aimnova.
DashboardMy LearningPaper MasteryStudy Plan

Stay in the loop

Study tips, product updates, and early access to new features.

aimnova.

AI-powered IB study platform with personalised plans, instant feedback, and examiner-style marking.

IB Subjects
  • All IB Subjects
  • IB Diploma
  • IB ESS
  • IB Economics
  • IB Business Management
  • IB Math AI
  • IB Math AA
  • IB Physics
  • IB Biology
  • IB Chemistry
  • IB History
  • IB History (2028+)
  • IB Global Politics
  • IB Psychology
  • IB Philosophy
  • IB Geography
  • IB Spanish B
  • IB German B
  • IB Italian B
  • IB French B
  • IB English B
  • IB English A Lang & Lit
  • IB Spanish A Lang & Lit
  • IB French A Lang & Lit
Question Banks
  • ESS Question Bank
  • Economics Question Bank
  • Business Management Question Bank
  • Math AI Question Bank
  • Math AA Question Bank
  • Physics Question Bank
  • Biology Question Bank
  • Chemistry Question Bank
  • History Question Bank
  • History (2028+) Question Bank
  • Global Politics Question Bank
  • Psychology Question Bank
  • Philosophy Question Bank
  • Geography Question Bank
  • Spanish B Question Bank
  • German B Question Bank
  • Italian B Question Bank
  • French B Question Bank
  • English B Question Bank
  • English A Lang & Lit Question Bank
  • Spanish A Lang & Lit Question Bank
  • French A Lang & Lit Question Bank
Predicted Topics 2026
  • ESS Predictions 2026
  • Economics Predictions 2026
  • Business Management Predictions 2026
  • Math AI Predictions 2026
  • Math AA Predictions 2026
  • Physics Predictions 2026
  • Geography Predictions 2026
  • Spanish B Predictions 2026
  • German B Predictions 2026
  • Italian B Predictions 2026
  • French B Predictions 2026
  • English B Predictions 2026

Study Resources

  • Free Study Notes
  • Mock Exams
  • Revision Guide
  • Flashcards
  • Exam Skills
  • Command Terms
  • Past Paper Feedback
  • Grade Calculator
  • Exam Timetable 2026

Company

  • Features
  • Pricing
  • About Us
  • Blog
  • Contact
  • Terms
  • Privacy
  • Cookies

© 2026 Aimnova. All rights reserved.

Made with 💜 for IB students worldwide

c059741
NotesPhysics HLTopic 2.1
Unit 2 · The particulate nature of matter · Topic 2.1

IB Physics HL — Thermal energy transfers

Topic 2.1 of IB Physics covers Thermal energy transfers, which is part of Unit 2: The particulate nature of matter. Students explore key concepts including Internal energy and the particle model, Specific heat capacity, Latent heat and calorimetry, Conduction, convection and radiation. A strong understanding of thermal energy transfers is essential for IB Physics HL exams and builds the foundation for connected topics across the syllabus.

Higher Level students should use this topic hub as a map: start with the shared sub-topics, then follow the HL-only extensions and exam-skill links where this topic asks for deeper analysis.

Exam technique guidePractice questions

Key concepts in Thermal energy transfers

Key Idea: Topic 2.1 is about how thermal energy is stored in matter and how it moves from hot to cold. It ties together four ideas: what internal energy is (and the particle model), how much energy a temperature change needs (Q = mcΔT), the hidden energy of a state change (Q = mL), and the three ways heat travels — conduction, convection and radiation. It is examined on Paper 1A (quick MCQs — define internal energy, compare densities, spot which formula a heating-curve part needs) and on Paper 2 (rearrange Q = mcΔT, energy-balance/calorimetry with latent heat, and the conduction rate ΔQ/Δt = kA·ΔT/Δx with its unit, the watt).

📐 Key formulas (all four are given)

Every equation in this topic is given in the data booklet — so you do not memorise them, but you must know which one to reach for and how to rearrange it.

