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The atomic hydrogen distribution at 250 km during December 1974 solstice has been inferred, considering charge exchange equilibrium, from Atmosphere Explorer‐C measurements of n (H + ), n (O + ), and n (O). An empirical model, derived from the observations by least square analysis in terms of spherical harmonics, has the following characteristics: (a) n (H) increases by as much as a factor of two between the summer and winter hemispheres, (b) the n (H) diurnal variation is largest at the equator where n max/ n min = 3.2, the maximum occurring at 03 h LT, and (c) the diurnal variation is larger in the winter hemisphere ( n max/ n min = 2.6 at +40°) than in the summer ( n max/ n min = 2.3 at −40°). Similar analysis of the gas temperature derived from n (N 2 ) measurements reveals that all n (H) and T g spherical harmonic coefficients are anticorrelated. Both the diurnal and latitudinal (annual) n (H) and T g amplitudes are in substantial agreement with the “zero flux condition,” in which exospheric flow dominates the hydrogen distribution. The observed diurnal phase lag of n (H) with respect to T g is about one hour, agreeing with theory. During the period of measurement the observed mean global values of T g and n (H) were 800K and 3.6 × 10 5 cm −3 , respectively, the latter exceeding the Kockarts‐Nicolet model concentration by a factor of two.
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Brinton et al. (1975) studied this question.
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