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QLDPhysicsSyllabus dot point

Topic 1: Heating processes

Solve problems involving specific heat capacity (Q=mcΔTQ = mc\Delta T) and specific latent heat (Q=mLQ = mL) of fusion and vaporisation, including state changes

A focused answer to the QCE Physics Unit 1 dot point on specific heat capacity and latent heat. Applies Q=mcΔTQ = mc\Delta T and Q=mLQ = mL to heating, cooling and phase-change calculations, and works the QCAA-style multi-stage problem (heating ice, melting, heating water, vaporising) used in EA Paper 1.

Generated by Claude Opus 4.88 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. Specific heat capacity
  3. Latent heat
  4. Conservation of energy in heat exchanges
  5. Examples in context
  6. Try this

What this dot point is asking

QCAA wants you to apply Q=mcΔTQ = mc\Delta T to temperature changes within a single phase, and Q=mLQ = mL 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 (cc) of a substance is the energy required to raise the temperature of 11 kg by 11 K:

Q=mcΔTQ = m c \Delta T

where QQ is heat (J), mm is mass (kg), cc is specific heat capacity (J kg1^{-1} K1^{-1}) and ΔT\Delta T is temperature change (K or °C; the size of the unit is identical).

Typical values to know: cwater=4186c_{\text{water}} = 4186 J kg1^{-1} K1^{-1}, cice=2100c_{\text{ice}} = 2100, caluminium=900c_{\text{aluminium}} = 900, ccopper=385c_{\text{copper}} = 385. Water has an unusually high specific heat, which is why coastal climates are mild.

A positive QQ means heat absorbed and temperature rises. A negative QQ (or negative ΔT\Delta T) 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.

Q=mLQ = m L

  • LfL_f = specific latent heat of fusion (solid to liquid). For water, Lf=3.34×105L_f = 3.34 \times 10^5 J kg1^{-1}.
  • LvL_v = specific latent heat of vaporisation (liquid to gas). For water, Lv=2.26×106L_v = 2.26 \times 10^6 J kg1^{-1}.

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:

Qlost by hot=Qgained by coldQ_{\text{lost by hot}} = Q_{\text{gained by cold}}

This is the principle behind calorimetry. Set up the equation, substitute mcΔTm c \Delta T on each side, and solve for the unknown (final temperature or unknown specific heat).

Examples in context

Example 1. A Bundaberg sugar mill heats 1500 kg1500 \text{ kg} of raw juice from 25C25^\circ \text{C} to 90C90^\circ \text{C} before evaporation. With c=3850 J kg1 K1c = 3850 \text{ J kg}^{-1} \text{ K}^{-1} (sugar solution), Q=mcΔT=1500×3850×65=3.75×108 JQ = mc\Delta T = 1500 \times 3850 \times 65 = 3.75 \times 10^8 \text{ J} per batch, supplied by bagasse-fired steam. The mill then vaporises 1000 kg1000 \text{ kg} of water in evaporators using Q=mLv=1000×2.26×106=2.26×109 JQ = mL_v = 1000 \times 2.26 \times 10^6 = 2.26 \times 10^9 \text{ J}, an order of magnitude larger because LvL_v exceeds cΔTc\Delta T. 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 5000 kg5000 \text{ kg} of strawberries (effective c3900 J kg1 K1c \approx 3900 \text{ J kg}^{-1} \text{ K}^{-1}) at intake at 28C28^\circ \text{C}, cooling them to 4C4^\circ \text{C}. The sensible-heat load is Q=5000×3900×24=4.68×108 JQ = 5000 \times 3900 \times 24 = 4.68 \times 10^8 \text{ J}. If 200 kg200 \text{ kg} of surface dew freezes en route (Lf=3.34×105 J kg1L_f = 3.34 \times 10^5 \text{ J kg}^{-1}), an extra Q=6.68×107 JQ = 6.68 \times 10^7 \text{ J} 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. Q=mcΔTQ = mc\Delta T (no phase change); Q=mLQ = mL (at phase change).

Q2. Calculate the energy needed to heat 0.50 kg0.50 \text{ kg} of water from 20C20^\circ \text{C} to 100C100^\circ \text{C} (c=4186 J kg1 K1c = 4186 \text{ J kg}^{-1} \text{ K}^{-1}) and then boil it all to steam (Lv=2.26×106 J kg1L_v = 2.26 \times 10^6 \text{ J kg}^{-1}). [3 marks]

  • Cue. Heating 1.67×105 J1.67 \times 10^5 \text{ J}; vaporising 1.13×106 J1.13 \times 10^6 \text{ J}; total 1.30×106 J1.30 \times 10^6 \text{ J}.

Q3. A Bundaberg mill needs to raise 2000 kg2000 \text{ kg} of juice (c=3850 J kg1 K1c = 3850 \text{ J kg}^{-1} \text{ K}^{-1}) from 30C30^\circ \text{C} to 95C95^\circ \text{C}. (a) Calculate the heat required. (b) The boiler delivers 750 kW750 \text{ kW}. 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) 5.01×108 J5.01 \times 10^8 \text{ J}; (b) 668 s668 \text{ s} or 11.1 min11.1 \text{ min}; (c) higher ambient reduces feedwater ΔT\Delta T recovery, lowering throughput.

Exam-style practice questions

Practice questions written in the style of QCAA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Year 11 SAC5 marksCalculate the total energy required to heat 200200 g of ice from 10°-10°C to water at 30°30°C. Use cice=2100c_{\text{ice}} = 2100 J kg1^{-1} K1^{-1}, cwater=4186c_{\text{water}} = 4186 J kg1^{-1} K1^{-1} and Lf=3.34×105L_f = 3.34 \times 10^5 J kg1^{-1}.
Show worked answer →

Split into three stages.

Stage 1. Warm ice from 10°-10°C to 0°C.

Q1=mcΔT=(0.200)(2100)(10)=4200Q_1 = mc \Delta T = (0.200)(2100)(10) = 4200 J.

Stage 2. Melt ice at 0°C.

Q2=mLf=(0.200)(3.34×105)=66800Q_2 = m L_f = (0.200)(3.34 \times 10^5) = 66\,800 J.

Stage 3. Warm water from 0°C to 30°30°C.

Q3=mcΔT=(0.200)(4186)(30)=25116Q_3 = mc \Delta T = (0.200)(4186)(30) = 25\,116 J.

Total =4200+66800+25116=9.61×104= 4200 + 66\,800 + 25\,116 = 9.61 \times 10^4 J.

Markers reward splitting at every phase boundary, correct use of mass in kilograms, and a final answer in scientific notation with units.

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