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31.
Several numerical experiments are conducted to examine the influence of mesoscale, bottom topography roughness on the inertial circulation of a wind-driven, mid-latitude ocean gyre. The ocean model is based on the quasi-geostrophic formulation, and is eddy-resolving as it features high vertical and horizontal resolutions (six layers and a 10 km grid). An antisymmetrical double-gyre wind stress curl forces the baroclinic modes and generates a strong surface jet. In the case of a flat bottom, inertia and inverse energy cascade force the barotropic mode, and the resulting circulation features strong, barotropic, inertial gyres. The sea-floor roughness inhibits the inertial circulation in the deep layers; the barotropic component of the flow is then forced by eddy-topography interactions, and its energy concentrates at the scales of the topography. As a result, the baroclinicity of the flow is intesified: the barotropic mode is reduced with regard to the baroclinic modes, and the bottom flow (constrained by the mesoscale sea-floor roughness) is decoupled from the surface flow (forced by the gyre-scale wind). Rectified, mesoscale bottom circulation induces an interfacial form stress at the thermocline, which enhances horizontal shear instability and opposes the eastward penetration of the jet. The mean jet is consequently shortened, but the instantaneous jet remains very turbulent, with meanders of large meridional extent. The sea-floor roughness modifies the energy pathways, and the eddies have an even more important role in the establishment of the mean circulation: below the thermocline, rectification processes are dominant, and eddies transfer energy toward permanent mesoscale circulations strongly correlated with topography, whereas above the thermocline mean flow and eddy generation are influenced by the mean bottom circulation through interfacial stress. The topography modifies the vorticity of the barotropic and highest baroclinic modes. Vorticity accumulates at the small topographic scales, and the vorticity content of the highest modes, which is very weak in the flat-bottom case, increases significantly. Few changes occur in surface-intensified modes. In the deep layers of the model, the inverse correlation between relative vorticity and topography at small scales ensures the homogenization of the potential vorticity, which mainly retains the largest scales of the bottom flow and the scale of β. 相似文献
32.
E. García-Bustamante J. F. González-Rouco J. Navarro E. Xoplaki P. A. Jiménez J. P. Montávez 《Climate Dynamics》2012,38(1-2):141-160
The variability and predictability of the surface wind field at the regional scale is explored over a complex terrain region in the northeastern Iberian Peninsula by means of a downscaling technique based on Canonical Correlation Analysis. More than a decade of observations (1992–2005) allows for calibrating and validating a statistical method that elicits the main associations between the large scale atmospheric circulation over the North Atlantic and Mediterranean areas and the regional wind field. In an initial step the downscaling model is designed by selecting parameter values from practise. To a large extent, the variability of the wind at monthly timescales is found to be governed by the large scale circulation modulated by the particular orographic features of the area. The sensitivity of the downscaling methodology to the selection of the model parameter values is explored, in a second step, by performing a systematic sampling of the parameters space, avoiding a heuristic selection. This provides a metric for the uncertainty associated with the various possible model configurations. The uncertainties associated with the model configuration are considerably dependent on the spatial variability of the wind. While the sampling of the parameters space in the model set up moderately impact estimations during the calibration period, the regional wind variability is very sensitive to the parameters selection at longer timescales. This fact illustrates that downscaling exercises based on a single configuration of parameters should be interpreted with extreme caution. The downscaling model is used to extend the estimations several centuries to the past using long datasets of sea level pressure, thereby illustrating the large temporal variability of the regional wind field from interannual to multicentennial timescales. The analysis does not evidence long term trends throughout the twentieth century, however anomalous episodes of high/low wind speeds are identified. 相似文献
33.
Synoptic and mesoscale study of a severe convective outbreak with the nonhydrostatic Global Environmental Multiscale (GEM) model 总被引:1,自引:0,他引:1
A. Erfani A. Méthot R. Goodson S. Bélair K.-S. Yeh J. Côté R. Moffet 《Meteorology and Atmospheric Physics》2003,82(1-4):31-53
Summary ?A nonhydrostatic 4-km version of the Global Environmental Multiscale (GEM) model, with detailed microphysics included, was
used to forecast the initiation, development, and structure of a tornado-producing supercell storm that occurred near Pine
Lake (Alberta, Canada) on 15 July 2000. Examination of observations and comparison with conceptual models indicate that this
storm is a good example of supercell storms that regularly produce summertime severe weather over Alberta.
It was found that the high-resolution model was able to reproduce the early initiation of convective activity along the Rocky
Mountains foothills, as well as the rapid northeastward propagation towards the Pine Lake area and the subsequent intensification
into a supercell storm. The general structures of the forecasted convective system correspond well with conceptual representations
of such events. Overall, this high-resolution forecast of the Pine Lake supercell storm was a significant improvement over
the current operational version of the GEM model (24 km), which was not able to intensify the foothills’ convection into a
supercell storm. Finally, it was found that the nonhydrostatic version of the model produces better trajectory and propagation
speed of the convective system, as compared with the hydrostatic one.
Received March 20, 2001; revised August 24, 2001 相似文献
34.
María Charco José Fernández Francisco Luzón Kristy F. Tiampo John B. Rundle 《Pure and Applied Geophysics》2007,164(4):865-878
Surface displacements and gravity changes due to volcanic sources are influenced by medium properties. We investigate topographic,
elastic and self-gravitation interaction in order to outline the major factors that are significant in data modelling. While
elastic-gravitational models can provide a suitable approximation to problems of volcanic loading in areas where topographic
relief is negligible, for prominent volcanoes the rough topography could affect deformation and gravity changes to a greater
extent than self-gravitation. This fact requires the selection, depending on local relief, of a suitable model for use in
the interpretation of surface precursors of volcanic activity. We use the three-dimensional Indirect Boundary Element Method
to examine the effects of topography on deformation and gravity changes in models of magma chamber inflation/deflation. Topography
has a significant effect on predicted surface deformation and gravity changes. Both the magnitude and pattern of the geodetic
signals are significantly different compared to half-space solutions. Thus, failure to account for topographic effects in
areas of prominent relief can bias the estimate of volcanic source parameters, since the magnitude and pattern of deformation
and gravity changes depend on such effects. 相似文献
35.
