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AEROSOL PROFILING DURING THE LARGE SCALE FIELD CAMPAIGN CINDI-2

Arnoud Apituley1,*, Michel Van Roozendael2, Andreas Richter3, Thomas Wagner4, Udo Friess5, Francois Hendrick2, Karin Kreher6, Jan-Lukas Tirpitz5and CINDI-2 Participants7

1Royal Netherlands Meteorological Institute (KNMI), The Netherlands,apituley@knmi.nl

2BIRA-IASB, Brussels, Belgium

3IUP-Bremen, Germany

4MPIC, Mainz, Germany

5IUP-Heidelberg, Germany

6Bodeker Scientific, Alexandra, New Zealand

7Various countries world-wide

ABSTRACT

For the validation of space borne observations of NO2 and other trace gases from hyperspec- tral imagers, ground based instruments based on the MAXDOAS technique are an excel- lent choice, since they rely on similar retrieval techniques as the observations from orbit. To ensure proper traceability of the MAXDOAS observations, a thorough validation and inter- comparison is mandatory. Advanced MAX- DOAS observation and retrieval techniques en- able inferring vertical structure of trace gases and aerosols. These techniques and their results need validation by e.g. lidar techniques.

For the proper understanding of the results from passive remote sensing techniques, independent observations are needed that include parameters needed to understand the light paths, i.e. in-situ aerosol observations of optical and microphysi- cal properties, and essential are in particular the vertical profiles of aerosol optical properties by (Raman) lidar.

The approach used in the CINDI-2 campaign held in Cabauw in 2016 is presented in this pa- per and the results will be discussed in the pre- sentation at the conference.

1 INTRODUCTION

Ground based and spaceborne hyperspectral in- struments for observations of NO2 and other

trace gases rely on similar retrieval techniques.

In both cases, retrievals take into account the light path of scattered sunlight though the entire atmosphere (see Fig.1). In case of high aerosol load close to the surface, this will dominate the light path and therefore bias the sensitivity of the measurement to this part of the atmosphere.

Since MAXDOAS instruments are relatively low cost and can be operated autonomously al- most anywhere, they are credible candidates to form a world-wide ground based reference network for satellite observations. To ensure proper traceability of the MAXDOAS observa- tions, a thorough intercomparison is mandatory.

With the imminent launch of Sentinel-5 Pre- cursor/TROPOMI (6), with a nadir pixelsize of 3.5 ×3.5 km2, and recent developments in MAXDOAS instruments there was a need for

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Figure 1: Schematic of light paths for MAXDOAS (left) and for lidar (right). Note that the effective

footprint of the passive MAXDOAS observation extends multiple kilometers (similar to satellite observations), while the lidar footprint is much

smaller.

EPJ Web of Conferences 176, 10005 (2018) https://doi.org/10.1051/epjconf/201817610005 ILRC 28

© The Authors, published by EDP Sciences. This is an open access article distributed under the terms of the Creative Commons Attribution License 4.0 (http://creativecommons.org/licenses/by/4.0/).

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MAXDOAS IN-SITU Raman

Lidar

LP-DOAS

NO2 lidar WindLidar

Figure 2: Aerial view of the CESAR site near Cabauw, showing the location of the main

instrumentation of the campaign.

CINDI-2. This campaign was completed in September 2016 and had the goals to: 1) Asess the consistency of slant column measurements of key target species (NO2, O3, O4and HCHO) relevant for the validation of S5P and the fu- ture ESA atmospheric Sentinels, from a large number of DOAS and MAXDOAS instruments from all over the world, and 2) study the re- lationship between remote-sensing column and profile measurements of those species and ref- erence measurements of the same species.

Figure 3: Picture of the CINDI-2 observation site.

The MAXDOAS instruments were placed on the roof of temporary containers situated at the Remote

Sensing Site of the CESAR Observatory where the Raman lidar and ceilometer are permanently

located.

2 CAMPAIGN DESIGN

A feature of recent MAXDOAS developments is the use azimuthal scanning, in addition to el- evation scanning such as in e.g. the PANDORA type of instruments (3). This, and the number of participating instruments, that expanded to 42, posed a challenge to the design of the CINDI-2 campaign.

The Cabauw Experimental Site for Atmo- spheric Research (CESAR) site in centre of The Netherlands (1) was the stage of the Cabauw Intercomparison of Nitrogen Dioxide Measur- ing Instruments (CINDI) in June-July 2009 (4) and again for the second campaign, CINDI-2, in 2016. Cabauw was chosen because the flat terrain offers a free view of large parts of the horizon, needed to accommodate the viewing geometry of the MAXDOAS observations. The location is under influence of both clean as well as polluted airmasses. This gives a wide range of possible trace gas concentrations and mix- tures.

