Skip to topic
    ← Back to course topics

    Thermodynamics — Edexcel A-Level Physics

    Test yourself on Thermodynamics with PEARSON EDEXCEL A-Level practice questions.

    Start free

    7 days Premium · Then free forever · No card, no charge

    Thermodynamics explained

    This topic covers the fundamental principles of electric circuits, including the definitions of current, potential difference, and resistance.

    Read the full explanation

    It explores the conservation of charge and energy in series and parallel circuits, the properties of various electrical components, and the application of Ohm's law and resistivity.

    What to demonstrate

    1. Use of I = ΔQ/Δt
    2. Use of V = W/Q
    3. Use of R = V/I
    Show all 13 objectives
    1. Application of charge conservation in circuits
    2. Application of energy conservation in circuits
    3. Derivation and use of series and parallel resistance formulas
    4. Use of P = VI, P = I²R, P = V²/R, and W = VIt
    5. Interpretation of I-V graphs for ohmic conductors, filament bulbs, thermistors, and diodes
    6. Use of R = ρl/A
    7. Use of I = nqvA
    8. Analysis of potential divider circuits
    9. Distinction between e.m.f. and terminal potential difference
    10. Modeling resistance changes with temperature and illumination

    Thermodynamics exam tips

    Topic Overview

    Thermodynamics in A-Level Physics (Edexcel) explores the principles governing energy transfer, heat, and work. It builds on GCSE ideas of energy conservation and introduces key concepts like internal energy, specific heat capacity, and the first law of thermodynamics. You'll learn how to calculate energy changes in systems, understand the behaviour of gases, and apply the second law to explain why processes have a natural direction. This topic is crucial for understanding engines, refrigerators, and even the fate of the universe.

    The topic is divided into two main areas: thermal properties of materials and the kinetic theory of gases. You'll derive the ideal gas equation from molecular motion, calculate work done by gases, and use the first law (ΔU = Q + W) to analyse energy transfers. The second law introduces entropy, explaining why heat flows from hot to cold and why perpetual motion machines are impossible. These ideas are fundamental to engineering, meteorology, and cosmology.

    Mastering thermodynamics requires strong algebraic skills and the ability to interpret graphs (e.g., pressure-volume diagrams). You'll need to apply equations like pV = nRT, ΔU = Q + W, and efficiency = 1 - (Tc/Th). Practical skills are tested through experiments like measuring specific heat capacity or verifying Boyle's law. This topic appears in both multiple-choice and long-answer questions, often requiring you to explain concepts in words as well as calculations.

