Hella Garny
German Aerospace Center
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Hella Garny.
Journal of Geophysical Research | 2010
Seok-Woo Son; Edwin P. Gerber; Judith Perlwitz; Lorenzo M. Polvani; Nathan P. Gillett; Kyong-Hwan Seo; Veronika Eyring; Theodore G. Shepherd; Darryn W. Waugh; Hideharu Akiyoshi; J. Austin; A. J. G. Baumgaertner; Slimane Bekki; Peter Braesicke; C. Brühl; Neal Butchart; M. P. Chipperfield; David Cugnet; Martin Dameris; S. Dhomse; S. M. Frith; Hella Garny; Rolando R. Garcia; Steven C. Hardiman; Patrick Jöckel; Jean-Francois Lamarque; E. Mancini; Marion Marchand; M. Michou; Tetsu Nakamura
The impact of stratospheric ozone on the tropospheric general circulation of the Southern Hemisphere (SH) is examined with a set of chemistry-climate models participating in the Stratospheric Processes and their Role in Climate (SPARC)/Chemistry-Climate Model Validation project phase 2 (CCMVal-2). Model integrations of both the past and future climates reveal the crucial role of stratospheric ozone in driving SH circulation change: stronger ozone depletion in late spring generally leads to greater poleward displacement and intensification of the tropospheric midlatitude jet, and greater expansion of the SH Hadley cell in the summer. These circulation changes are systematic as poleward displacement of the jet is typically accompanied by intensification of the jet and expansion of the Hadley cell. Overall results are compared with coupled models participating in the Intergovernmental Panel on Climate Change Fourth Assessment Report (IPCC AR4), and possible mechanisms are discussed. While the tropospheric circulation response appears quasi-linearly related to stratospheric ozone changes, the quantitative response to a given forcing varies considerably from one model to another. This scatter partly results from differences in model climatology. It is shown that poleward intensification of the westerly jet is generally stronger in models whose climatological jet is biased toward lower latitudes. This result is discussed in the context of quasi-geostrophic zonal mean dynamics.
Journal of Geophysical Research | 2010
Andrew Gettelman; M. I. Hegglin; Say-Jin Son; Jung-Hyun Kim; Masatomo Fujiwara; Thomas Birner; Stefanie Kremser; Markus Rex; Juan A. Añel; Hideharu Akiyoshi; John Austin; Slimane Bekki; P. Braesike; C. Brühl; Neal Butchart; M. P. Chipperfield; Martin Dameris; S. Dhomse; Hella Garny; Steven C. Hardiman; Patrick Jöckel; Douglas E. Kinnison; Jean-Francois Lamarque; E. Mancini; Marion Marchand; M. Michou; Olaf Morgenstern; Steven Pawson; G. Pitari; David A. Plummer
The performance of 18 coupled Chemistry Climate Models (CCMs) in the Tropical Tropopause Layer (TTL) is evaluated using qualitative and quantitative diagnostics. Trends in tropopause quantities in the tropics and the extratropical Upper Troposphere and Lower Stratosphere (UTLS) are analyzed. A quantitative grading methodology for evaluating CCMs is extended to include variability and used to develop four different grades for tropical tropopause temperature and pressure, water vapor and ozone. Four of the 18 models and the multi‐model mean meet quantitative and qualitative standards for reproducing key processes in the TTL. Several diagnostics are performed on a subset of the models analyzing the Tropopause Inversion Layer (TIL), Lagrangian cold point and TTL transit time. Historical decreases in tropical tropopause pressure and decreases in water vapor are simulated, lending confidence to future projections. The models simulate continued decreases in tropopause pressure in the 21st century, along with ∼1K increases per century in cold point tropopause temperature and 0.5–1 ppmv per century increases in water vapor above the tropical tropopause. TTL water vapor increases below the cold point. In two models, these trends are associated with 35% increases in TTL cloud fraction. These changes indicate significant perturbations to TTL processes, specifically to deep convective heating and humidity transport. Ozone in the extratropical lowermost stratosphere has significant and hemispheric asymmetric trends. O3 is projected to increase by nearly 30% due to ozone recovery in the Southern Hemisphere (SH) and due to enhancements in the stratospheric circulation. These UTLS ozone trends may have significant effects in the TTL and the troposphere.
