Boundary layer and aerosol evolution during the 3rd Lagrangian experiment of ACE‐2     

Robert Wood  Doug Johnson  Simon Osborne  Meinrat O. Andreae  Brain Bandy  Timothy S. Bates  Colin O'Dowd  Paul Glantz  Kevin Noone  Patricia K. Quinn  Jochen Rudolph  Karsten Suhre 《Tellus. Series B, Chemical and physical meteorology》2000,52(2):401-422

Aircraft measurements are presented of the Lagrangian evolution of a marine boundary layer over a 30‐h period during the ACE‐2 field campaign. At the start of the observational period, a 500‐m deep polluted marine internal boundary layer (MIBL) was overlain by the remnants of a polluted continental boundary layer extending to around 2 km below a clean, dry free troposphere. The MIBL grew rapidly to a thickness of 900–1000 m in response to increasing sea surface temperatures. No significant aerosol spectral evolution was observed in the boundary layer. Low concentrations of SO₂ were observed in the MIBL suggesting that the air mass contained relatively aged aerosol. Aerosol spectra show a broad mode with a modal diameter of around 0.1μm. The polluted layer between the MIBL and the unpolluted free troposphere was only weakly and intermittently turbulent which prevented significant entrainment of clean air into the polluted layer from aloft. The polluted layer depth was thus controlled mainly by subsidence which as a result becomes shallower, decreasing from over 2000 m to around 1200 m during the observational period. The aerosol characteristics of the polluted layer were similar to those in the MIBL and so although the MIBL entrained considerable amounts of air from above the MIBL the aerosol characteristics underwent no significant change. This has important implications for the rate at which a polluted continental air mass is converted to a clean marine one. The dataset should prove useful in the validation of the modelling of continental pollution outbreaks.  相似文献   

Three-dimensional slope stability analysis of South Peak, Crowsnest Pass, Alberta, Canada   总被引：2，自引：2，他引：0  

Marc-Andr�� Brideau  Andrea Pedrazzini  Doug Stead  Corey Froese  Michel Jaboyedoff  David van Zeyl 《Landslides》2011,8(2):139-158

South Peak is a 7-Mm³ potentially unstable rock mass located adjacent to the 1903 Frank Slide on Turtle Mountain, Alberta. This paper presents three-dimensional numerical rock slope stability models and compares them with a previous conceptual slope instability model based on discontinuity surfaces identified using an airborne LiDAR digital elevation model (DEM). Rock mass conditions at South Peak are described using the Geological Strength Index and point load tests, whilst the mean discontinuity set orientations and characteristics are based on approximately 500 field measurements. A kinematic analysis was first conducted to evaluate probable simple discontinuity-controlled failure modes. The potential for wedge failure was further assessed by considering the orientation of wedge intersections over the airborne LiDAR DEM and through a limit equilibrium combination analysis. Block theory was used to evaluate the finiteness and removability of blocks in the rock mass. Finally, the complex interaction between discontinuity sets and the topography within South Peak was investigated through three-dimensional distinct element models using the code 3DEC. The influence of individual discontinuity sets, scale effects, friction angle and the persistence along the discontinuity surfaces on the slope stability conditions were all investigated using this code.  相似文献   

Fundamental differences between SPH and grid methods   总被引：1，自引：0，他引：1  

Oscar Agertz  Ben Moore  Joachim Stadel  Doug Potter  Francesco Miniati  Justin Read  Lucio Mayer  Artur Gawryszczak  rey Kravtsov  Åke Nordlund  Frazer Pearce  Vicent Quilis  Douglas Rudd  Volker Springel  James Stone  Elizabeth Tasker  Romain Teyssier  James Wadsley  Rolf Walder 《Monthly notices of the Royal Astronomical Society》2007,380(3):963-978

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Young star clusters immersed in intermediate-age fields in the Small Magellanic Cloud     

Andrés E. Piatti  Ata Sarajedini  Doug Geisler  David Clark  Juan Seguel 《Monthly notices of the Royal Astronomical Society》2007,377(1):300-316

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What do hydrologists mean when they use the term flushing?     

