Adiabatic Process Temperature Calculator
Calculate temperature rise during adiabatic compression or expansion of ideal gases.
Adiabatic Compression Raises Ideal-Gas Temperature
In an adiabatic process, no heat crosses the system boundary, so compression work increases internal energy and temperature for an ideal gas. For a reversible adiabatic ideal-gas process with constant heat capacities, TVγ−1=constant and T2/T1=(P2/P1)(γ−1)/γ. Expansion reverses the trend and lowers temperature.
Adiabatic does not automatically mean isentropic. A reversible adiabatic process is isentropic, but real adiabatic compression can generate entropy through friction, shocks, or other irreversibilities and may reach a different final state.
| Symbol | Meaning | Why it appears / units |
|---|---|---|
| T | Absolute temperature | K. |
| P | Absolute pressure | Pa, kPa, or bar consistently. |
| V | Gas volume | Any consistent volume unit in a ratio. |
| γ | Heat-capacity ratio cp/cv | Dimensionless; about 1.4 for air near ordinary conditions. |
Compression ratios can produce substantial temperature increases, which is central to diesel engines, compressors, and atmospheric processes. Use absolute temperatures and absolute pressures, not gauge values, in thermodynamic ratios.
Check the pressure ratio before evaluating the exponent. For compression, P2/P1 should exceed 1 and the ideal-gas temperature should rise; for expansion the trend reverses. Kelvin is mandatory, while the pressure units may be any consistent pair because only their ratio enters.
Worked Examples
Common Mistakes
Thermodynamic power-law relations require absolute Kelvin temperatures.
Pressure ratios must use absolute pressure because zero gauge is not zero thermodynamic pressure.
Irreversible adiabatic processes generate entropy; isentropic requires both adiabatic and reversible behavior.
Frequently Asked Questions
Formula Explorer connections
Interpretation: This formula tracks heat, temperature, work, entropy or transport in a thermodynamic system. Assumption: Use absolute temperature where required and consistent energy units. Constant properties, equilibrium, ideal gases or negligible losses may be assumed.