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Standard Atmosphere & Density Altitude

ISA / U.S. Standard Atmosphere 1976 temperature, pressure, density, speed of sound and viscosity from −5 to 80 km, plus pressure and density altitude.

Layer
Other height
Temperature
Pressure
Density
Speed of sound
Dynamic viscosity
Kinematic viscosity
Gravity
Ratios to sea level

U.S. Standard Atmosphere 1976 / ICAO, computed in your browser. For planning only; use your aircraft's official performance data.

How to use

  1. Pick Standard atmosphere to look up a height, or Density altitude for an airfield.
  2. For a height, enter it in metres, feet or kilometres and say whether it is geometric or geopotential.
  3. For density altitude, enter the field elevation, the altimeter setting, the temperature and optionally the dew point; click a result to copy it.

About this tool

Show

Two calculators built on the same model. The first gives the properties of the International Standard Atmosphere, identical to the U.S. Standard Atmosphere 1976 from −5 km to 80 km: temperature, pressure, density, speed of sound, dynamic and kinematic viscosity, gravity, and the temperature, pressure and density ratios θ, δ and σ used in aircraft performance work, for either a geometric height or a geopotential one, with the other shown alongside. The second is the pilot's density altitude check: from the field elevation, the altimeter setting (QNH), the outside air temperature and optionally the dew point, it gives the station pressure, the pressure altitude, the deviation from ISA and the density altitude, the height in the standard atmosphere where the air is as thin as it is on the runway now. Humidity is included through the vapour pressure, because moist air is lighter than dry air: a humid 32 °C day at Denver reads a couple of hundred feet higher than a dry one. The values match the ambiance library, itself checked against the 1976 tables, to within a few parts per million. What the model cannot tell you: the real atmosphere on a given day departs from ISA by tens of degrees, so the first calculator describes an average, not today's sky; and above 80 km the gas composition changes, which is why the tool stops there. Density altitude here comes from physics, not the 120-feet-per-degree rule of thumb, so it can differ from a quick E6B estimate by a few hundred feet.

Frequently asked questions

What is the difference between geometric and geopotential height?

Geometric height is distance above sea level. Geopotential height scales it by the weakening of gravity with height, so that the equations of the standard atmosphere stay simple. They differ by 19 m at 11 km and about 1 km at 80 km.

Why does density altitude matter?

Engines, propellers and wings all perform according to air density. A high density altitude means a longer take-off run and a weaker climb, even at a low airport on a hot day.

Why does humidity raise density altitude?

Water vapour is lighter than the nitrogen and oxygen it displaces, so humid air at the same pressure and temperature is less dense. The effect is small in cold air and grows quickly with temperature.

Why does the tool stop at 80 km?

Above about 80 km the mean molecular weight of air starts to change and the 1976 model switches to a different formulation. Up to 80 km the ICAO and U.S. 1976 atmospheres agree exactly.

Is this the same as the rule of thumb of 120 ft per degree?

No. The rule approximates density altitude as pressure altitude plus 120 ft for every degree above ISA. This tool solves the standard atmosphere for the actual density, which is more accurate, especially far from standard conditions.

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