The AOTF-based NO<sub>2</sub> camera
The abundance of NO<sub>2</sub> in the boundary layer relates to air quality and pollution source monitoring. Observing the spatiotemporal distribution of NO<sub>2</sub> above well-delimited (flue gas stacks, volcanoes, ships) or more extended sources (cities) allows for appl...
Main Authors: | , , , |
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Format: | Article |
Language: | English |
Published: |
Copernicus Publications
2016-12-01
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Series: | Atmospheric Measurement Techniques |
Online Access: | http://www.atmos-meas-tech.net/9/6025/2016/amt-9-6025-2016.pdf |
Summary: | The abundance of NO<sub>2</sub> in the boundary layer relates to air
quality and pollution source monitoring. Observing the spatiotemporal
distribution of NO<sub>2</sub> above well-delimited (flue gas stacks, volcanoes,
ships) or more extended sources (cities) allows for applications such as
monitoring emission fluxes or studying the plume dynamic chemistry and its
transport. So far, most attempts to map the NO<sub>2</sub> field from the ground
have been made with visible-light scanning grating spectrometers. Benefiting from a
high retrieval accuracy, they only achieve a relatively low spatiotemporal
resolution that hampers the detection of dynamic features.
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We present a new type of passive remote sensing instrument aiming at the
measurement of the 2-D distributions of NO<sub>2</sub> slant column densities
(SCDs) with a high spatiotemporal resolution. The measurement principle has
strong similarities with the popular filter-based SO<sub>2</sub> camera as it
relies on spectral images taken at wavelengths where the molecule absorption
cross section is different. Contrary to the SO<sub>2</sub> camera, the spectral
selection is performed by an acousto-optical tunable filter (AOTF) capable of
resolving the target molecule's spectral features.
<br><br>
The NO<sub>2</sub> camera capabilities are demonstrated by imaging the
NO<sub>2</sub> abundance in the plume of a coal-fired power plant. During this
experiment, the 2-D distribution of the NO<sub>2</sub> SCD was retrieved with a
temporal resolution of 3 min and a spatial sampling of 50 cm (over a
250 × 250 m<sup>2</sup> area). The detection limit was close to 5 × 10<sup>16</sup> molecules cm<sup>−2</sup>, with a maximum detected SCD of 4 × 10<sup>17</sup> molecules cm<sup>−2</sup>. Illustrating the added value of the NO<sub>2</sub>
camera measurements, the data reveal the dynamics of the NO to
NO<sub>2</sub> conversion in the early plume with an unprecedent resolution:
from its release in the air, and for 100 m upwards, the observed NO<sub>2</sub>
plume concentration increased at a rate of 0.75–1.25 g s<sup>−1</sup>. In joint
campaigns with SO<sub>2</sub> cameras, the NO<sub>2</sub> camera could also help in
removing the bias introduced by the NO<sub>2</sub> interference with the SO<sub>2</sub> spectrum. |
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ISSN: | 1867-1381 1867-8548 |