Speed of sound in an ideal gas: c = √(γRT). Covers all common gases with presets for γ and R.
Compressible Flow · Fundamentalcp/cv — 1.4 for air, 1.667 for monatomic gases
R = Ru/M — 287.05 for air, 2077 for helium
T = 293.15 K
Speed of sound in an ideal gas:
Where:
Gas properties and speed of sound at 20°C (293.15 K):
| Gas | γ | R [J/(kg·K)] | c at 20°C [m/s] |
|---|---|---|---|
| Air (dry) | 1.400 | 287.05 | 343 |
| Nitrogen N₂ | 1.400 | 296.80 | 349 |
| Oxygen O₂ | 1.395 | 259.83 | 326 |
| Helium | 1.667 | 2077.1 | 1007 |
| Hydrogen H₂ | 1.405 | 4124.2 | 1270 |
| Argon | 1.667 | 208.13 | 323 |
| CO₂ | 1.289 | 188.92 | 267 |
| Methane CH₄ | 1.303 | 518.28 | 446 |
ISA standard atmosphere (air):
| Altitude [m] | T [K] | c [m/s] |
|---|---|---|
| 0 (sea level) | 288.15 | 340.3 |
| 1 000 | 281.65 | 336.4 |
| 5 000 | 255.65 | 320.5 |
| 10 000 | 223.25 | 299.5 |
| 20 000 | 216.65 | 295.1 |
The speed of sound increases with temperature because higher T means faster molecular motion. In the ISA atmosphere, c decreases with altitude as temperature drops (lapse rate −6.5 K/km in the troposphere).