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    Standard Atmosphere

    The earth's atmosphere is a dynamically changing system

    The pressure and temperature of the atmosphere depend on altitude, location onthe globe (longitude and latitude), time of day, season, and even solar sunspotactivity. To take all these variations into account when considering the design andperformance of flight vehicles is impractical.

    A standard atmosphere is defined in order to relate flight tests, wind tunnelresults, and general airplane design and performance to a common reference . Itgives mean values of pressure, temperature, density, and other properties asfunctions of altitude; these values are obtained from experimental balloon andsounding-rocket measurements combined with a mathematical model of the

    Principles of Flight (MEC 2710) 1

    atmosphere.

    The tables in Apps. A (SI units) and B (English units) at the end of the book.

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    Geometric altitudegeometric height above sea level.

    Absolute altitude ha. If r is theradius of the earth, thenha = h G + r.

    From Newton's law of gravitation,

    Principles of Flight (MEC 2710) 3

    Hydrostatic Equation

    Now assume that (where h is the geopotential altitude)

    divide

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    Geopotential Altitude

    There is little difference between h and h G for low altitudes. For such a case, h G r, r/ (r + hG) ~ 1; hence h ~ h G .

    Earth radius r = 6.356766 x 10 6 m (at a latitude of 45), for hG = 7 km

    Principles of Flight (MEC 2710)

    h = 6.9923 km 0.001 error

    Only at altitudes above 65 km (213,000 ft) does the difference exceed 1 percent.

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    DEFINITION OF THE STANDARD ATMOSPHERE

    The keystone of the standardatmosphere is a defined variation of Twith altitude, based on experimentalevidence.

    cons s s o a ser es o s ra g nes,some vertical (called the constant-temperature, or isothermal regions )and others inclined (called the gradientregions ).

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    PRESSURE, TEMPERATURE, AND DENSITY ALTITUDES

    start at sea level (h = 0)

    PRESSURE, TEMPERATURE, AND DENSITY ALTITUDESSuppose you are flying at actual pressure 6.16 x 10 4 Pa, and actual T= 265.4 K

    If actual (measured) pressure = 6.16 x 10 4 Pa App. A hG = 4 km pressure altitude of 4 km.

    for actual measured tem erature = 265.4 K A . A h = 3.5 km

    Principles of Flight (MEC 2710)

    temperature altitude of 3.5 km.

    Thus you are simultaneously flying at a pressure altitude of 4 km and a temperaturealtitude of 3.5 km while your actual geometric altitude is yet a different value. Thedefinition of density altitude is made in the same way.

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    Chap 2 : 1 5* 11 14 Chap 3 : 1 2 4* 9 12

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