Journal of Geophysical Research | 2010
Olaf Morgenstern; Marco A. Giorgetta; Kiyotaka Shibata; Veronika Eyring; Darryn W. Waugh; Theodore G. Shepherd; Hideharu Akiyoshi; J. Austin; A. J. G. Baumgaertner; Slimane Bekki; Peter Braesicke; C. Brühl; M. P. Chipperfield; David Cugnet; Martin Dameris; S. Dhomse; S. M. Frith; Hella Garny; Andrew Gettelman; Steven C. Hardiman; M. I. Hegglin; Patrick Jöckel; Douglas E. Kinnison; Jean-Francois Lamarque; E. Mancini; Elisa Manzini; Marion Marchand; M. Michou; Tetsu Nakamura; J. E. Nielsen
The goal of the Chemistry-Climate Model Validation (CCMVal) activity is to improve understanding of chemistry-climate models (CCMs) through process-oriented evaluation and to provide reliable projections of stratospheric ozone and its impact on climate. An appreciation of the details of model formulations is essential for understanding how models respond to the changing external forcings of greenhouse gases and ozone-depleting substances, and hence for understanding the ozone and climate forecasts produced by the models participating in this activity. Here we introduce and review the models used for the second round (CCMVal-2) of this intercomparison, regarding the implementation of chemical, transport, radiative, and dynamical processes in these models. In particular, we review the advantages and problems associated with approaches used to model processes of relevance to stratospheric dynamics and chemistry. Furthermore, we state the definitions of the reference simulations performed, and describe the forcing data used in these simulations. We identify some developments in chemistry-climate modeling that make models more physically based or more comprehensive, including the introduction of an interactive ocean, online photolysis, troposphere-stratosphere chemistry, and non-orographic gravity-wave deposition as linked to tropospheric convection. The relatively new developments indicate that stratospheric CCM modeling is becoming more consistent with our physically based understanding of the atmosphere.
Journal of Geophysical Research | 2010
Edwin P. Gerber; Mark P. Baldwin; Hideharu Akiyoshi; John Austin; Slimane Bekki; Peter Braesicke; Neal Butchart; M. P. Chipperfield; Martin Dameris; S. Dhomse; S. M. Frith; Rolando R. Garcia; Hella Garny; Andrew Gettelman; Steven C. Hardiman; Alexey Yu. Karpechko; Marion Marchand; Olaf Morgenstern; J. Eric Nielsen; Steven Pawson; Tom Peter; David A. Plummer; J. A. Pyle; E. Rozanov; J. F. Scinocca; Theodore G. Shepherd; Dan Smale
The internal variability and coupling between the stratosphere and troposphere in CCMValA¢Â�Â�2 chemistryA¢Â�Â�climate models are evaluated through analysis of the annular mode patterns of variability. Computation of the annular modes in long data sets with secular trends requires refinement of the standard definition of the annular mode, and a more robust procedure that allows for slowly varying trends is established and verified. The spatial and temporal structure of the modelsA¢Â�Â� annular modes is then compared with that of reanalyses. As a whole, the models capture the key features of observed intraseasonal variability, including the sharp vertical gradients in structure between stratosphere and troposphere, the asymmetries in the seasonal cycle between the Northern and Southern hemispheres, and the coupling between the polar stratospheric vortices and tropospheric midlatitude jets. It is also found that the annular mode variability changes little in time throughout simulations of the 21st century. There are, however, both common biases and significant differences in performance in the models. In the troposphere, the annular mode in models is generally too persistent, particularly in the Southern Hemisphere summer, a bias similar to that found in CMIP3 coupled climate models. In the stratosphere, the periods of peak variance and coupling with the troposphere are delayed by about a month in both hemispheres. The relationship between increased variability of the stratosphere and increased persistence in the troposphere suggests that some tropospheric biases may be related to stratospheric biases and that a wellA¢Â�Â�simulated stratosphere can improve simulation of tropospheric intraseasonal variability.
Journal of the Atmospheric Sciences | 2011
Hella Garny; Martin Dameris; William J. Randel; Greg Bodeker; Rudolf Deckert
Drivers of upwelling in the tropical lower stratosphere are investigated using the E39C-A chemistry‐ climate model. The climatological annual cycle in upwelling and its wave forcing are compared to the interim ECMWF Re-Analysis (ERA-Interim). The strength in tropical upwelling and its annual cycle can be largely explainedby local resolvedwave forcing. The climatological meanforcing is due to both stationaryplanetaryscale waves that originate in the tropics and extratropical transient synoptic-scale waves that are refracted equatorward. Increases in atmospheric greenhouse gas (GHG) concentrations to 2050 force a year-round positive trend in tropical upwelling, which maximizes in the lowermost stratosphere. Tropical ascent is balanced by downwelling between 208 and 408. Strengthening of tropical upwelling can be explained by stronger local forcing by resolved wave flux convergence, which is driven in turn by processes initiated by increases in tropical sea surface temperatures (SSTs). Higher tropical SSTs cause a strengthening of the subtropical jets and modification of deep convection affecting latent heat release. While the former can modify wave propagation and dissipation, the latter affects tropical wave generation. The dominant mechanism leading to enhanced vertical wave propagation into the lower stratosphere is an upward shift of the easterly shear zone due to the strengthening and upward shift of the subtropical jets.