Gustavo?Bastos?Lyra Tamíres?Partelli?Correia José?Francisco?de?Oliveira-Júnior Marcelo?ZeriEmail authorView authors OrcID profile 《Theoretical and Applied Climatology》2018,134(3-4):955-965
Five deterministic methods of spatial interpolation of monthly rainfall were compared over the state of Rio de Janeiro, southeast Brazil. The methods were the inverse distance weight (IDW), nearest neighbor (NRN), triangulation with linear interpolation (TLI), natural neighbor (NN), and spline tension (SPT). A set of 110 weather stations was used to test the methods. The selection of stations had two criteria: time series longer than 20 years and period of data from 1960 to 2009. The methods were evaluated using cross-validation, linear regression between values observed and interpolated, root mean square error (RMSE), coefficient of determination (r 2), coefficient of variation (CV, %), and the Willmott index of agreement (d). The results from different methods are influenced by the meteorological systems and their seasonality, as well as by the interaction with the topography. The methods presented higher precision (r 2) and accuracy (d, RMSE) during the summer and transition to autumn, in comparison with the winter or spring months. The SPT had the highest precision and accuracy in relation to other methods, in addition to having a good representation of the spatial patterns expected for rainfall over the complex terrain of the state and its high spatial variability. 相似文献
36.
José Luís Argaín Miguel A. C. Teixeira Pedro M. A. Miranda 《Boundary-Layer Meteorology》2017,165(1):145-160
A method is proposed for estimating the surface-layer depth \((z_s)\) and the friction velocity \((u_*)\) as a function of stability (here quantified by the Obukhov length, L) over the complete range of unstable flow regimes. This method extends that developed previously for stable conditions by Argaín et al. (Boundary-Layer Meteorol 130:15–28, 2009), but uses a qualitatively different approach. The method is specifically used to calculate the fractional speed-up \((\varDelta S)\) in flow over a ridge, although it is suitable for more general boundary-layer applications. The behaviour of \(z_s \left( L\right) \) and \(u_*\left( L\right) \) as a function of L is indirectly assessed via calculation of \(\varDelta S\left( L\right) \) using the linear model of Hunt et al. (Q J R Meteorol Soc 29:16–26, 1988) and its comparison with the field measurements reported in Coppin et al. (Boundary-Layer Meteorol 69:173–199, 1994) and with numerical simulations carried out using a non-linear numerical model, FLEX. The behaviour of \(\varDelta S\) estimated from the linear model is clearly improved when \(u_*\) is calculated using the method proposed here, confirming the importance of accounting for the dependences of \(z_s\left( L \right) \) and \(u_*\left( L \right) \) on L to better represent processes in the unstable boundary layer. 相似文献
37.
38.
珠兰埠岩体是南岭地区大面积出露的岩体之一, 也是缺少精确年龄数据的复杂岩体之一, 在以往工作中被认为是燕山期早期岩体, 此后相关研究较少, 由于时代和方法的限制未见确切的同位素年龄数据发表。本文采用LA-(MC)-ICPMS锆石U-Pb法对珠兰埠复式岩体的粗粒斑状黑云母花岗岩、中细粒含斑黑云母花岗岩进行同位素年代学研究, 探讨其成矿可能性。获得粗粒斑状黑云母花岗岩、中细粒含斑黑云母花岗岩等时线年龄分别为228.7±2.0 Ma和231.0±1.2 Ma, 表明珠兰埠复式花岗岩体主体形成于印支期, 而不是前人认为的燕山早期, 由此修正了岩体成岩时代, 同时结合珠兰埠岩体的地球化学特征与印支期花岗岩的成矿特点, 较好印证了目前在该岩体及其周边, 并未发现钨矿床的现象。本研究成果为赣南地区花岗岩研究提供了新的实例。 相似文献
39.
内蒙古林西朝阳沟早白垩世花岗岩锆石U-Pb年代学和地球化学及其意义 总被引:1,自引:0,他引:1
林西县朝阳沟地区位于华北板块与西伯利亚板块之间的兴蒙造山带的东部.朝阳沟花岗岩体的LA-ICP-MS锆石U-Pb测年结果表明,岩体的侵位时间为早白垩世(126.2±2.5 Ma).地球化学分析显示,该花岗岩体具有富硅(SiO2=68.5%~72.1%)、铝(Al2O3=14.05%~14.95%)、碱(K2O+Na2O=8.34%~10.03%)和Fe2O(3 2.27%~4.15%)的特点,属于准铝质碱性花岗岩系列;A/CNK=0.97~1.09,Mg#值较高,为12.66~15.02;稀土配分曲线呈明显的右倾型,轻、重稀土元素分馏明显;具有显著的Eu负异常和Ba、Ta、Nb、Sr、P、Ti亏损,富集Rb、Th、U、K等大离子亲石元素.在(Yb+Nb)-Rb判别图解和R1-R2判别图解中,样品全部落于后碰撞花岗岩区和造山晚期花岗岩区.结合区域地质背景,认为该岩体形成于后碰撞伸展构造环境中. 相似文献
40.
P. Schmidt-Thomé 《International Journal of Earth Sciences》1943,33(4-6):446-473
Ohne Zusammenfassung 相似文献