Remote Sensing of the Earth From Space: Atmospheric Correction 1992
DOI: 10.1007/978-3-642-76747-0_4
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Theoretical Models of the Non-Polarized Optical Radiation in the Atmosphere-Surface System

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Cited by 5 publications
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“…In fact, atmospheric water vapor is known to be the most dominant greenhouse gas in the Earth's atmosphere [Marsden and Valero, 2004], exerting a strong influence on the radiation balance of the surface-atmosphere system, due to its intense absorption of short-wave (solar) and long-wave (terrestrial) radiation [Yamanouchi and Charlok, 1995]. The former process is caused by the numerous absorption bands distributed throughout the 0.6 Ä 3.7 mm wavelength range of the solar spectrum [Kondratyev, 1969;Leckner, 1978], whereas the latter takes place substantially through two distinct absorption mechanisms: (1) selective absorption, mainly produced by the vibrorotational band centered at 6.25 mm wavelength and the rotational bands beyond 16 mm [Goody, 1964], and (2) continuum absorption, induced by both foreign and self-broadening mechanisms of the lines belonging to the absorption bands of water vapor and its dimer molecules in the middle and far infrared [Bignell, 1970;Clough et al, 1989].…”
Section: Introductionmentioning
confidence: 99%
“…In fact, atmospheric water vapor is known to be the most dominant greenhouse gas in the Earth's atmosphere [Marsden and Valero, 2004], exerting a strong influence on the radiation balance of the surface-atmosphere system, due to its intense absorption of short-wave (solar) and long-wave (terrestrial) radiation [Yamanouchi and Charlok, 1995]. The former process is caused by the numerous absorption bands distributed throughout the 0.6 Ä 3.7 mm wavelength range of the solar spectrum [Kondratyev, 1969;Leckner, 1978], whereas the latter takes place substantially through two distinct absorption mechanisms: (1) selective absorption, mainly produced by the vibrorotational band centered at 6.25 mm wavelength and the rotational bands beyond 16 mm [Goody, 1964], and (2) continuum absorption, induced by both foreign and self-broadening mechanisms of the lines belonging to the absorption bands of water vapor and its dimer molecules in the middle and far infrared [Bignell, 1970;Clough et al, 1989].…”
Section: Introductionmentioning
confidence: 99%
“…The relationship of the angle of incidence for a surface inclined and oriented in any direction with the local meridian is trigonometric (see Berod and Bock [44], Kondratyev [45], and Coffari [46]) and can be described with Equations ( 17) or (18). cos θ = (sen φ cos β − cos φsen β cos γ)sen δ +(cos φ cos β + senφsen β cos γ) cos δ cos ω + cos δsenβsen γ sen ω…”
Section: − Modeling the Angle Of Incidence For An Inclined Solar Pane...mentioning
confidence: 99%
“…As such, parametric models for estimating longwave irradiance during clear‐sky conditions (henceforth LW 0↓ ) often rely on screen‐level measurements of temperature and humidity (Flerchinger et al., 2009). Under cloudy or “all‐sky” (AS) conditions, however, cloud water droplets and ice crystals represent additional emitters that complicate LW ↓ estimation and typically serve to increase LW ↓ over LW 0↓ (Arking, 1991; Kondratyev, 1969; Yamanouchi & Kawaguchi, 1984). Various models have been proposed to correct for this increase by incorporating cloud covered area fraction ( f c ) or cloudiness proxies based on the clearness index (i.e., SW ↓ /SW ↓,TOA ) or fractional clear‐sky solar irradiance (i.e., SW ↓ /SW 0,↓ ; see the review by Flerchinger et al.…”
Section: Introductionmentioning
confidence: 99%