📘 Heat: Thermodynamics
Intermediate study of heat, energy transfer, and thermodynamic laws
What you’ll learn
- Heat, Temperature, and Thermal EquilibriumDistinguish heat from temperature and apply the zeroth law to systems in thermal contact.Heat is energy transferred due to temperature difference, not a stored fluid. The zeroth law establishes transitive thermal equilibrium and defines temperature empirically. These foundations allow consistent measurement scales and prepare for the first law.
- The First Law and Internal EnergyState and apply the first law to closed systems with both heat and work exchanges.Internal energy is a state function fixed by the current state variables. Any process changes U only by the net energy crossing the boundary. Sign conventions for Q and W are fixed so that cyclic processes yield zero net change in U.
- Work in Thermodynamic ProcessesCalculate expansion work for reversible and irreversible paths on a P-V diagram.Work is path-dependent and equals the integral of P dV. Reversible paths yield the maximum work for expansion and minimum work for compression. Graphical representation on indicator diagrams connects abstract integrals to measurable quantities.
- Heat Capacity and EnthalpyRelate Cp and Cv through the first law and derive enthalpy for ideal gases.Enthalpy H = U + PV accounts for flow work in open systems. For ideal gases, both U and H depend only on temperature, so ΔH = nCpΔT. Experimental values of Cp and Cv reveal molecular degrees of freedom.
- Phase Changes and Latent HeatApply latent-heat data to calculate energy requirements during isothermal phase transitions.Latent heat reflects the potential-energy change associated with breaking intermolecular bonds. On a P-V or T-S diagram the process appears as a horizontal line at constant pressure or temperature. Steam tables and property charts supply the numerical values used in engineering calculations.
- The Second Law and EntropyDefine entropy as a state function and calculate ΔS for reversible and irreversible processes.Entropy increases quantify irreversibility and lost work potential. For reversible heat transfer, ΔS = ∫ dQrev/T. Irreversible processes generate entropy inside the system boundary, driving the universe toward thermodynamic equilibrium.
- Heat Engines and Thermal EfficiencyApply the first and second laws to calculate thermal efficiency of heat engines.Efficiency η = Wnet/Qh = 1 – |Qc|/Qh. The second law requires |Qc| > 0 for any finite-temperature engine. Real plants fall short of ideal limits because of irreversibilities such as friction and finite temperature differences.
- The Carnot CycleAnalyze the Carnot cycle on T-S and P-V diagrams and prove its maximum efficiency.All reversible engines operating between the same temperatures achieve the same efficiency. The T-S diagram shows that the enclosed area equals net work while the ratio of heat transfers fixes η. Any irreversibility reduces the enclosed area and therefore efficiency.
- Refrigerators and Heat PumpsDerive coefficients of performance for refrigeration and heat-pump cycles.COPR = Qc/Wnet and COPHP = Qh/Wnet. Both exceed unity because the device moves existing thermal energy rather than creating it. The reversed Carnot cycle sets the theoretical upper bound on these coefficients.
- Kinetic Theory of HeatConnect molecular kinetic energy to temperature and derive pressure from momentum transfer.Pressure arises from the rate of molecular collisions with container walls. Equipartition assigns 1/2 kT per quadratic degree of freedom, yielding Cv = 3/2 R for monatomic gases. This statistical foundation explains why temperature measures average kinetic energy.
- Irreversibility and Entropy GenerationCalculate entropy generation for mixing, throttling, and heat-transfer processes.Entropy generation is always positive inside real boundaries. Mixing, unrestrained expansion, and finite ΔT heat transfer are classic sources. Quantifying σgen identifies the largest irreversibilities for engineering improvement.
- Applications and Measurement StandardsLink thermodynamic theory to calibrated instruments and property databases used in engineering practice.Standard reference data allow engineers to predict performance before building devices. Real-time sensors and property tables convert the abstract laws into quantitative design tools. The course therefore ends by returning heat and temperature to measurable laboratory quantities.
Questions this course answers
Two objects are each in thermal equilibrium with a third object. What can be concluded?
The zeroth law states that thermal equilibrium is transitive, so if both objects share equilibrium with the third they share it with each other and no heat flows between them.
A student claims that heat is a fluid stored inside hot objects. Using the copper-aluminum block example, explain in one sentence why this view fails.
Heat is the energy crossing the boundary because of a temperature difference; once transfer stops, the objects retain different amounts of energy per degree of temperature change, so heat cannot be a stored fluid.
A closed system receives 1200 J of heat while the surroundings do 450 J of work on the system. What is ΔU?
Work done on the system is negative in the chosen convention, so ΔU = Q − (−450 J) = 1650 J.
In Joule’s original units, how many joules of work are required to raise the temperature of 1 g of water by 1 °C?
Joule measured 4.184 J per gram per degree Celsius, establishing the mechanical equivalent of heat.
An ideal gas expands from 2 L to 6 L. Which path produces the largest work output?
The reversible isothermal path follows the highest possible pressure at every volume and therefore encloses the largest area under the P-V curve.
Place the steps in the correct order to calculate work for a constant-external-pressure expansion.
Work equals the product of the actual opposing pressure and the observed volume change; the sign follows the convention that expansion work done by the system is negative.
Grounded in trusted sources
- National Institute of Standards and Technology
- U.S. Department of Energy
- NASA
- OpenStax University Physics, Heat and Heat Transfer Methods, https://openstax.org/books/university-physics-volume-2/pages/1-introduction
- PhET, Energy Forms and Changes, https://phet.colorado.edu/
- Khan Academy, Specific heat and calorimetry, https://www.khanacademy.org/science/physics
- NASA, Heat transfer education resources, https://www.nasa.gov/
Every Wunder lesson is built from real, reputable sources — never invented.
Related courses
Wunder is a personalized learn-anything platform — tell it any topic and it builds a beautiful, fact-checked course in minutes, with narration, a knowledge check, and a college-style University track.
© 2026 Wunder Learning LLC · Terms & Privacy