CIOP   05384
CENTRO DE INVESTIGACIONES OPTICAS
Unidad Ejecutora - UE
artículos
Título:
Measurements of NO2 and O3 vertical column densities over ...
Autor/es:
MARCELO M. RAPONI; JIMENEZ R; WOLFRAM, E. A.; J. O. TOCHO; QUEL, E. J.
Revista:
optica pura y aplicada
Editorial:
SEDO
Referencias:
Año: 2012 vol. 45 p. 397 - 403
ISSN:
2171-8814
Resumen:
Stratospheric ozone (O3) plays a critical role in the atmosphere due to its capacity to absorb
biologically harmful solar UV radiation before it reaches the Earth¡¯s surface. Nitrogen dioxide (NO2)
is a key trace gas in the ozone photochemical. The remote sensing of NO2 and other atmospheric
minority gases is essential in order to understand the stratospheric O3 destruction and formation
processes. A study carried out on the seasonal variation of the O3 and NO2 vertical column densities
(VCDs) using a zenith©\sky DOAS (Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO23) plays a critical role in the atmosphere due to its capacity to absorb
biologically harmful solar UV radiation before it reaches the Earth¡¯s surface. Nitrogen dioxide (NO2)
is a key trace gas in the ozone photochemical. The remote sensing of NO2 and other atmospheric
minority gases is essential in order to understand the stratospheric O3 destruction and formation
processes. A study carried out on the seasonal variation of the O3 and NO2 vertical column densities
(VCDs) using a zenith©\sky DOAS (Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO22)
is a key trace gas in the ozone photochemical. The remote sensing of NO2 and other atmospheric
minority gases is essential in order to understand the stratospheric O3 destruction and formation
processes. A study carried out on the seasonal variation of the O3 and NO2 vertical column densities
(VCDs) using a zenith©\sky DOAS (Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO22 and other atmospheric
minority gases is essential in order to understand the stratospheric O3 destruction and formation
processes. A study carried out on the seasonal variation of the O3 and NO2 vertical column densities
(VCDs) using a zenith©\sky DOAS (Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO23 destruction and formation
processes. A study carried out on the seasonal variation of the O3 and NO2 vertical column densities
(VCDs) using a zenith©\sky DOAS (Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO23 and NO2 vertical column densities
(VCDs) using a zenith©\sky DOAS (Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO2Differential Optical Absorption Spectroscopy) is presented. This
system is composed of a spectral analyzer (portable mini©\spectrometer HR4000, Ocean Optics), two
optical fibers (400 ¦Ì of core, 25 cm and 6 m of longitude) and an automatic mechanical shutter. NO22
and O3 VCDs are derived from zenithal solar spectra acquired during twilights (zenithal angles
between 87¡ãand 91¡ã. The data retrieved by our instrument are compared with those coming from
the SAOZ spectrometer (Systeme d'Analyse par Observation Zenithale, Laboratoire Atmosph¨¨es,
Milieux, Observations Spatiales (LATMOS), France). Both systems are located in Rio Gallegos, Santa
Cruz province, Argentine (51¡ã6¡¯S; 69¡ã9¡¯W, 15 m asl), in the CEILAP©\RG remote sensing station. We
observed that NO2 VCD ranging from 6¡Á015 molec/cm2 in summer to 1.6¡Á015 molec/cm2 in winter
and early spring. An anticorrelation (shifting approximately 40 days) between NO2 and O3 VCDs was
calculated. A good agreement (average relative difference about 13%) among O3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.3 VCDs are derived from zenithal solar spectra acquired during twilights (zenithal angles
between 87¡ãand 91¡ã. The data retrieved by our instrument are compared with those coming from
the SAOZ spectrometer (Systeme d'Analyse par Observation Zenithale, Laboratoire Atmosph¨¨es,
Milieux, Observations Spatiales (LATMOS), France). Both systems are located in Rio Gallegos, Santa
Cruz province, Argentine (51¡ã6¡¯S; 69¡ã9¡¯W, 15 m asl), in the CEILAP©\RG remote sensing station. We
observed that NO2 VCD ranging from 6¡Á015 molec/cm2 in summer to 1.6¡Á015 molec/cm2 in winter
and early spring. An anticorrelation (shifting approximately 40 days) between NO2 and O3 VCDs was
calculated. A good agreement (average relative difference about 13%) among O3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.Systeme d'Analyse par Observation Zenithale, Laboratoire Atmosph¨¨es,
Milieux, Observations Spatiales (LATMOS), France). Both systems are located in Rio Gallegos, Santa
Cruz province, Argentine (51¡ã6¡¯S; 69¡ã9¡¯W, 15 m asl), in the CEILAP©\RG remote sensing station. We
observed that NO2 VCD ranging from 6¡Á015 molec/cm2 in summer to 1.6¡Á015 molec/cm2 in winter
and early spring. An anticorrelation (shifting approximately 40 days) between NO2 and O3 VCDs was
calculated. A good agreement (average relative difference about 13%) among O3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.S; 69¡ã9¡¯W, 15 m asl), in the CEILAP©\RG remote sensing station. We
observed that NO2 VCD ranging from 6¡Á015 molec/cm2 in summer to 1.6¡Á015 molec/cm2 in winter
and early spring. An anticorrelation (shifting approximately 40 days) between NO2 and O3 VCDs was
calculated. A good agreement (average relative difference about 13%) among O3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.2 VCD ranging from 6¡Á015 molec/cm2 in summer to 1.6¡Á015 molec/cm2 in winter
and early spring. An anticorrelation (shifting approximately 40 days) between NO2 and O3 VCDs was
calculated. A good agreement (average relative difference about 13%) among O3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.2 and O3 VCDs was
calculated. A good agreement (average relative difference about 13%) among O3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.3 VCD measurements
of both instruments was observed. In the case of NO2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.2, a better agreement among results at sunrise
than at sunset between SAOZ and ERO©\DOAS data was determined.