Journal of Geophysical Research | 2010
John Austin; J. F. Scinocca; David A. Plummer; Luke D. Oman; Darryn W. Waugh; Hideharu Akiyoshi; Slimane Bekki; Peter Braesicke; Neal Butchart; M. P. Chipperfield; David Cugnet; Martin Dameris; S. Dhomse; Veronika Eyring; S. M. Frith; Rolando R. Garcia; Hella Garny; Andrew Gettelman; Steven C. Hardiman; Douglas E. Kinnison; Jean-Francois Lamarque; E. Mancini; Marion Marchand; M. Michou; Olaf Morgenstern; Tetsu Nakamura; Steven Pawson; G. Pitari; J. A. Pyle; E. Rozanov
Simulations of 15 coupled chemistry climate models, for the period 1960–2100, are presented. The models include a detailed stratosphere, as well as including a realistic representation of the tropospheric climate. The simulations assume a consistent set of changing greenhouse gas concentrations, as well as temporally varying chlorofluorocarbon concentrations in accordance with observations for the past and expectations for the future. The ozone results are analyzed using a nonparametric additive statistical model. Comparisons are made with observations for the recent past, and the recovery of ozone, indicated by a return to 1960 and 1980 values, is investigated as a function of latitude. Although chlorine amounts are simulated to return to 1980 values by about 2050, with only weak latitudinal variations, column ozone amounts recover at different rates due to the influence of greenhouse gas changes. In the tropics, simulated peak ozone amounts occur by about 2050 and thereafter total ozone column declines. Consequently, simulated ozone does not recover to values which existed prior to the early 1980s. The results also show a distinct hemispheric asymmetry, with recovery to 1980 values in the Northern Hemisphere extratropics ahead of the chlorine return by about 20 years. In the Southern Hemisphere midlatitudes, ozone is simulated to return to 1980 levels only 10 years ahead of chlorine. In the Antarctic, annually averaged ozone recovers at about the same rate as chlorine in high latitudes and hence does not return to 1960s values until the last decade of the simulations.
Journal of Geophysical Research | 2010
M. I. Hegglin; Andrew Gettelman; P. Hoor; R. Krichevsky; G. L. Manney; Laura L. Pan; Say-Jin Son; G. P. Stiller; Simone Tilmes; Kaley A. Walker; Veronika Eyring; Theodore G. Shepherd; Darryn W. Waugh; Hideharu Akiyoshi; Juan A. Añel; J. Austin; A. J. G. Baumgaertner; Slimane Bekki; Peter Braesicke; C. Brühl; Neal Butchart; M. P. Chipperfield; Martin Dameris; S. Dhomse; S. M. Frith; Hella Garny; Steven C. Hardiman; Patrick Jöckel; Douglas E. Kinnison; Jean-Francois Lamarque
A multimodel assessment of the performance of chemistry-climate models (CCMs) in the extratropical upper troposphere/lower stratosphere (UTLS) is conducted for the first time. Process-oriented diagnostics are used to validate dynamical and transport characteristics of 18 CCMs using meteorological analyses and aircraft and satellite observations. The main dynamical and chemical climatological characteristics of the extratropical UTLS are generally well represented by the models, despite the limited horizontal and vertical resolution. The seasonal cycle of lowermost stratospheric mass is realistic, however with a wide spread in its mean value. A tropopause inversion layer is present in most models, although the maximum in static stability is located too high above the tropopause and is somewhat too weak, as expected from limited model resolution. Similar comments apply to the extratropical tropopause transition layer. The seasonality in lower stratospheric chemical tracers is consistent with the seasonality in the Brewer-Dobson circulation. Both vertical and meridional tracer gradients are of similar strength to those found in observations. Models that perform less well tend to use a semi-Lagrangian transport scheme and/or have a very low resolution. Two models, and the multimodel mean, score consistently well on all diagnostics, while seven other models score well on all diagnostics except the seasonal cycle of water vapor. Only four of the models are consistently below average. The lack of tropospheric chemistry in most models limits their evaluation in the upper troposphere. Finally, the UTLS is relatively sparsely sampled by observations, limiting our ability to quantitatively evaluate many aspects of model performance.
