% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Hoffmann:834516,
author = {Hoffmann, Lars and Hertzog, Albert and Rössler, Thomas and
Stein, Olaf and Wu, Xue},
title = {{I}ntercomparison of meteorological analyses and
trajectories in the {A}ntarctic lower stratosphere with
{C}oncordiasi superpressure balloon observations},
journal = {Atmospheric chemistry and physics},
volume = {17},
number = {13},
issn = {1680-7324},
address = {Katlenburg-Lindau},
publisher = {EGU},
reportid = {FZJ-2017-04447},
pages = {8045 - 8061},
year = {2017},
abstract = {In this study we compared temperatures and horizontal winds
of meteorological analyses in the Antarctic lower
stratosphere, a region of the atmosphere that is of major
interest regarding chemistry and dynamics of the polar
vortex. The study covers the European Centre for
Medium-Range Weather Forecasts (ECMWF) operational analysis,
the ERA-Interim reanalysis, the Modern-Era Retrospective
analysis for Research and Applications version 1 and 2
(MERRA and MERRA-2), and the National Centers for
Environmental Prediction and National Center for Atmospheric
Research (NCEP/NCAR) reanalysis. The comparison was
performed with respect to long-duration observations from 19
superpressure balloon flights during the Concordiasi field
campaign in September 2010 to January 2011. Most of the
balloon measurements were conducted at altitudes of
17–18.5 km and latitudes of 60–85° S. We found that
large-scale state temperatures of the analyses have a mean
precision of 0.5–1.4 K and a warm bias of 0.4–2.1 K
with respect to the balloon data. Zonal and meridional winds
have a mean precision of 0.9–2.3 m s−1 and a bias
below ±0.5 m s−1. Standard deviations related to
small-scale fluctuations due to gravity waves are reproduced
at levels of $15–60 \%$ for temperature and
$30–60 \%$ for the horizontal winds. Considering the
fact that the balloon observations have been assimilated
into all analyses, except for NCEP/NCAR, notable differences
found here indicate that other observations, the forecast
models, and the data assimilation procedures have a
significant impact on the analyses as well. We also used the
balloon observations to evaluate trajectory calculations
with our new Lagrangian transport model Massive-Parallel
Trajectory Calculations (MPTRAC), where vertical motions of
simulated trajectories were nudged to pressure measurements
of the balloons. We found relative horizontal transport
deviations of $4–12 \%$ and error growth rates of
60–170 km day−1 for 15-day trajectories. Dispersion
simulations revealed some difficulties with the
representation of subgrid-scale wind fluctuations in MPTRAC,
as the spread of air parcels simulated with different
analyses was not consistent. However, although case studies
suggest that the accuracy of trajectory calculations is
influenced by meteorological complexity, diffusion generally
does not contribute significantly to transport deviations in
our analysis. Overall, evaluation results are satisfactory
and compare well to earlier studies using superpressure
balloon observations.},
cin = {JSC},
ddc = {550},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {511 - Computational Science and Mathematical Methods
(POF3-511)},
pid = {G:(DE-HGF)POF3-511},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000404773700002},
doi = {10.5194/acp-17-8045-2017},
url = {https://juser.fz-juelich.de/record/834516},
}