TY - JOUR
T1 - An intercomparison of total column-averaged nitrous oxide between ground-based FTIR TCCON and NDACC measurements at seven sites and comparisons with the GEOS-Chem model
AU - Zhou, Minqiang
AU - Langerock, Bavo
AU - Wells, Kelley C.
AU - Millet, Dylan B.
AU - Vigouroux, Corinne
AU - Sha, Mahesh Kumar
AU - Hermans, Christian
AU - Metzger, Jean Marc
AU - Kivi, Rigel
AU - Heikkinen, Pauli
AU - Smale, Dan
AU - Pollard, David F.
AU - Jones, Nicholas
AU - Deutscher, Nicholas M.
AU - Blumenstock, Thomas
AU - Schneider, Matthias
AU - Palm, Mathias
AU - Notholt, Justus
AU - Hannigan, James W.
AU - De Mazière, Martine
N1 - Publisher Copyright:
© Author(s) 2019.
PY - 2019
Y1 - 2019
N2 - Nitrous oxide (N 2 O) is an important greenhouse gas and it can also generate nitric oxide, which depletes ozone in the stratosphere. It is a common target species of ground-based Fourier transform infrared (FTIR) nearinfrared (TCCON) and mid-infrared (NDACC) measurements. Both TCCON and NDACC networks provide a longterm global distribution of atmospheric N 2 O mole fraction. In this study, the dry-air column-averaged mole fractions of N 2 O (XN 2 O) from the TCCON and NDACC measurements are compared against each other at seven sites around the world (Ny-Ålesund, Sodankylä, Bremen, Izaña, Réunion, Wollongong, Lauder) in the time period of 2007–2017. The mean differences in XN 2 O between TCCON and NDACC (NDACC–TCCON) at these sites are between -3:32 and 1.37 ppb (-1:1 %–0.5 %) with standard deviations between 1.69 and 5.01 ppb (0.5 %–1.6 %), which are within the uncertainties of the two datasets. The NDACC N 2 O retrieval has good sensitivity throughout the troposphere and stratosphere, while the TCCON retrieval underestimates a deviation from the a priori in the troposphere and overestimates it in the stratosphere. As a result, the TCCON XN 2 O measurement is strongly affected by its a priori profile. Trends and seasonal cycles of XN 2 O are derived from the TCCON and NDACC measurements and the nearby surface flask sample measurements and compared with the results from GEOS-Chem model a priori and a posteriori simulations. The trends and seasonal cycles from FTIR measurement at Ny-Ålesund and Sodankylä are strongly affected by the polar winter and the polar vortex. The a posteriori N 2 O fluxes in the model are optimized based on surface N 2 O measurements with a 4D-Var inversion method. The XN 2 O trends from the GEOS-Chem a posteriori simulation (0:97-0:02 (1) ppb yr-1) are close to those from the NDACC (0:93- 0:04 ppb yr-1) and the surface flask sample measurements (0:93-0:02 ppb yr-1). The XN 2 O trend from the TCCON measurements is slightly lower (0:81-0:04 ppb yr-1) due to the underestimation of the trend in TCCON a priori simulation. The XN 2 O trends from the GEOS-Chem a priori simulation are about 1.25 ppb yr-1, and our study confirms that the N 2 O fluxes from the a priori inventories are overestimated. The seasonal cycles of XN 2 O from the FTIR measurements and the model simulations are close to each other in the Northern Hemisphere with a maximum in August–October and a minimum in February–April. However, in the Southern Hemisphere, the modeled XN 2 O values show a minimum in February–April while the FTIR XN 2 O retrievals show different patterns. By comparing the partial column-averaged N 2 O from the model and NDACC for three vertical ranges (surface–8, 8–17, 17–50 km), we find that the discrepancy in the XN 2 O seasonal cycle between the model simulations and the FTIR measurements in the Southern Hemisphere is mainly due to their stratospheric differences.
AB - Nitrous oxide (N 2 O) is an important greenhouse gas and it can also generate nitric oxide, which depletes ozone in the stratosphere. It is a common target species of ground-based Fourier transform infrared (FTIR) nearinfrared (TCCON) and mid-infrared (NDACC) measurements. Both TCCON and NDACC networks provide a longterm global distribution of atmospheric N 2 O mole fraction. In this study, the dry-air column-averaged mole fractions of N 2 O (XN 2 O) from the TCCON and NDACC measurements are compared against each other at seven sites around the world (Ny-Ålesund, Sodankylä, Bremen, Izaña, Réunion, Wollongong, Lauder) in the time period of 2007–2017. The mean differences in XN 2 O between TCCON and NDACC (NDACC–TCCON) at these sites are between -3:32 and 1.37 ppb (-1:1 %–0.5 %) with standard deviations between 1.69 and 5.01 ppb (0.5 %–1.6 %), which are within the uncertainties of the two datasets. The NDACC N 2 O retrieval has good sensitivity throughout the troposphere and stratosphere, while the TCCON retrieval underestimates a deviation from the a priori in the troposphere and overestimates it in the stratosphere. As a result, the TCCON XN 2 O measurement is strongly affected by its a priori profile. Trends and seasonal cycles of XN 2 O are derived from the TCCON and NDACC measurements and the nearby surface flask sample measurements and compared with the results from GEOS-Chem model a priori and a posteriori simulations. The trends and seasonal cycles from FTIR measurement at Ny-Ålesund and Sodankylä are strongly affected by the polar winter and the polar vortex. The a posteriori N 2 O fluxes in the model are optimized based on surface N 2 O measurements with a 4D-Var inversion method. The XN 2 O trends from the GEOS-Chem a posteriori simulation (0:97-0:02 (1) ppb yr-1) are close to those from the NDACC (0:93- 0:04 ppb yr-1) and the surface flask sample measurements (0:93-0:02 ppb yr-1). The XN 2 O trend from the TCCON measurements is slightly lower (0:81-0:04 ppb yr-1) due to the underestimation of the trend in TCCON a priori simulation. The XN 2 O trends from the GEOS-Chem a priori simulation are about 1.25 ppb yr-1, and our study confirms that the N 2 O fluxes from the a priori inventories are overestimated. The seasonal cycles of XN 2 O from the FTIR measurements and the model simulations are close to each other in the Northern Hemisphere with a maximum in August–October and a minimum in February–April. However, in the Southern Hemisphere, the modeled XN 2 O values show a minimum in February–April while the FTIR XN 2 O retrievals show different patterns. By comparing the partial column-averaged N 2 O from the model and NDACC for three vertical ranges (surface–8, 8–17, 17–50 km), we find that the discrepancy in the XN 2 O seasonal cycle between the model simulations and the FTIR measurements in the Southern Hemisphere is mainly due to their stratospheric differences.
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U2 - 10.5194/amt-12-1393-2019
DO - 10.5194/amt-12-1393-2019
M3 - Article
AN - SCOPUS:85062538489
SN - 1867-1381
VL - 12
SP - 1393
EP - 1408
JO - Atmospheric Measurement Techniques
JF - Atmospheric Measurement Techniques
IS - 2
ER -