Dry air at 20 °C and 1 atm has cp = 1006.1 J/(kg·K) (0.2403 Btu/(lb·°F)), cv = 717.67 J/(kg·K) and γ = 1.402. At 1000 °C and 1 atm, cp is 1184.7 J/(kg·K) and γ is 1.320. This page is for dry air.
cp is the heat needed to raise one kilogram of air by one kelvin at constant pressure. cv is the same at constant volume. Their ratio is γ:
γ = cp / cv
For an ideal gas, cp − cv = R = 287.05 J/(kg·K). The table shows that real air stays close to this at 1 atm. Use cp for heating air in a duct or heat exchanger (see LMTD calculator). Use γ for the speed of sound (see speed of sound of air), nozzle flow and compression work.
At 1 atm, cp changes by about 17 % from −100 to 1000 °C. Pressure matters more at high pressure and low temperature. At 100 bar and −100 °C, cp is 2358.6 J/(kg·K), against 1008.8 J/(kg·K) at 1 atm.
Accuracy. Lemmon et al. (2000) state an uncertainty of about 0.1 % in density, 0.2 % in speed of sound and 1 % in heat capacity from the solidification point to 873 K (600 °C) and up to 70 MPa. Above 873 K there were no reliable air data, so nitrogen data were used and the paper gives about 0.5 % for density. Lemmon & Jacobsen (2004) state about 5 % for the viscosity and thermal conductivity of air, and more near the critical point. Viscosity and conductivity above about 600 °C, and the 1000 °C end of the range, are less certain than that. CoolProp uses a molar mass of 28.96546 g/mol, the U.S. Standard Atmosphere uses 28.9644 g/mol. That is the main reason CoolProp density at 15 °C and 1 atm is 0.04 % above the Standard Atmosphere value.