S. R. Beagley
York University
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Featured researches published by S. R. Beagley.
Journal of Geophysical Research | 2007
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
Journal of Geophysical Research | 1997
Daniel J. Jacob; Michael J. Prather; Philip J. Rasch; Run-Lie Shia; Yves Balkanski; S. R. Beagley; D. Bergmann; W. T. Blackshear; Margaret Brown; Masaru Chiba; M. P. Chipperfield; J. de Grandpré; Jane Dignon; Johann Feichter; Christophe Genthon; William L. Grose; Prasad S. Kasibhatla; Ines Köhler; Mark A. Kritz; Kathy S. Law; Joyce E. Penner; Michel Ramonet; C. E. Reeves; Douglas A. Rotman; Deianeira Z. Stockwell; Peter F. J. van Velthoven; Gé Verver; Oliver Wild; Hu Yang; Peter H. Zimmermann
Simulations of 222Rn and other short-lived tracers are used to evaluate and intercompare the representations of convective and synoptic processes in 20 global atmospheric transport models. Results show that most established three-dimensional models simulate vertical mixing in the troposphere to within the constraints offered by the observed mean 222Rn concentrations and that subgrid parameterization of convection is essential for this purpose. However, none of the models captures the observed variability of 222Rn concentrations in the upper troposphere, and none reproduces the high 222Rn concentrations measured at 200 hPa over Hawaii. The established three-dimensional models reproduce the frequency and magnitude of high-222Rn episodes observed at Crozet Island in the Indian Ocean, demonstrating that they can resolve the synoptic-scale transport of continental plumes with no significant numerical diffusion. Large differences between models are found in the rates of meridional transport in the upper troposphere (interhemispheric exchange, exchange between tropics and high latitudes). The four two-dimensional models which participated in the intercomparison tend to underestimate the rate of vertical transport from the lower to the upper troposphere but show concentrations of 222Rn in the lower troposphere that are comparable to the zonal mean values in the three-dimensional models.
Atmosphere-ocean | 1997
S. R. Beagley; J. de Grandpré; John N. Koshyk; Norman McFarlane; Theodore G. Shepherd
Abstract The Canadian Middle Atmosphere Modelling (MAM) project is a collaboration between the Atmospheric Environment Service (AES) of Environment Canada and several Canadian universities. Its goal is the development of a comprehensive General Circulation Model of the troposphere‐stratosphere‐mesosphere system, starting from the AES/CCCma third‐generation atmospheric General Circulation Model. This paper describes the basic features of the first‐generation Canadian MAM and some aspects of its radiative‐dynamical climatology. Standard first‐order mean diagnostics are presented for monthly means and for the annual cycle of zonal‐mean winds and temperatures. The mean meridional circulation is examined, and comparison is made between the steady diabatic, downward controlled, and residual streamfunctions. It is found that downward control holds quite well in the monthly mean through most of the middle atmosphere, even during equinoctal periods. The relative roles of different drag processes in determining the...
Journal of Geophysical Research | 2000
J. de Grandpré; S. R. Beagley; V. I. Fomichev; E. Griffioen; J. C. McConnell; A. S. Medvedev; Theodore G. Shepherd
The climatology of ozone produced by the Canadian Middle Atmosphere Model (CMAM) is presented. This three-dimensional global model incorporates the radiative feedbacks of ozone and water vapor calculated on-line with a photochemical module. This module includes a comprehensive gas-phase reaction set and a limited set of heterogeneous reactions to account for processes occurring on background sulphate aerosols. While transport is global, photochemistry is solved from about 400 hPa to the top of the model at ∼95 km. This approach provides a complete and comprehensive representation of transport, emission, and photochemistry of various constituents from the surface to the mesopause region. A comparison of model results with observations indicates that the ozone distribution and variability are in agreement with observations throughout most of the model domain. Column ozone annual variation is represented to within 5–10% of the observations except in the Southern Hemisphere for springtime high latitudes. The vertical ozone distribution is generally well represented by the model up to the mesopause region. Nevertheless, in the upper stratosphere, the model generally underestimates the amount of ozone as well as the latitudinal tilting of ozone isopleths at high latitude. Ozone variability is analyzed and compared with measurements. The comparison shows that the phase and amplitude of the seasonal variation as well as shorter timescale variations are well represented by the model at various latitudes and heights. Finally, the impact of incorporating ozone radiative feedback on the model climatology is isolated. It is found that the incorporation of ozone radiative feedback results in a cooling of ∼8 K in the summer stratopause region, which corrects a warm bias that results when climatological ozone is used.
