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Dive into the research topics where Theodore G. Shepherd is active.

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Featured researches published by Theodore G. Shepherd.


Journal of the Atmospheric Sciences | 1991

On the downward control of extratropical diabatic circulations by eddy-induced mean zonal forces

Peter H. Haynes; Michael E. McIntyre; Theodore G. Shepherd; C. J. Marks; Keith P. Shine

Abstract The situation considered is that of a zonally symmetric model of the middle atmosphere subject to a given quasi-steady zonal force F, conceived to be the result of irreversible angular momentum transfer due to the upward propagation and breaking of Rossby and gravity waves together with any other dissipative eddy effects that may be relevant. The models diabatic heating is assumed to have the qualitative character of a relaxation toward some radiatively determined temperature field. To the extent that the force F may be regarded as given, and the extratropical angular momentum distribution is realistic, the extratropical diabatic mass flow across a given isentropic surface may be regarded as controlled exclusively by the F distribution above that surface (implying control by the eddy dissipation above that surface and not, for instance, by the frequency of tropopause folding below). This “downward control” principle expresses a critical part of the dynamical chain of cause and effect governin...


Journal of Geophysical Research | 2006

Assessment of temperature, trace species, and ozone in chemistry-climate model simulations of the recent past

Veronika Eyring; Neal Butchart; Darryn W. Waugh; Hideharu Akiyoshi; John Austin; Slimane Bekki; G. E. Bodeker; B. A. Boville; C. Brühl; M. P. Chipperfield; Eugene C. Cordero; Martin Dameris; Makoto Deushi; Vitali E. Fioletov; S. M. Frith; Rolando R. Garcia; Andrew Gettelman; Marco A. Giorgetta; Volker Grewe; L. Jourdain; Douglas E. Kinnison; E. Mancini; Elisa Manzini; Marion Marchand; Daniel R. Marsh; Tatsuya Nagashima; Paul A. Newman; J. E. Nielsen; Steven Pawson; G. Pitari

Simulations of the stratosphere from thirteen coupled chemistry-climate models (CCMs) are evaluated to provide guidance for the interpretation of ozone predictions made by the same CCMs. The focus of the evaluation is on how well the fields and processes that are important for determining the ozone distribution are represented in the simulations of the recent past. The core period of the evaluation is from 1980 to 1999 but long-term trends are compared for an extended period (1960–2004). Comparisons of polar high-latitude temperatures show that most CCMs have only small biases in the Northern Hemisphere in winter and spring, but still have cold biases in the Southern Hemisphere spring below 10 hPa. Most CCMs display the correct stratospheric response of polar temperatures to wave forcing in the Northern, but not in the Southern Hemisphere. Global long-term stratospheric temperature trends are in reasonable agreement with satellite and radiosonde observations. Comparisons of simulations of methane, mean age of air, and propagation of the annual cycle in water vapor show a wide spread in the results, indicating differences in transport. However, for around half the models there is reasonable agreement with observations. In these models the mean age of air and the water vapor tape recorder signal are generally better than reported in previous model intercomparisons. Comparisons of the water vapor and inorganic chlorine (Cly) fields also show a large intermodel spread. Differences in tropical water vapor mixing ratios in the lower stratosphere are primarily related to biases in the simulated tropical tropopause temperatures and not transport. The spread in Cly, which is largest in the polar lower stratosphere, appears to be primarily related to transport differences. In general the amplitude and phase of the annual cycle in total ozone is well simulated apart from the southern high latitudes. Most CCMs show reasonable agreement with observed total ozone trends and variability on a global scale, but a greater spread in the ozone trends in polar regions in spring, especially in the Arctic. In conclusion, despite the wide range of skills in representing different processes assessed here, there is sufficient agreement between the majority of the CCMs and the observations that some confidence can be placed in their predictions.


Journal of Geophysical Research | 2007

Multimodel projections of stratospheric ozone in the 21st century

Veronika Eyring; Darryn W. Waugh; G. E. Bodeker; Eugene C. Cordero; Hideharu Akiyoshi; John Austin; S. R. Beagley; B. A. Boville; Peter Braesicke; C. Brühl; Neal Butchart; M. P. Chipperfield; Martin Dameris; Rudolf Deckert; Makoto Deushi; S. M. Frith; Rolando R. Garcia; Andrew Gettelman; Marco A. Giorgetta; Douglas E. Kinnison; E. Mancini; Elisa Manzini; Daniel R. Marsh; Sigrun Matthes; Tatsuya Nagashima; Paul A. Newman; J. E. Nielsen; S. Pawson; G. Pitari; David A. Plummer

