Airglow as an Indicator of Upper Atmospheric Structure and by Vladislav Yu Khomich PDF

By Vladislav Yu Khomich

ISBN-10: 3642095003

ISBN-13: 9783642095009

The ebook summarizes overseas development during the last few many years in top surroundings airglow study. dimension tools, theoretical techniques and empirical types of a large spectrum of higher atmospheric emissions and their variability are thought of. The e-book incorporates a designated bibliography of reviews concerning the higher surroundings airglow and many helpful info on emission features and its formation procedures. The booklet is of curiosity to scientists operating within the box of aeronomy, physics of the higher surroundings of the Earth in addition to the opposite planets, and in addition for specialists drawn to utilized features of the Earth's top atmospheric emissions.

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Extra resources for Airglow as an Indicator of Upper Atmospheric Structure and Dynamics

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The ratio of the illuminated portion of the disk to its total area is k = cos2 Φ . 2 The relation between the Moon brightness and k is nonlinear. It has been tabulated by Kulikovsky (2002), and its approximation is presented by Hapke (1963, 1971). 2 Extra-Atmospheric Radiation 21 Fig. 12 Brightness of the Moon as a function of the phase angle. 7853) for a decreasing Moon, where tL is expressed in days. 0 · 10−3 (erg · cm−2 · s−1 · nm−1 ). 86 22 1 The Radiating Atmosphere and Space – – The albedo of the Moon in the ultraviolet spectral region is given by Flynn et al.

If the observation is performed at the Earth surface in the direction with zenith angle ζ, the line of sight intersects the emission layer at an altitude Z and has at the intersection point a zenith angle ζZ , which is determined by the relation (Fig. 20) sin ζZ = RE sin ζ . RE + Z The distance L between two points with coordinates ϕ1 , λ1 and ϕ2 , λ2 on the Earth surface (Fig. 21) is determined by the formula L = RE · ψ, where the angle ψ of the great circle arc is calculated by the formula cos ψ = sin ϕ1 · sin ϕ2 + cosϕ1 · cosϕ2 · cos(λ1 − λ2 ) .

1981; Kononovich and Moroz 2001; Kulikovsky 2002). 4·(m1−m2 ) . I1 To denote the brightness of a star, a special notation is commonly used. 3m and 0m , respectively. 78m. 4(10−m) . deg). 4·(10−m) . 786) . 4·m (erg · cm−2 · s−1 · nm−1 ) . These relations remain almost unchanged as the spectral type (class) of stars is changed from B to M. 4·m (photon · cm−2 · s−1 · nm−1 ) . 4·m (lx) . 84 · 10−6 (sb) . According to the data of Roach and Gordon (1973), we have 1 S10 / ◦ ˚ . 4 · 10−3 (Rayleigh/A) The definition of the Rayleigh photometric unit is given in Sect.

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Airglow as an Indicator of Upper Atmospheric Structure and Dynamics by Vladislav Yu Khomich

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