Journal of Geophysical Research | 2010
John Austin; Hamish Struthers; J. F. Scinocca; David A. Plummer; Hideharu Akiyoshi; A. J. G. Baumgaertner; Slimane Bekki; G. E. Bodeker; Peter Braesicke; C. Brühl; Neal Butchart; M. P. Chipperfield; David Cugnet; Martin Dameris; S. Dhomse; S. M. Frith; Hella Garny; Andrew Gettelman; Steven C. Hardiman; Patrick Jöckel; Douglas E. Kinnison; Anne Kubin; Jean-Francois Lamarque; Ulrike Langematz; E. Mancini; Marion Marchand; M. Michou; Olaf Morgenstern; Tetsu Nakamura; J. E. Nielsen
Coupled chemistry-climate model simulations covering the recent past and continuing throughout the 21st century have been completed with a range of different models. Common forcings are used for the halogen amounts and greenhouse gas concentrations, as expected under the Montreal Protocol (with amendments) and Intergovernmental Panel on Climate Change A1b Scenario. The simulations of the Antarctic ozone hole are compared using commonly used diagnostics: the minimum ozone, the maximum area of ozone below 220 DU, and the ozone mass deficit below 220 DU. Despite the fact that the processes responsible for ozone depletion are reasonably well understood, a wide range of results is obtained. Comparisons with observations indicate that one of the reasons for the model underprediction in ozone hole area is the tendency for models to underpredict, by up to 35%, the area of low temperatures responsible for polar stratospheric cloud formation. Models also typically have species gradients that are too weak at the edge of the polar vortex, suggesting that there is too much mixing of air across the vortex edge. Other models show a high bias in total column ozone which restricts the size of the ozone hole (defined by a 220 DU threshold). The results of those models which agree best with observations are examined in more detail. For several models the ozone hole does not disappear this century but a small ozone hole of up to three million square kilometers continues to occur in most springs even after 2070.
International Journal of Remote Sensing | 2009
Diego Loyola; R. M. Coldewey-Egbers; Martin Dameris; Hella Garny; Andrea Stenke; M. Van Roozendael; Christophe Lerot; Dimitris Balis; M. E. Koukouli
Although the Montreal Protocol now controls the production and emission of ozone depleting substances, the timing of ozone recovery is unclear. There are many other factors affecting the ozone layer, in particular climate change is expected to modify the speed of re-creation of the ozone layer. Therefore, long-term observations are needed to monitor the further evolution of the stratospheric ozone layer. Measurements from satellite instruments provide global coverage and are supplementary to selective ground-based observations. The combination of data derived from different space-borne instruments is needed to produce homogeneous and consistent long-term data records. They are required for robust investigations including trend analysis. For the first time global total ozone columns from three European satellite sensors GOME (ERS-2), SCIAMACHY (ENVISAT), and GOME-2 (METOP-A) are combined and added up to a continuous time series starting in June 1995. On the one hand it is important to monitor the consequences of the Montreal Protocol and its amendments; on the other hand multi-year observations provide the basis for the evaluation of numerical models describing atmospheric processes, which are also used for prognostic studies to assess the future development. This paper gives some examples of how to use satellite data products to evaluate model results with respective data derived from observations, and to disclose the abilities and deficiencies of atmospheric models. In particular, multi-year mean values derived from the Chemistry-Climate Model E39C-A are used to check climatological values and the respective standard deviations.
Journal of Geophysical Research | 2014
Hella Garny; Thomas Birner; Harald Bönisch; Felix Bunzel
Mean age of air (AoA) measures the mean transit time of air parcels along the Brewer-Dobson circulation (BDC) starting from their entry into the stratosphere. AoA is determined both by transport along the residual circulation and by two-way mass exchange (mixing). The relative roles of residual circulation transport and two-way mixing for AoA, and for projected AoA changes are not well understood. Here effects of mixing on AoA are quantified by contrasting AoA with the transit time of hypothetical transport solely by the residual circulation. Based on climate model simulations, we find additional aging by mixing throughout most of the lower stratosphere, except in the extratropical lowermost stratosphere where mixing reduces AoA. We use a simple Lagrangian model to reconstruct the distribution of AoA in the GCM and to illustrate the effects of mixing at different locations in the stratosphere. Predicted future reduction in AoA associated with an intensified BDC is equally due to faster transport along the residual circulation as well as reduced aging by mixing. A tropical leaky pipe model is used to derive a mixing efficiency, measured by the ratio of the two-way mixing mass flux and the net (residual) mass flux across the subtropical boundary. The mixing efficiency remains close to constant in a future climate, suggesting that the strength of two-way mixing is tightly coupled to the strength of the residual circulation in the lower stratosphere. This implies that mixing generally amplifies changes in AoA due to uniform changes in the residual circulation.