Journal of the Atmospheric Sciences | 2012
Charles McLandress; Theodore G. Shepherd; Saroja Polavarapu; S. R. Beagley
Nearly all chemistry‐climate models (CCMs) have a systematic bias of a delayed springtime breakdown of the Southern Hemisphere (SH) stratospheric polar vortex, implying insufficient stratospheric wave drag. In this study the Canadian Middle Atmosphere Model (CMAM) and the CMAM Data Assimilation System (CMAM-DAS) are used to investigate the cause of this bias. Zonal wind analysis increments from CMAMDAS reveal systematic negative values in the stratosphere near 608S in winter and early spring. These are interpretedas indicatinga bias in the model physics, namely, missing gravity wave drag (GWD). The negative analysisincrementsremainatanearlyconstantheightduringwinteranddescendasthevortexweakens,much like orographic GWD. This region is also where current orographic GWD parameterizations have a gap in wave drag, which is suggested to be unrealistic because of missing effects in those parameterizations. These findings motivate a pair of free-running CMAM simulations to assess the impact of extra orographic GWD at 608S. The control simulation exhibits the cold-pole bias and delayed vortex breakdown seen in the CCMs. In thesimulationwithextraGWD,the cold-polebiasis significantly reducedandthe vortexbreaks downearlier. Changes in resolved wave drag in the stratosphere also occur in response to the extra GWD, which reduce stratospheric SH polar-cap temperature biases in late spring and early summer. Reducing the dynamical biases, however, results in degraded Antarctic column ozone. This suggests that CCMs that obtain realistic columnozoneinthepresenceofanoverlystrongandpersistentvortexmaybedoingsothroughcompensating errors.
Journal of Climate | 2007
V. I. Fomichev; A. I. Jonsson; J. de Grandpré; S. R. Beagley; Charles McLandress; K. Semeniuk; Theodore G. Shepherd
Abstract The Canadian Middle Atmosphere Model (CMAM) has been used to examine the middle atmosphere response to CO2 doubling. The radiative-photochemical response induced by doubling CO2 alone and the response produced by changes in prescribed SSTs are found to be approximately additive, with the former effect dominating throughout the middle atmosphere. The paper discusses the overall response, with emphasis on the effects of SST changes, which allow a tropospheric response to the CO2 forcing. The overall response is a cooling of the middle atmosphere accompanied by significant increases in the ozone and water vapor abundances. The ozone radiative feedback occurs through both an increase in solar heating and a decrease in infrared cooling, with the latter accounting for up to 15% of the total effect. Changes in global mean water vapor cooling are negligible above ∼30 hPa. Near the polar summer mesopause, the temperature response is weak and not statistically significant. The main effects of SST changes a...
Journal of Geophysical Research | 2004
A. I. Jonsson; J. de Grandpré; V. I. Fomichev; J. C. McConnell; S. R. Beagley
Doubled CO2-induced cooling in the middle atmosphere : Photochemical analysis of the ozone radiative feedback
Journal of Geophysical Research | 2006
Charles McLandress; William E. Ward; V. I. Fomichev; K. Semeniuk; S. R. Beagley; Norman McFarlane; Theodore G. Shepherd
The extended Canadian Middle Atmosphere Model is used to investigate the large-scale dynamics of the mesosphere and lower thermosphere (MLT). It is shown that the 4-day wave is substantially amplified in southern polar winter in the presence of instabilities arising from strong vertical shears in the MLT zonal mean zonal winds brought about by parameterized nonorographic gravity wave drag. A weaker 4-day wave in northern polar winter is attributed to the weaker wind shears that result from weaker parameterized wave drag. The 2-day wave also exhibits a strong dependence on zonal wind shears, in agreement with previous modeling studies. In the equatorial upper mesosphere, the migrating diurnal tide provides most of the resolved westward wave forcing, which varies semiannually in conjunction with the tide itself; resolved forcing by eastward traveling disturbances is dominated by smaller scales. Nonmigrating tides and other planetary-scale waves play only a minor role in the zonal mean zonal momentum budget in the tropics at these heights. Resolved waves are shown to play a significant role in the zonal mean meridional momentum budget in the MLT, impacting significantly on gradient wind balance. Balance fails at low latitudes as a result of a strong Reynolds stress associated with the migrating diurnal tide, an effect which is most pronounced at equinox when the tide is strongest. Resolved and parameterized waves account for most of the imbalance at higher latitudes in summer. This results in the gradient wind underestimating the actual eastward wind reversal by up to 40%.
Geophysical Research Letters | 1998
Alexander S. Medvedev; G. P. Klaassen; S. R. Beagley
The spectral parameterization of gravity wave momentum deposition proposed by Medvedev and Klaassen has been incorporated into the Canadian Middle Atmosphere Model. Numerical experiments show that an anisotropic gravity wave source significantly improves the middle atmosphere circulation compared to an isotropic source. These results suggest that, at least in midlatitudes, the gravity waves primarily responsible for the momentum deposition at mesospheric heights are launched with observed phase velocities which are primarily in the same direction as the mean wind at tropospheric (source) heights.
Atmosphere-ocean | 1997
J. de Grandpré; J.W. Sandilands; J. C. McConnell; S. R. Beagley; P.C. Croteau; M.Y. Danilin
Abstract An important objective of middle atmosphere global climate modelling is the development of the capability of predicting the response of the middle atmosphere to natural or anthropogenic perturbations. To achieve this, a comprehensive chemistry package interactively coupled with radiative and dynamical modules is required. This paper presents preliminary results obtained with a photochemistry module which has been incorporated in the Canadian Middle Atmosphere Model (CMAM). The module contains 42 species including necessary oxygen, hydrogen, nitrogen, chlorine, bromine and methane oxidation cycle species. Photochemical balance equations are solved on‐line throughout the middle atmosphere at every dynamical time step. A full diurnal cycle is simulated with photolysis rates provided by a look‐up table. The chemistry solver is a mass conserving, fully implicit, backward difference scheme which currently uses less than 10% of the GCM run time. We present the results obtained from short integrations an...