particles are gaining or losing the potential energy needed to break or form intermolecular bonds.
- = specific latent heat of fusion (solid to liquid). For water, J kg.
- = specific latent heat of vaporisation (liquid to gas). For water, J kg.
Vaporisation is much more energy-intensive than fusion because all intermolecular bonds must be broken, not just rearranged.
Conservation of energy in heat exchanges
If two bodies exchange heat in an insulated container, energy is conserved:
This is the principle behind calorimetry. Set up the equation, substitute on each side, and solve for the unknown (final temperature or unknown specific heat).
A g aluminium block at C is placed in g of water at C in an insulated container. We find the final equilibrium temperature using conservation of energy.
Step 1: Set up the conservation of energy equation
In an insulated container no energy escapes, so the heat lost by the hot aluminium exactly equals the heat gained by the cooler water. We write for each substance, with as the unknown final temperature.
The left side represents heat leaving the aluminium (which starts hotter than ) and the right side represents heat entering the water (which starts cooler than ). Both terms are positive if lies between C and C.
Step 2: Expand and collect terms in
Multiplying out each side gives numerical coefficients.
Collecting all terms involving on the right and constants on the left:
Step 3: Solve for the final temperature
Final answer: the equilibrium temperature is approximately C. The result sits much closer to the water's initial temperature of C than to aluminium's C, because the water has a far higher heat capacity and therefore dominates the thermal balance.
- Using grams instead of kilograms
- Both formulas are written for SI units. A g sample is kg, not kg.
- Treating temperature change in celsius differently from kelvin
- C K. Both are correct because the units of temperature interval are identical in size.
- Forgetting to include the phase change
- A common QCAA trap is "ice at C to water at C". You need three stages: warm ice, melt ice, warm water. Skipping the latent heat gives an answer about times too small.
Using for boiling water at C all the way to steam at a higher temperature. Latent heat covers the phase change at C only. Heating the steam further uses on top.
Examples in context
Example 1. A Bundaberg sugar mill heats of raw juice from to before evaporation. With (sugar solution), per batch, supplied by bagasse-fired steam. The mill then vaporises of water in evaporators using , an order of magnitude larger because exceeds . The QCAA Unit 1 EA Paper 1 industrial stem is a direct lift from this kind of process calculation.
Example 2. A Sunshine Coast cool-store handles of strawberries (effective ) at intake at , cooling them to . The sensible-heat load is . If of surface dew freezes en route (), an extra is removed. Refrigeration sizing in Queensland packing houses combines both terms, as the QCAA dot point demands.
Try this
Q1. State the specific heat capacity equation and the specific latent heat equation, defining each symbol. [2 marks]
- Cue. (no phase change); (at phase change).
Q2. Calculate the energy needed to heat of water from to () and then boil it all to steam (). [3 marks]
- Cue. Heating ; vaporising ; total .
Q3. A Bundaberg mill needs to raise of juice () from to . (a) Calculate the heat required. (b) The boiler delivers . Determine the heating time. (c) Explain why the boiler may be derated in tropical summer conditions. [3+2+2 marks; ISMG: Analysis and interpretation, Evaluation]
- Cue. (a) ; (b) or ; (c) higher ambient reduces feedwater recovery, lowering throughput.
Exam-style questions
Questions in the style of QCAA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.
Year 11 SAC-style5 marksCalculate the total energy required to heat g of ice from C to water at C. Use J kg K, J kg K and J kg.Show worked answer →
Split into three stages.
Stage 1. Warm ice from C to C.
J.
Stage 2. Melt ice at C.
J.
Stage 3. Warm water from C to C.
J.
Total J.
Markers reward splitting at every phase boundary, correct use of mass in kilograms, and a final answer in scientific notation with units.