ρ=mV\rho = \frac{m}{V}ρ=Vm​
Density = mass ÷ volume. Lets you compare how tightly packed a solid and a liquid are.
ρ\rhoρ
density (kg m⁻³)
mmm
mass (kg)
VVV
volume (m³)
Q=mcΔTQ = mc\Delta TQ=mcΔT
Specific heat capacity — the energy for a TEMPERATURE change (no state change). Rearrange to c = Q ÷ (mΔT) or m = Q ÷ (cΔT).
QQQ
thermal energy added or removed (J)
mmm
mass (kg)
ccc
specific heat capacity (J kg⁻¹ K⁻¹)
ΔT\Delta TΔT
temperature change (K, or °C — same size)
Q=mLQ = mLQ=mL
Latent heat — the energy for a STATE change at constant temperature (melting/boiling). No ΔT term.
QQQ
thermal energy transferred (J)
mmm
mass changing state (kg)
LLL
specific latent heat (J kg⁻¹)
ΔQΔt=kA ΔTΔx\frac{\Delta Q}{\Delta t} = kA\,\frac{\Delta T}{\Delta x}ΔtΔQ​=kAΔxΔT​
Rate of thermal conduction, in watts (W). Thickness Δx is on the bottom, so rate ∝ 1 ÷ thickness.
ΔQΔt\frac{\Delta Q}{\Delta t}ΔtΔQ​
rate of heat flow — energy each second (W, i.e. J s⁻¹)
kkk
thermal conductivity of the material (W m⁻¹ K⁻¹)
AAA
cross-sectional area the heat flows through (m²)
ΔT\Delta TΔT
temperature difference across the slab (K or °C)
Δx\Delta xΔx
thickness of the slab (m)

🧭 Which equation, and when?

The single most-tested decision in this topic: is the temperature changing (a slope) or is the state changing (a flat plateau at constant temperature)?

SituationWhat is changingEquation to use
Warming or cooling a substanceTemperature (a sloping line)Q = mcΔT
Melting / freezing, boiling / condensingState, at constant temperature (a flat line)Q = mL
Comparing how tightly matter is packedMass per volumeρ = m/V
Heat conducting through a wall, window or iceRate of heat flow (per second)ΔQ/Δt = kA·ΔT/Δx

🔥 The three ways heat travels

MechanismWhat actually movesNeeds a material?Everyday example
Conductionenergy passes along; particles stay putYes — best in solids (esp. metals)a metal spoon's handle getting hot
Convectionthe hot fluid itself rises and circulatesYes — only in fluidswarm air rising off a radiator
Radiationinfrared waves (no particles needed)No — crosses a vacuumthe Sun's heat reaching Earth

🧊 Latent heats — fusion vs vaporisation

QuantityState change it coversRelative size
Latent heat of fusion (Lf)melting ↔ freezingsmaller — the shorter plateau
Latent heat of vaporisation (Lv)boiling ↔ condensingmuch larger — the longer plateau

✍️ IB-style worked examples

IB-style questionCalculate[2 marks]

A heater warms 0.40 kg of water from 15 °C to 65 °C. The specific heat capacity of water is 4200 J kg⁻¹ K⁻¹. Calculate the thermal energy supplied.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

Unlock free for 7 days →
IB-style questionCalculate[3 marks]

0.20 kg of ice at −10 °C is heated until it is water at 0 °C. Take c(ice) = 2.1 × 10³ J kg⁻¹ K⁻¹ and L(fusion) = 3.3 × 10⁵ J kg⁻¹. Find the total energy needed.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

Unlock free for 7 days →
IB-style questionCalculate[3 marks]

Heat conducts through a wall of area 5.0 m² and thickness 0.25 m, with k = 0.60 W m⁻¹ K⁻¹. Inside is 21 °C and outside is 6 °C. Calculate the rate of heat loss, give its unit, and state what happens to it if the wall is made twice as thick.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

Unlock free for 7 days →
IB-style questionDetermine[3 marks]

0.15 kg of water at 40 °C is poured onto ice already at 0 °C; the water cools to 0 °C and some ice melts. Take c(water) = 4.2 × 10³ J kg⁻¹ K⁻¹ and L(fusion) = 3.3 × 10⁵ J kg⁻¹. Assuming no energy is lost, find the mass of ice melted.