Doug Burns 《水文研究》2005,19(6):1325-1327

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昆仑断裂带东段滑动速率梯度     

Eric Kirdy  Nathan Harkins  Douglas Burbank  扈桂让 《世界地震译丛》2011,(1)

欧亚大陆走滑断裂带是否实现对青藏地壳及岩石层的向东挤出,很大程度上取决于断层尾端变形的动力学机制。本文我们利用青藏高原北部昆仑断裂最东段千年尺度的地貌标志物提供一组最新的滑动速率测定结果。该断裂带是印度?亚欧碰撞带产生的最主要走滑断裂带之一,在西藏岩石层向东挤出的模型中扮演着主要的作用。曾有人争论在相当长的长度内该断裂显示出相同的滑动速率。黄河支流上的河流阶地位移以及阶地上物质的14C测年可以控制晚更新世至全新世断层以来的滑动速率。结果显示沿断裂东部约150km滑动速率从>10mm/a～<2mm/a自西向东系统地递减。这些数据向那些认为整条断裂滑动速率保持一致的观点提出质疑,相反揭示出位错的梯度性,这与那些在断层尾端预期的情形是类似的。另外,沿断层的滑动看起来在增厚的高原地壳内部终结,因此沿昆仑断裂的滑动导致的西藏岩石层的挤出都会被断裂尾端周围高原的内部变形所吸收。  相似文献   

西南天山前缘乌拉根背斜南翼逆断层的发现及其地质意义   总被引：2，自引：1，他引：1       下载免费PDF全文

李涛  陈杰  肖伟鹏  Burbank D W  Thompson J  杨晓东 《地震地质》2011,33(2):277-288

塔里木盆地新疆喀什以西部分是西南天山和帕米尔两大对冲构造系统的会聚带,关于两者变形前缘和分界的确切位置存在不同认识.在乌恰县以南的玛依卡克盆地南缘,清晰可见属于帕米尔构造带、向N或NNE逆冲的帕米尔前缘逆冲推覆体(PFT).最近野外调查在盆地北部发现了西南天山前缘的最新变形带:向南逆冲的乌拉根背斜南翼断层.断层总体近E...  相似文献   

Identification of sorption processes and parameters for radionuclide transport in fractured rock     

Zhenxue Dai  Andrew Wolfsberg  Paul Reimus  Hailin Deng  Edward Kwicklis  Mei Ding  Doug Ware  Ming Ye 《Journal of Hydrology》2012

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Using GRASS GIS to Model Solar Irradiation on North Carolina Aquatic Habitats with Canopy Data     

Doug Newcomb 《Transactions in GIS》2012,16(2):161-176

Sunlight can have a significant impact on freshwater aquatic communities. Using 64‐ bit GRASS, a previously generated 18.2 m resolution forest canopy height grid for the State of North Carolina was used as a base elevation layer for calculation of 18.2 m resolution total irradiance (Watt‐hours/square meter/day) grids for 365 days of the year. Daily calculations were aggregated annually and overlaid on rasterized 1:24,000‐scale USGS hydrology with canopy type and seasonal filters to quantify annual solar irradiation input to streams and rivers in North Carolina. Bare earth calculations of solar irradiation for the aquatic habitats were compared to the canopy filtered calculations. There was substantially less solar irradiation in aquatic habitats under the canopy filtered model. Total solar irradiation for subbasins created from point locations of occurrences of Dwarf wedgemussel (Alasmidonta heterodon) were compared with total solar irradiation for watersheds created from locations with no mussels for the full subbasin, 1 km, and 500 m upstream from the sampling point. There was no significant difference in the amount of total solar irradiation modeled for the subbasins with Dwarf wedgemussel and watersheds with no mussels.  相似文献   

Atmospheric equilibrium,instability and energy transport at the last glacial maximum     

Nicholas M. J. Hall  Buwen Doug  Paul J. Valdes 《Climate Dynamics》1996,12(7):497-511

A range of diagnostics from two GCM simulations, one of the present-day climate and one of the last glacial maximum (LGM) is used to gain insight into their different temperature structures and eddy dynamics. There are large local increases in baroclinicity at the LGM, especially in the Atlantic storm track, with large accompanying increases in the low level transient eddy heat flux. However, the differences in the zonal mean are much smaller, and the increases in both baroclinicity and heat flux are confined to low levels. Supplementary experiments with baroclinic wave lifecycles confirm the marked contrast between local and zonal mean behaviour, but do not adequately explain the differences between the zonal mean climates. The total flux of energy across latitude circles in the Northern Hemisphere does not change much during DJF, although its transient component is actually reduced at the LGM (during JJA the transient component is increased). Calculations of total linear eddy diffusivity reveal that changes in the time mean stationary waves are chiefly responsible for the seasonal range of this quantity at the LGM, while they only account for half the seasonal range at the present-day.  相似文献