Furthermore, at CESAR a wide range of obser- vations are routinely carried out that fulfil the requirement to provide the background neces- sary for unraveling the differences between the observations from different MAXDOAS instru- ments that can be quite diverse in design and data treatment. These observations include pa- rameters needed to understand the light paths, i.e. in-situ aerosol observations of optical and microphysical properties, as well as vertical profiles of aerosol optical properties by (Ra- man) lidar (2). In addition, vertical profiles of NO2 were provided by the unique NO2 sonde (5), and a NO2 lidar system (7). In situ ob- servations of aerosol scattering and absorbing properties, as well as microphysical properties were made in collaboration with the ACTRIS- 2 project. The placement of the instruments on the Cabauw site is schematically shown in Fig.2 and a picture of the remote sensing site is shown

2

EPJ Web of Conferences 176, 10005 (2018) https://doi.org/10.1051/epjconf/201817610005 ILRC 28

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MAXDOAS IN-SITU Raman

Lidar

LP-DOAS

NO2 lidar WindLidar

Figure 2: Aerial view of the CESAR site near Cabauw, showing the location of the main

instrumentation of the campaign.

CINDI-2. This campaign was completed in September 2016 and had the goals to: 1) Asess the consistency of slant column measurements of key target species (NO2, O3, O4and HCHO) relevant for the validation of S5P and the fu- ture ESA atmospheric Sentinels, from a large number of DOAS and MAXDOAS instruments from all over the world, and 2) study the re- lationship between remote-sensing column and profile measurements of those species and ref- erence measurements of the same species.

Figure 3: Picture of the CINDI-2 observation site.

The MAXDOAS instruments were placed on the roof of temporary containers situated at the Remote

Sensing Site of the CESAR Observatory where the Raman lidar and ceilometer are permanently

located.

2 CAMPAIGN DESIGN

A feature of recent MAXDOAS developments is the use azimuthal scanning, in addition to el- evation scanning such as in e.g. the PANDORA type of instruments (3). This, and the number of participating instruments, that expanded to 42, posed a challenge to the design of the CINDI-2 campaign.

The Cabauw Experimental Site for Atmo- spheric Research (CESAR) site in centre of The Netherlands (1) was the stage of the Cabauw Intercomparison of Nitrogen Dioxide Measur- ing Instruments (CINDI) in June-July 2009 (4) and again for the second campaign, CINDI-2, in 2016. Cabauw was chosen because the flat terrain offers a free view of large parts of the horizon, needed to accommodate the viewing geometry of the MAXDOAS observations. The location is under influence of both clean as well as polluted airmasses. This gives a wide range of possible trace gas concentrations and mix- tures.

Furthermore, at CESAR a wide range of obser- vations are routinely carried out that fulfil the requirement to provide the background neces- sary for unraveling the differences between the observations from different MAXDOAS instru- ments that can be quite diverse in design and data treatment. These observations include pa- rameters needed to understand the light paths, i.e. in-situ aerosol observations of optical and microphysical properties, as well as vertical profiles of aerosol optical properties by (Ra- man) lidar (2). In addition, vertical profiles of NO2 were provided by the unique NO2 sonde (5), and a NO2 lidar system (7). In situ ob- servations of aerosol scattering and absorbing properties, as well as microphysical properties were made in collaboration with the ACTRIS- 2 project. The placement of the instruments on the Cabauw site is schematically shown in Fig.2 and a picture of the remote sensing site is shown

Figure 4: General meteorological conditions during the campaign main intercomparison phase

between 12 and 28 Sept. 2016.

in Fig.3. Here, we focus on the aerosol profile.

The NO2profiles are discussed in a paper by S.

Berkhout at ILRC28.

3 FIRST RESULTS

Due to favourable weather conditions for mak- ing MAXDOAS and lidar observations, i.e. ab- sence of clouds as shown in Fig.4, a very inter- esting dataset has been collected, where most of the instruments were able to provide data.

