Comparison of a graph of International Standard Atmosphere temperature and pressure and approximate altitudes of various objects and successful stratospheric jumps
Air density must be calculated in order to solve for the pressure, and is used in calculating dynamic pressure for moving vehicles. Dynamic viscosity is an empirical function of temperature, and kinematic viscosity is calculated by dividing dynamic viscosity by the density.
Thus the standard consists of a tabulation of values at various altitudes, plus some formulas by which those values were derived. To accommodate the lowest points on Earth, the model starts at a base geopotential altitude of 610 meters (2,000ft)below sea level, with standard temperature set at 19°C. With a temperature lapse rate of −6.5°C (-11.7°F) per km (roughly −2°C (-3.6°F) per 1,000ft), the table interpolates to the standard mean sea level values of 15°C (59°F) temperature, 101,325 pascals (14.6959psi) (1 atm) pressure, and a density of 1.2250 kilograms per cubic meter (0.07647lb/cuft). The tropospheric tabulation continues to 11,000 meters (36,089ft), where the temperature has fallen to −56.5°C (−69.7°F), the pressure to 22,632 pascals (3.2825psi), and the density to 0.3639 kilograms per cubic meter (0.02272lb/cuft). Between 11km and 20km, the temperature remains constant.[3][4]
alapse rate given per kilometer of geopotential altitude (A positive lapse rate (λ > 0) means temperature decreases with height)
In the above table, geopotential altitude is calculated from a mathematical model that adjusts the altitude to include the variation of gravity with height, while geometric altitude is the standard direct vertical distance above mean sea level (MSL).[2]
The equation that relates the two altitudes are (where z is the geometric altitude, h is the geopotential altitude, and r0 = 6,356,766 m in this model):
Note that the Lapse Rates cited in the table are given as °C per kilometer of geopotential altitude, not geometric altitude.
The ISA model is based on average conditions at mid latitudes, as determined by the ISO's TC 20/SC 6 technical committee. It has been revised from time to time since the middle of the 20th century.
Use at non-standard day conditions
The ISA models a hypothetical standard day to allow a reproducible engineering reference for calculation and testing of engine and vehicle performance at various altitudes. It does not provide a rigorous meteorological model of actual atmospheric conditions (for example, changes in barometric pressure due to wind conditions). Neither does it account for humidity effects; air is assumed to be dry and clean and of constant composition. Humidity effects are accounted for in vehicle or engine analysis by adding water vapor to the thermodynamic state of the air after obtaining the pressure and density from the standard atmosphere model.
Non-standard (hot or cold) days are modeled by adding a specified temperature delta to the standard temperature at altitude, but pressure is taken as the standard day value. Density and viscosity are recalculated at the resultant temperature and pressure using the ideal gas equation of state. Hot day, Cold day, Tropical, and Polar temperature profiles with altitude have been defined for use as performance references, such as United States Department of Defense MIL-STD-210C, and its successor MIL-HDBK-310.[6]
ICAO Standard Atmosphere
The International Civil Aviation Organization (ICAO) published their "ICAO Standard Atmosphere" as Doc 7488-CD in 1993. It has the same model as the ISA, but extends the altitude coverage to 80 kilometers (262,500 feet).[7]
The ICAO Standard Atmosphere, like the ISA, does not contain water vapor.
Some of the values defined by ICAO are:
ICAO Standard Atmosphere
Height km & ft
Temperature °C
Pressure hPa
Lapse rate °C/1000ft
Lapse rate C/1000m
0km MSL
15.0
1013.25
+1.98 (tropospheric)
+6.5 (tropospheric)
11km 36 000ft
−56.5
226.00
0.00 (stratospheric)
0.00 (stratospheric)
20km 65 000ft
−56.5
54.70
-0.3 (stratospheric)
-0.1 (stratospheric)
32km 105 000ft
−44.5
8.68
Aviation standards and flying rules are based on the International Standard Atmosphere. Airspeed indicators are calibrated on the assumption that they are operating at sea level in the International Standard Atmosphere where the air density is 1.225kg/m3.
Physical properties of the ICAO Standard Atmosphere are:[8]
Physical properties of the ICAO Standard Atmosphere
The U.S. Standard Atmosphere is a set of models that define values for atmospheric temperature, density, pressure and other properties over a wide range of altitudes. The first model, based on an existing international standard, was published in 1958 by the U.S. Committee on Extension to the Standard Atmosphere,[9] and was updated in 1962,[5] 1966,[10] and 1976.[11] The U.S. Standard Atmosphere, International Standard Atmosphere and WMO (World Meteorological Organization) standard atmospheres are the same as the ISO International Standard Atmosphere for altitudes up to 32km.[12][13]
NRLMSISE-00 is a newer model of the Earth's atmosphere from ground to space, developed by the US Naval Research Laboratory taking actual satellite drag data into account. A primary use of this model is to aid predictions of satellite orbital decay due to atmospheric drag. The COSPAR International Reference Atmosphere (CIRA) 2012 and the ISO 14222 Earth Atmosphere Density standard both recommend NRLMSISE-00 for composition uses.
↑Tomasi, C.; Vitake, V.; De Santis, L.V. (1998). "Relative optical mass functions for air, water vapour, ozone and nitrogen dioxide in atmospheric models presenting different latitudinal and seasonal conditions". Meteorology and Atmospheric Physics. 65 (1): 11–30. Bibcode:1998MAP....65...11T. doi:10.1007/BF01030266. S2CID123129752. ...the ISO (International Organisation for Standardisation) Standard Atmosphere, 1972. This model is identical to the present Standard Atmospheres of ICAO (International Civil Aviation Organization) and WMO (World Meteorological Organization) up to a height of 32 km