Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient

The interaction of NO<sub>2</sub> with TiO<sub>2</sub> solid films was studied under UV irradiation using a low pressure flow reactor (1–10 Torr) combined with a modulated molecular beam mass spectrometer for monitoring of the gaseous species involved. The NO<sub>2</...

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Main Authors: Y. Bedjanian, A. El Zein
Format: Article
Language:English
Published: Copernicus Publications 2012-01-01
Series:Atmospheric Chemistry and Physics
Online Access:http://www.atmos-chem-phys.net/12/1013/2012/acp-12-1013-2012.pdf
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spelling doaj-29c01d60199e481bbd961166eaf60c322020-11-24T22:46:02ZengCopernicus PublicationsAtmospheric Chemistry and Physics1680-73161680-73242012-01-011221013102010.5194/acp-12-1013-2012Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficientY. BedjanianA. El ZeinThe interaction of NO<sub>2</sub> with TiO<sub>2</sub> solid films was studied under UV irradiation using a low pressure flow reactor (1–10 Torr) combined with a modulated molecular beam mass spectrometer for monitoring of the gaseous species involved. The NO<sub>2</sub> to TiO<sub>2</sub> reactive uptake coefficient was measured from the kinetics of NO<sub>2</sub> loss on TiO<sub>2</sub> coated Pyrex rods as a function of NO<sub>2</sub> concentration, irradiance intensity (<i>J</i><sub>NO<sub>2</sub></sub> = 0.002–0.012 s<sup>−1</sup>), relative humidity (RH = 0.06–69 %), temperature (<i>T</i> = 275–320 K) and partial pressure of oxygen (0.001–3 Torr). TiO<sub>2</sub> surface deactivation upon exposure to NO<sub>2</sub> was observed. The initial uptake coefficient of NO<sub>2</sub> on illuminated TiO<sub>2</sub> surface (with 90 ppb of NO<sub>2</sub> and <i>J</i><sub>NO<sub>2</sub></sub>&cong;0.006 s<sup>−1</sup>) was found to be &gamma;<sub>0</sub> = (1.2±0.4) &times;10<sup>&minus;4</sup> (calculated using BET surface area) under dry conditions at <i>T</i> = 300 K. The steady state uptake, &gamma;, was several tens of times lower than the initial one, independent of relative humidity, and was found to decrease in the presence of molecular oxygen. In addition, it was shown that γ is not linearly dependent on the photon flux and seems to level off under atmospheric conditions. Finally, the following expression for γ was derived, γ = 2.3×10<sup>−3</sup> exp(&minus;1910/<i>T</i>)/(1 + <i>P</i><sup>0.36</sup>) (where <i>P</i> is O<sub>2</sub> pressure in Torr), and recommended for atmospheric applications (for any RH, near 90 ppb of NO<sub>2</sub> and <i>J</i><sub>NO<sub>2</sub></sub> = 0.006 s<sup>−1</sup>).http://www.atmos-chem-phys.net/12/1013/2012/acp-12-1013-2012.pdf
collection DOAJ
language English
format Article
sources DOAJ
author Y. Bedjanian
A. El Zein
spellingShingle Y. Bedjanian
A. El Zein
Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient
Atmospheric Chemistry and Physics
author_facet Y. Bedjanian
A. El Zein
author_sort Y. Bedjanian
title Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient
title_short Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient
title_full Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient
title_fullStr Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient
title_full_unstemmed Interaction of NO<sub>2</sub> with TiO<sub>2</sub> surface under UV irradiation: measurements of the uptake coefficient
title_sort interaction of no<sub>2</sub> with tio<sub>2</sub> surface under uv irradiation: measurements of the uptake coefficient
publisher Copernicus Publications
series Atmospheric Chemistry and Physics
issn 1680-7316
1680-7324
publishDate 2012-01-01
description The interaction of NO<sub>2</sub> with TiO<sub>2</sub> solid films was studied under UV irradiation using a low pressure flow reactor (1–10 Torr) combined with a modulated molecular beam mass spectrometer for monitoring of the gaseous species involved. The NO<sub>2</sub> to TiO<sub>2</sub> reactive uptake coefficient was measured from the kinetics of NO<sub>2</sub> loss on TiO<sub>2</sub> coated Pyrex rods as a function of NO<sub>2</sub> concentration, irradiance intensity (<i>J</i><sub>NO<sub>2</sub></sub> = 0.002–0.012 s<sup>−1</sup>), relative humidity (RH = 0.06–69 %), temperature (<i>T</i> = 275–320 K) and partial pressure of oxygen (0.001–3 Torr). TiO<sub>2</sub> surface deactivation upon exposure to NO<sub>2</sub> was observed. The initial uptake coefficient of NO<sub>2</sub> on illuminated TiO<sub>2</sub> surface (with 90 ppb of NO<sub>2</sub> and <i>J</i><sub>NO<sub>2</sub></sub>&cong;0.006 s<sup>−1</sup>) was found to be &gamma;<sub>0</sub> = (1.2±0.4) &times;10<sup>&minus;4</sup> (calculated using BET surface area) under dry conditions at <i>T</i> = 300 K. The steady state uptake, &gamma;, was several tens of times lower than the initial one, independent of relative humidity, and was found to decrease in the presence of molecular oxygen. In addition, it was shown that γ is not linearly dependent on the photon flux and seems to level off under atmospheric conditions. Finally, the following expression for γ was derived, γ = 2.3×10<sup>−3</sup> exp(&minus;1910/<i>T</i>)/(1 + <i>P</i><sup>0.36</sup>) (where <i>P</i> is O<sub>2</sub> pressure in Torr), and recommended for atmospheric applications (for any RH, near 90 ppb of NO<sub>2</sub> and <i>J</i><sub>NO<sub>2</sub></sub> = 0.006 s<sup>−1</sup>).
url http://www.atmos-chem-phys.net/12/1013/2012/acp-12-1013-2012.pdf
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