An example of an aerosol profiling case is shown in Fig.5 and 6. Fig.5 shows the (prelim- inary) MAXDOAS aerosol extinction profiles retrieved for 477 nm. The extinction peaks be- tween 0.5 and 1.5 km above ground while some structure in the aerosol profile is present for the results from all groups below 1 km. The peak value of the extinction is about 0.3 km−1. Li- dar data for the same day are shown in Fig.6, where the top panel shows the 24-h aerosol pro- file from the Lufft CHM15k ceilometer and the bottom left in the figure shows the Raman lidar range corrected signal. The lower right shows the Raman lidar backscatter and extinction pro- files, as well as the lidar-ratio and Ångström co- efficient. From the lidar extinction profile at 355 nm it can be seen that extinction profile peaks at≈ 2.5 km at a value of ≈ 0.3 km−1. So, while the peak extinction values are very similar, the shape of the profile shows marked differences. The analysis of the CINDI-2 data is ongoing and the latest stage of development

will be shown at the conference.

Figure 5: Example of MAXDOAS aerosol profile retrieval at 477 nm for 15 Sept. 2016 around 9 UTC from various participating groups. Note that

these are preliminary results.

4 CONCLUSIONS

The CINDI-2 campaign conducted in Sept.

2016 in Cabauw was successful due to well functioning instruments and thanks to favourable weather conditions. A valuable dataset was collected. Preliminary data anal- ysis shows that the observations are suitable for study of the (aerosol) profile retrieval from MAXDOAS observations. The lidar measure- ments carried out the the facility are key data for the evaluation of the results.

ACKNOWLEDGEMENTS

The CINDI-2 campaign was supported by ESA, the Netherands Space Office (NSO) and ACTRIS-2 (H2020-INFRAIA 654109).

References

[1] A. Apituley, et al. Overview of research and networking with ground based remote sensing for atmospheric profiling at the cabauw exper- imental site for atmospheric research (cesar) – the netherlands. InProceedings IGARSS 2008,

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EPJ Web of Conferences 176, 10005 (2018) https://doi.org/10.1051/epjconf/201817610005 ILRC 28

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−2 0 2 4 6 Backscatter [10−6m−1Sr−1] 0

1 2 3 4 5

Altitude ASL [km]

355 nm 532 nm 1064 nm 355 nm 532 nm

−100 0 100 200 300 Extinction [10−6m−1] 0

1 2 3 4 5

0 50 100 150

Lidar Ratio [Sr]

0 1 2 3 4 5

−2 −1 0 1 2 3

Ångstrom Exponent 0

1 2 3 4 5

a

β, VIS−UV

a

β, IR−VIS

a

β, VIS−UV

Figure 6: Example of a diurnal CHM15k ceilometer observation for 15 Sept. 2016 (top) and a daytime multi-wavelength Raman lidar observation between 8-10 UTC (bottom). In the lower-right panel, the

retrieved backscatter and extinction profiles are shown. Note that these are daytime

measurements.Therefore, only the 355 nm Raman extinction profile is available. The lidar ratio above the aersol layer that extends to about 2.5 km appears as noise, since the extinction fluctuates around zero.

Boston, Massachusetts, volume III, pages 903–

906, 2008.

[2] A. Apituley, et al. Performance Assessment and Application of Caeli – A high-performance Ra- man lidar for diurnal profiling of Water Vapour, Aerosols and Clouds. In A. Apituley, H. Russ- chenberg, and W. Monna, editors,Proceedings of the 8th ISTP, pages S06–O10, 2009.

[3] J. Herman, et al. NO2 column amounts from ground-based Pandora and MFDOAS spec- trometers using the direct-sun DOAS technique:

Intercomparisons and application to OMI vali- dation. Journal of Geophysical Research: At- mospheres, 114(D13):n/a–n/a, 2009. D13307.

[4] A. J. M. Piters, et al. The Cabauw Intercom- parison campaign for Nitrogen Dioxide mea-

suring Instruments (CINDI): design, execution, and early results. Atm. Meas. Tech., 5(2):457–

485, 2012.

[5] W. W. Sluis, et al. The development of a nitro- gen dioxide sonde. Atmospheric Measurement Techniques, 3(6):1753–1762, 2010.

[6] J. Veefkind, et al. TROPOMI on the ESA Sentinel-5 Precursor: A GMES mission for global observations of the atmospheric compo- sition for climate, air quality and ozone layer applications. Remote Sensing of Environment, 120(0):70 – 83, 2012.

[7] H. Volten, et al. NO2 lidar profile measure- ments for satellite interpretation and validation.

J. Geophys. Res., 114, 12 2009.

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EPJ Web of Conferences 176, 10005 (2018) https://doi.org/10.1051/epjconf/201817610005 ILRC 28

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