[1] Simulations from eleven coupled chemistry-climate models (CCMs) employing nearly identical forcings have been used to project the evolution of stratospheric ozone throughout the 21st century. The model-to-model agreement in projected temperature trends is good, and all CCMs predict continued, global mean cooling of the stratosphere over the next 5 decades, increasing from around 0.25 K/decade at 50 hPa to around 1 K/ decade at 1 hPa under the Intergovernmental Panel on Climate Change (IPCC) Special Report on Emissions Scenarios (SRES) A1B scenario. In general, the simulated ozone evolution is mainly determined by decreases in halogen concentrations and continued cooling of the global stratosphere due to increases in greenhouse gases (GHGs). Column ozone is projected to increase as stratospheric halogen concentrations return to 1980s levels. Because of ozone increases in the middle and upper stratosphere due to GHGinduced cooling, total ozone averaged over midlatitudes, outside the polar regions, and globally, is projected to increase to 1980 values between 2035 and 2050 and before lowerstratospheric halogen amounts decrease to 1980 values. In the polar regions the CCMs simulate small temperature trends in the first and second half of the 21st century in midwinter. Differences in stratospheric inorganic chlorine (Cly) among the CCMs are key to diagnosing the intermodel differences in simulated ozone recovery, in particular in the Antarctic. It is found that there are substantial quantitative differences in the simulated Cly, with the October mean Antarctic Cly peak value varying from less than 2 ppb to over 3.5 ppb in the CCMs, and the date at which the Cly returns to 1980 values varying from before 2030 to after 2050. There is a similar variation in the timing of recovery of Antarctic springtime column ozone back to 1980 values. As most models underestimate peak Clynear 2000, ozone recovery in the Antarctic could occur even later, between 2060 and 2070. In the Arctic the column ozone increase in spring does not follow halogen decreases as closely as in the Antarctic, reaching 1980 values before Arctic halogen amounts decrease


Science | 2008

The Impact of Stratospheric Ozone Recovery on the Southern Hemisphere Westerly Jet

Seok-Woo Son; Lorenzo M. Polvani; Darryn W. Waugh; Hideharu Akiyoshi; Rolando R. Garcia; Douglas E. Kinnison; S. Pawson; E. Rozanov; Theodore G. Shepherd; Kiyotaka Shibata

In the past several decades, the tropospheric westerly winds in the Southern Hemisphere have been observed to accelerate on the poleward side of the surface wind maximum. This has been attributed to the combined anthropogenic effects of increasing greenhouse gases and decreasing stratospheric ozone and is predicted to continue by the Intergovernmental Panel on Climate Change/Fourth Assessment Report (IPCC/AR4) models. In this paper, the predictions of the Chemistry-Climate Model Validation (CCMVal) models are examined: Unlike the AR4 models, the CCMVal models have a fully interactive stratospheric chemistry. Owing to the expected disappearance of the ozone hole in the first half of the 21st century, the CCMVal models predict that the tropospheric westerlies in Southern Hemisphere summer will be decelerated, on the poleward side, in contrast with the prediction of most IPCC/AR4 models.


Journal of Geophysical Research | 2010

Impact of stratospheric ozone on Southern Hemisphere circulation change: A multimodel assessment

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 Climate | 2010

Chemistry-climate model simulations of twenty-first century stratospheric climate and circulation changes

Neal Butchart; Irene Cionni; Veronika Eyring; Theodore G. Shepherd; Darryn W. Waugh; Hideharu Akiyoshi; J. Austin; C. Brühl; M. P. Chipperfield; Eugene C. Cordero; Martin Dameris; Rudolf Deckert; S. Dhomse; S. M. Frith; Rolando R. Garcia; Andrew Gettelman; Marco A. Giorgetta; Douglas E. Kinnison; Feng Li; E. Mancini; Charles McLandress; Steven Pawson; G. Pitari; David A. Plummer; E. Rozanov; F. Sassi; J. F. Scinocca; K. Shibata; B. Steil; Wenshou Tian

The response of stratospheric climate and circulation to increasing amounts of greenhouse gases (GHGs) and ozone recovery in the twenty-first century is analyzed in simulations of 11 chemistry–climate models using near-identical forcings and experimental setup. In addition to an overall global cooling of the stratosphere in the simulations (0.59 6 0.07 K decade 21 at 10 hPa), ozone recovery causes a warming of the Southern Hemisphere polar lower stratosphere in summer with enhanced cooling above. The rate of warming correlates with the rate of ozone recovery projected by the models and, on average, changes from 0.8 to 0.48 K decade 21 at 100 hPa as the rate of recovery declines from the first to the second half of the century. In the winter northern polar lower stratosphere the increased radiative cooling from the growing abundance of GHGs is, in most models, balanced by adiabatic warming from stronger polar downwelling. In the Antarctic lower stratosphere the models simulate an increase in low temperature extremes required for polar stratospheric cloud (PSC) formation, but the positive trend is decreasing over the twenty-first century in all models. In the Arctic, none of the models simulates a statistically significant increase in Arctic PSCs throughout the twentyfirst century. The subtropical jets accelerate in response to climate change and the ozone recovery produces a westward acceleration of the lower-stratospheric wind over the Antarctic during summer, though this response is sensitive to the rate of recovery projected by the models. There is a strengthening of the Brewer–Dobson


