Inputs

Actual pressure at the location, not the altimeter setting.

%

Leave blank for dry air.

Results

Enter your values and select Calculate.

Educational use only. Results are not certified for operational flight planning or aircraft performance decisions. Always use approved aircraft documentation and official aviation information before flight.

How to use this calculator

  1. Enter Absolute pressure and choose hPa, inHg, kPa, psi or mmHg.
  2. Enter Air temperature in °C, °F or K.
  3. Optionally enter Relative humidity as a percentage from 0 to 100, or leave it blank for dry air.
  4. Read the density, the density ratio and the equivalent density altitude.

The pressure field needs the actual pressure of the air at the location, sometimes called station pressure. It is not the altimeter setting, which has been adjusted to sea level and at any elevated field is higher than the pressure really present. If the setting and elevation are all you have, the density altitude calculator is the right starting point. Humidity can only be included between −40 °C and 60 °C, the range in which the vapor-pressure formula is valid.

Formula

dry air: ρ = P ÷ (Rd × T)

humid air: ρ = (P − Pv) ÷ (Rd × T) + Pv ÷ (Rv × T)

Pv = RH × 610.94 × exp( 17.625 × t ÷ (t + 243.04) )

What the variables mean

ρ
air density in kg/m³
P
absolute (station) pressure in pascals
T, t
temperature in kelvin and in °C
Pv
partial pressure of water vapor
RH
relative humidity as a fraction
Rd, Rv
287.05287 and 461.495 J/(kg·K)

Worked example

These example values are illustrative round numbers, not data for any particular aircraft. Select "Fill in the example" in the calculator to load them.

Inputs

  • Absolute pressure: 1013.25 hPa (mbar)
  • Air temperature: 30 °C
  • Relative humidity: 60%

Working

  1. T = 303.15 K, P = 101,325 Pa.
  2. Saturation vapor pressure = 610.94 × exp(17.625 × 30.0 ÷ (30.0 + 243.04)) = 4,237 Pa.
  3. Pv = 60% of that = 2,542 Pa.
  4. ρ = (101,325 − 2,542) ÷ (287.05287 × 303.15) + 2,542 ÷ (461.495 × 303.15) = 1.1533 kg/m³.

Result

  • Air density: 1.1533 kg/m³ (0.002238 slug/ft³)
  • Density ratio (σ): 0.9415 (94.2% of sea-level standard)
  • Water-vapor pressure: 25.42 hPa (Dry-air density would be 1.1644 kg/m³)
  • Equivalent density altitude: 2,045 ft (623 m in the standard atmosphere)

Reading the result

Air density is given in kg/m³ with slug/ft³ beside it. Density ratio (σ) divides that by the sea-level standard value and repeats it as a percentage. Water-vapor pressure is the share of the total pressure exerted by water vapor; when humidity is entered, the density dry air would have under the same conditions is printed next to it so the humidity effect is visible. Equivalent density altitude is the height in the standard atmosphere that has the same density, in feet and meters. It reads “Outside the 20 km model” when the density falls beyond the range the atmosphere model covers.

Assumptions and limitations

  • Dry air and water vapor are each treated as ideal gases, with gas constants of 287.05287 and 461.495 J/(kg·K).
  • Saturation vapor pressure comes from a Magnus-type approximation over liquid water, which is why humidity is limited to −40 °C to 60 °C.
  • The pressure entered is taken to be the true absolute pressure at the point of interest; no conversion from an altimeter setting is made.
  • Composition is assumed to be standard air, with no allowance for dust, smoke, liquid droplets or ice crystals.
  • Temperature, pressure and humidity are single values for one point, not an average over a runway or a climb.
  • A humidity that would make the vapor pressure exceed the total pressure is rejected as physically impossible.

Common mistakes

  • Entering the altimeter setting in the Absolute pressure field at an airport well above sea level.
  • Expecting humid air to be denser than dry air, when water vapor is lighter than the air it displaces.
  • Using the temperature in °C or °F directly in the gas law when working by hand, instead of kelvin.
  • Overestimating the humidity effect, which is small beside the effect of temperature or pressure.
  • Entering the dew point where relative humidity is asked for.
  • Choosing kPa and typing a value in hPa, which is ten times too large and falls outside the accepted range.

References

  1. NASA Glenn Research Center, Earth Atmosphere Model.
  2. NOAA, NASA and the U.S. Air Force, U.S. Standard Atmosphere, 1976.
  3. Federal Aviation Administration, Pilot's Handbook of Aeronautical Knowledge (FAA-H-8083-25).

These public sources explain the formulas and definitions used here. Citing them does not mean they have reviewed, endorsed or certified AviationCalc.

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