🔒 Model answer plan

See the mark-by-mark plan — for / against / judgement, with marking guidance — in study mode.

Unlock free for 7 days →

✅ Quick self-check

Tap each card to reveal the answer.

What are the two parts of internal energy? Total random kinetic energy of the particles (sets the temperature) + total intermolecular potential energy (depends on spacing).

What does ΔT mean in Q = mcΔT? The temperature change (final − start), not the actual temperature. A change of 1 K equals a change of 1 °C, so never convert.

Slope vs flat on a heating curve — which formula? Sloping (temperature changing) → Q = mcΔT. Flat (state changing at constant temperature) → Q = mL.

Why is the boiling plateau longer than the melting one? For one substance Lv ≫ Lf: vaporising fully separates the particles, needing far more energy than melting.

Which heat transfer works through a vacuum? Radiation only — it travels as infrared waves and needs no material; conduction and convection both need particles.

A wall is made twice as thick. What happens to the conduction rate? It halves — Δx is on the bottom of ΔQ/Δt = kA·ΔT/Δx, so rate ∝ 1 ÷ thickness.


🎯 Highest-yield exam reminders

Exam Tips

  • Internal energy = random KE + intermolecular PE — always name BOTH parts; never forget the PE. Temperature tracks only the KE part.
  • ΔT in Q = mcΔT is a temperature CHANGE (final − start), and a change in K equals a change in °C — never convert ΔT to kelvin.
  • Decide slope vs flat: temperature changing ⇒ Q = mcΔT; state changing at constant temperature ⇒ Q = mL (no ΔT). Multi-step problems need one Q-term per step.
  • Lv ≫ Lf for the same substance, so boiling needs much more energy than melting — that is the longer plateau and the reason steam burns are worse than hot-water burns.
  • Calorimetry with no losses: energy lost by the hot part = energy gained by the cold part. A measured value is usually 'off' because heat escapes to the surroundings or the container.
  • The conduction rate ΔQ/Δt = kA·ΔT/Δx is a RATE — its unit is the watt (W). Work out ΔT first; thickness Δx is on the bottom, so a thicker layer conducts more slowly (rate ∝ 1 ÷ thickness).
  • A cooling curve flattens because the temperature difference driving the heat loss keeps shrinking — smaller difference, smaller gradient. Only radiation crosses a vacuum.

What you'll learn in Topic 2.1

  • 2.1.1 Internal energy and the particle model
  • 2.1.2 Specific heat capacity
  • 2.1.3 Latent heat and calorimetry
  • 2.1.4 Conduction, convection and radiation
Suggested study order: Read the notes for each sub-topic below → test yourself with flashcards → attempt practice questions → review exam technique.

Study resources — 2.1 Thermal energy transfers

2.1.1

Internal energy and the particle model

Notes
2.1.2

Specific heat capacity

Notes
2.1.3

Latent heat and calorimetry

Notes
2.1.4

Conduction, convection and radiation

Notes

Ready to study Thermal energy transfers?

Get expert practice questions with instant AI feedback, and a study planner tailored to your IB Physics HL exam date.

Start studying free

Topic 2.1 Thermal energy transfers forms a core part of Unit 2: The particulate nature of matter in IB Physics HL. Mastering these concepts will strengthen your understanding of connected topics across the syllabus and prepare you for exam questions that require analysis, evaluation, and real-world application.

Previous topic
1.5 Galilean and special relativity (HL)
Next topic
2.2 Greenhouse effect
All Physics HL topics
Exam technique

Ready to practice?

Get AI-graded practice questions, mock exams, flashcards, and a personalised study plan — all aligned to your IB syllabus.

Start Studying Free

No credit card required · Cancel anytime