Journal of the Atmospheric Sciences | 1983

Large-Scale Two-Dimensional Turbulence in the Atmosphere

G. J. Boer; Theodore G. Shepherd

Abstract Global FGGE data are used to investigate several aspects of large-scale turbulence in the atmosphere. The approach follows that for two-dimensional, nondivergent turbulent flows which are homogeneous and isotropic on the sphere. Spectra of kinetic energy, enstrophy and available potential energy are obtained for both the stationary and transient parts of the flow. Nonlinear interaction terms and fluxes of energy and enstrophy through wavenumber space are calculated and compared with the theory. A possible method of parameterizing the interactions with unresolved scales is considered. Two rather different flow regimes are found in wavenumber space. The high-wavenumber regime is dominated by the transient components of the flow and exhibits, at least approximately, several of the conditions characterizing homogeneous and isotropic turbulence. This region of wavenumber space also displays some of the features of an enstrophy-cascading inertial subrange. The low-wavenumber region, on the other hand, ...


Journal of Climate | 2009

Simulated Anthropogenic Changes in the Brewer–Dobson Circulation, Including Its Extension to High Latitudes

Charles McLandress; Theodore G. Shepherd

Recent studies using comprehensive middle atmosphere models predict a strengthening of the Brewer-Dobson circulation in response to climate change. To gain confidence in the realism of this result it is important to quantify and understand the contributions from the different components of stratospheric wave drag that cause this increase. Such an analysis is performed here using three 150-yr transient simulations from the Canadian Middle Atmosphere Model (CMAM), a Chemistry-Climate Model that simulates climate change and ozone depletion and recovery. Resolved wave drag and parameterized orographic gravity wave drag account for 60% and 40%, respectively, of the long-term trend in annual mean net upward mass flux at 70 hPa, with planetary waves accounting for 60% of the resolved wave drag trend. Synoptic wave drag has the strongest impact in northern winter, where it accounts for nearly as much of the upward mass flux trend as planetary wave drag. Owing to differences in the latitudinal structure of the wave drag changes, the relative contribution of resolved and parameterized wave drag to the tropical upward mass flux trend over any particular latitude range is highly sensitive to the range of latitudes considered. An examination of the spatial structure of the climate change response reveals no straightforward connection between the low-latitude and high-latitude changes: while the model results show an increase in Arctic downwelling in winter, they also show a decrease in Antarctic downwelling in spring. Both changes are attributed to changes in the flux of stationary planetary wave activity into the stratosphere.


Advances in Geophysics | 1990

Symmetries, Conservation Laws, and Hamiltonian Structure in Geophysical Fluid Dynamics

Theodore G. Shepherd

Publisher Summary This chapter discusses symmetries, conservation laws, and Hamiltonian structure in geophysical fluid dynamics. Some basic definitions and results for finite-dimensional Hamiltonian dynamical systems, leading up to the introduction of the symplectic notation that proves crucial in the generalization to noncanonical, infinite-dimensional systems, such as the Eulerian representation of fluid flow are presented. It is found that in addition to the invariants, such as energy and momentum that are associated with explicit symmetries, noncanonical Hamiltonian systems generally possess what are sometimes known as Casimir invariants or distinguished functions. The equations of fluid dynamics are continuous in space and thus represent infinite-dimensional dynamical systems. The existence of nonlinearly stable solutions whose stability relies on the full infinity of Casimir invariants strongly suggests a failure of ergodicity, because trajectories originating sufficiently close to those states cannot fill out the entire energy–enstrophy hypersurface. It is found that the physical approximations made to derive the shallow-water equations from 3D incompressible flow consist of taking the fluid to be homogeneous and constrained to move in vertical columns.


Journal of Climate | 2010

Separating the Dynamical Effects of Climate Change and Ozone Depletion. Part II: Southern Hemisphere Troposphere

Charles McLandress; Theodore G. Shepherd; J. F. Scinocca; David A. Plummer; Michael Sigmond; A. I. Jonsson; M. Catherine Reader

Abstract The separate effects of ozone depleting substances (ODSs) and greenhouse gases (GHGs) on forcing circulation changes in the Southern Hemisphere extratropical troposphere are investigated using a version of the Canadian Middle Atmosphere Model (CMAM) that is coupled to an ocean. Circulation-related diagnostics include zonal wind, tropopause pressure, Hadley cell width, jet location, annular mode index, precipitation, wave drag, and eddy fluxes of momentum and heat. As expected, the tropospheric response to the ODS forcing occurs primarily in austral summer, with past (1960–99) and future (2000–99) trends of opposite sign, while the GHG forcing produces more seasonally uniform trends with the same sign in the past and future. In summer the ODS forcing dominates past trends in all diagnostics, while the two forcings contribute nearly equally but oppositely to future trends. The ODS forcing produces a past surface temperature response consisting of cooling over eastern Antarctica, and is the dominant...

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Hideharu Akiyoshi

National Institute for Environmental Studies

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Andrew Gettelman

National Center for Atmospheric Research

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Slimane Bekki

Centre national de la recherche scientifique

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