    Key Concepts
    • →Internal energy (U): the sum of the random kinetic and potential energies of particles in a system. For an ideal gas, it depends only on temperature.
    • →First law of thermodynamics: ΔU = Q + W, where Q is heat added to the system and W is work done on the system. Sign conventions are critical.
    • →Specific heat capacity (c) and specific latent heat (L): c = ΔQ/(mΔT) and L = ΔQ/m. Used to calculate energy changes during heating or phase changes.
    • →Ideal gas equation: pV = nRT, where R = 8.31 J mol⁻¹ K⁻¹. Combined with kinetic theory to relate pressure to molecular speed: pV = ⅓ Nm(c²).
    • →Second law and entropy: entropy (ΔS = ΔQ/T) increases in spontaneous processes. Efficiency of a heat engine is limited by Carnot efficiency: η_max = 1 - Tc/Th.
    Marking Points
    • Use of I = ΔQ/Δt
    • Use of V = W/Q
    • Use of R = V/I
    • Application of charge conservation in circuits
    • Application of energy conservation in circuits
    • Derivation and use of series and parallel resistance formulas
    • Use of P = VI, P = I²R, P = V²/R, and W = VIt
    • Interpretation of I-V graphs for ohmic conductors, filament bulbs, thermistors, and diodes
    • Use of R = ρl/A
    • Use of I = nqvA
    • Analysis of potential divider circuits
    • Distinction between e.m.f. and terminal potential difference
    • Modeling resistance changes with temperature and illumination
    Examiner Tips
    • 💡Ensure all calculations are shown clearly with appropriate units
    • 💡Be prepared to interpret I-V characteristics for non-ohmic components
    • 💡Practice analyzing potential divider circuits with variable resistors
    • 💡Understand the physical models behind resistance changes in thermistors and LDRs
    • 💡Use significant figures appropriately in all calculations
    • 💡Always state the sign convention for Q and W when using the first law. Many marks are lost for incorrect signs. Typically, Q positive = heat into system, W positive = work done on system.
    • 💡For efficiency questions, remember that Carnot efficiency is the maximum possible. If a question gives temperatures, use Kelvin. If it gives a real engine, compare its efficiency to Carnot to see if it's possible.
    • 💡When deriving the ideal gas equation from kinetic theory, be methodical: start with pressure = force/area, use momentum change per collision, and include the average speed squared. Show all steps for full marks.
    Common Mistakes
    • Confusing e.m.f. with terminal potential difference
    • Incorrectly applying Ohm's law to non-ohmic components
    • Misinterpreting I-V graphs for non-linear components
    • Errors in deriving or applying series and parallel resistance formulas
    • Incorrect use of units for resistivity and other derived quantities
    • Misconception: 'Work done by a gas is always positive.' Correction: In the first law, W is work done ON the system. So when a gas expands, it does work on the surroundings, meaning W (on gas) is negative. Always check sign conventions.
    • Misconception: 'Specific heat capacity and specific latent heat are the same thing.' Correction: Specific heat capacity involves temperature change without phase change; specific latent heat involves phase change at constant temperature.
    • Misconception: 'Entropy always increases in a system.' Correction: The second law says total entropy of the universe increases. A system can decrease in entropy if it is not isolated (e.g., a fridge).
    Frequently Asked Questions
    What is the difference between heat and temperature in thermodynamics?
    Heat is energy transferred between systems due to a temperature difference, measured in joules. Temperature is a measure of the average kinetic energy of particles, measured in Kelvin or Celsius. Two objects can have the same temperature but different heat capacities, meaning they store different amounts of thermal energy.
    How do I remember the sign convention for the first law of thermodynamics?
    Think of the system: if energy enters the system, it's positive. So heat added to the system (Q > 0) and work done on the system (W > 0) both increase internal energy. If the system does work on surroundings (expansion), W is negative. A common mnemonic is 'QW' - Q and W are positive when they increase U.
    What is entropy and why does it always increase?
    Entropy is a measure of disorder or the number of ways energy can be distributed. The second law states that in any spontaneous process, the total entropy of the universe increases. This is because there are more ways for energy to be spread out than concentrated, making high-entropy states more probable. For example, a hot object cools because the energy spreads into more particles.
    How do I calculate work done by a gas in a thermodynamic cycle?
    Work done by a gas is the area under the pressure-volume (p-V) graph. For a cycle, the net work is the area enclosed by the cycle. If the cycle is clockwise, net work is done by the gas (positive work by gas, negative work on gas). For an isothermal expansion, use W = nRT ln(V2/V1). For an isobaric process, W = pΔV.
    What is the Carnot efficiency and why can't real engines achieve it?
    Carnot efficiency is the maximum possible efficiency of a heat engine operating between two temperatures, given by η = 1 - Tc/Th (in Kelvin). Real engines cannot achieve it because they have irreversible processes like friction, heat loss, and non-quasistatic expansion. The Carnot cycle is an idealised reversible cycle that sets an upper limit.
    How do I derive the ideal gas equation from kinetic theory?
    Start with pressure p = F/A, where force F = rate of change of momentum. For a molecule of mass m and speed c, momentum change per collision is 2mc. Number of collisions per second on a wall of area A is (N/3V) * A * c (assuming ⅓ of molecules move in each direction). This gives p = (1/3) * (N/V) * m * c². Using average speed squared (c²) and n = N/NA, and kinetic energy ½ m c² = (3/2)kT, you get pV = nRT.