| Thermodynamic system | Any defined quantity of matter under study, separated from the surroundings by a boundary. |
| Surroundings | Everything outside the thermodynamic system. |
| Thermal equilibrium | Two bodies are in thermal equilibrium if no heat flows between them when placed in contact. |
| Zeroth Law | If A is in thermal equilibrium with B, and B with C, then A is in thermal equilibrium with C. Defines temperature. |
| First Law | Q = ΔU + W. Energy conservation applied to thermodynamic systems. |
| Internal energy (U) | Total microscopic energy of all molecules — kinetic and potential. For ideal gas: U = (f/2)nRT. |
| Work (W) | W = ∫P dV. Area under PV curve. Positive when gas expands. |
| Heat (Q) | Energy transferred between system and surroundings due to a temperature difference. |
| Isothermal | Process at constant temperature. ΔU = 0 for ideal gas. |
| Adiabatic | Process with no heat exchange (Q = 0). |
| Isochoric | Process at constant volume. W = 0. |
| Isobaric | Process at constant pressure. W = PΔV. |
| Carnot engine | Theoretical engine of maximum efficiency operating between T1 and T2 via two isothermal and two adiabatic steps. |
| Carnot efficiency | η = 1 − T2/T1. The upper limit for any heat engine. |
| COP | Coefficient of Performance. Figure of merit for refrigerators. COP = Q2/W. |
| Second Law | No cyclic engine converts all heat to work (Kelvin-Planck); heat does not spontaneously flow cold → hot (Clausius). |
| Entropy | Measure of disorder (microscopic randomness) of a system. Increases in any spontaneous irreversible process. |
| Degrees of freedom (f) | Number of independent ways a molecule can store energy. Monoatomic: 3, Diatomic: 5, Polyatomic: 6. |
| Equipartition theorem | Energy per degree of freedom = ½k_BT per molecule = ½RT per mole at thermal equilibrium. |
| v_rms | Root mean square speed: √(3RT/M). Used in pressure equation P = ½ρv_rms2. |
| v_avg | Mean (average) molecular speed: √(8RT/πM). |
| v_mp | Most probable speed: √(2RT/M). Speed at the peak of the Maxwell distribution. |
| Mayer's relation | Cₚ − Cᵥ = R. Difference in specific heats equals the gas constant for any ideal gas. |
| Boltzmann constant | k_B = 1.38×10−23 J/K. Relates microscopic energy to temperature. |