共查询到20条相似文献，搜索用时 62 毫秒
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西文建立了一处简单的热带海气耦合模式，模式大气和海洋中含了Ｋｅｌｉｖｎ波和长Ｒｏｓｓｂｙ波。在赤道β平面近似下，讨论了取耦合系统中最大径向模时，即大气和海洋中只存在Ｋｅｌｉｎ波时耦合波的性质。结果指出，向东传的耦合Ｋｅｌｖｉｎ波可以出现不稳定性，并且由于海气相互作用，在长波部分可以产生向西传的耦合Ｋｅｌｖｉｎ波。耦合Ｋｅｌｖｉｎ波的性质与模式中所选用的参数有很大关系，当大气与海洋中自由波的频率相差 相似文献
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地形对热带大气超长尺度Rossby波动的影响 总被引：5，自引：0，他引：5
应用赤道β平面近似，建立一个简单的正压大气半地转浅水线性模式，在连续方程中引入地形的作用，讨论地形对热带大气超长尺度Ｒｏｓｓｂｙ波的影响。结果分析表明，起伏不平的于形动力抬升作用导致热带大气超长尺度Ｒｏｓｓｂｙ波动不稳定并且影响波动的特性。 相似文献
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热带大气的CISK-Rossby波和30-50天振荡 总被引：1，自引：0，他引：1
利用斜压准地转滤波方法，通过引入一个反映ＣＩＳＫ机制的无量纲凝结潜热参数η（Ｚ），建立了描述热带大气的ＣＩＳＫ－Ｒｏｓｓｂｙ波模式，并求得了该模式的解析解。理论研究表明，考虑ＣＩＳＫ机制的ＣＩＳＫ－Ｒｏｓｓｂｙ波与经典的Ｒｏｓｓｂｙ波有明显差别，它可较好地解释热带大气３０—５０ｄ振荡现象。 相似文献
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从热带大气波动的频率方程出发，详细分析了过去给出的低频Ｒｏｓｓｂｙ波的近似频率公式ω＝－βκ／［（２ｎ＋１）β／ｃ０＋κ＾２］，发现其对热带Ｒｏｓｓｂｙ波的性质有一定程度的歪曲。针对这一问题，经分析得到一个能更精确地表征热带Ｒｏｓｓｂｙ波性质的近似频散公式ω＝－βκ／［（２ｎ＋１）β／ｃ０＋４ｎ（ｎ＋１）／（２ｎ＋１）＾２ｋ＾２］，还简要地比较了热带线性Ｒｏｓｓｂｙ波和孤立Ｒｏｓｓｂｙ波两者的频散 相似文献
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本文能过对美国宇航局Ｎｉｍｂｕｓ－７卫星观测的１９７９－１９８６年中国西部积雪资料的分析发现，２－３周的低频振荡现象普遍存在并与大气环流异常密切相关；大气环流对半年积雪２－３周的低频振荡有着明显的线性响应；冬半年积雪的这种低频振荡能激发出北半球５００ｈＰａ高度场准定常Ｒｏｓｓｂｙ波，并通过二维的Ｒｏｓｓｂｙ波能量频散而影响到北美。 相似文献
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对热带不稳定海气相互作用模式的改进 总被引：1，自引：1，他引：1
对以前提出的热带海气相互作用模式［１］风应力的参数化作了改进。和以前一样，在这个耦合模式中，滤去了大气和海洋中的重力惯性波，只保留了向西传播的Ｒｏｓｓｂｙ波。但经过海气相互作用后，理论分析指出，在耦合模式中存在着快的和慢的两类波动。快波频率的实部、即其相速度是向西传的，并接近于未经海气相互作用时大气中Ｒｏｓｓｂｙ波的频率；而慢波的性质和以前的结果类似，短波部分是向西传的，长波部分向东传，东传波的临界波数随海气相互作用增强向短波部分位移。与以前结果不同的是，除一个慢波不稳定增长外，另一个快波在长波部分也是不稳定增长的。海气相互作用越强，不稳定增长率和不稳定波所出现的波段范围越大。另外，本文的研究结果还指出，高频和低频不稳定波产生的物理条件是不一样的。 相似文献
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利用由两层准地转模式简化的低谱模式，得知相当正压结构Ｒｒｏｓｓｂｙ波为平衡态，讨论了具有相当正压结构的Ｒｏｓｓｂｙ波存在所需条件；并以定常Ｒｏｓｓｂｙ波（相当正压结构）为基态，导出反映高低层Ｒｏｓｓｂｙ波位相变化的振荡方程，指出高低层位相差的变化与垂直切交流的扰动、平均层上流函数和热成风流函数波动部分振幅扰动（Ａ’和Ｂ’）的关系，说明相当正压结构和斜医结构的Ｒｏｓｓｂｙ波是相互转换的。 相似文献
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On stochastic stability of regional ocean models to finite-amplitude perturbations of initial conditions 总被引：1，自引：0，他引：1
We consider error propagation near an unstable equilibrium state (classified as an unstable focus) for spatially uncorrelated and correlated finite-amplitude initial perturbations using short- (up to several weeks) and intermediate (up to 2 months) range forecast ensembles produced by a barotropic regional ocean model. An ensemble of initial perturbations is generated by the Latin Hypercube design strategy, and its optimal size is estimated through the Kullback–Liebler distance (the relative entropy). Although the ocean model is simple, the prediction error (PE) demonstrates non-trivial behavior similar to that existing in 3D ocean circulation models. In particular, in the limit of zero horizontal viscosity, the PE at first decays with time for all scales due to dissipation caused by non-linear bottom friction, and then grows faster than (quasi)-exponentially. Statistics of a prediction time scale (the irreversible predictability time (IPT)) quickly depart from Gaussian (the linear predictability regime) and becomes Weibullian (the non-linear predictability regime) as amplitude of initial perturbations grows. A transition from linear to non-linear predictability is clearly detected by the specific behavior of IPT variance. A new analytical formula for the model predictability horizon is introduced and applied to estimate the limit of predictability for the ocean model. 相似文献
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Two sets of sensitivity experiments are presented. The first set consists of three 100-day integrations with perpetual January conditions: a reference integration, an integration with a uniform +2 K sea surface temperature (SST) anomaly, and an integration with an anomaly of reverse sign. The second set is similar, but with perpetual July conditions. The zonal mean components of the water and heat budgets at the surface are studied over ocean and over land separately.The values of the reference integration are very close to those obtained when the model is run with annual cycle conditions, and reasonably close to observed values over 60° N−40° S ocean. The SST anomalies produce generally a stronger response in July than in January. This response is linear for the averages over ocean, but if we consider the zonal distribution, only the longwave radiation, latent and sensible heat exhibit a linear response. The model response to temperature increase consists of an enhancement of the water cycle over ocean, and a heat transfer from the ocean, through the latent heat, to the continent. In January, we observe also a water transfer from the ocean to the continent. As a consequence of the heat transfer, the land surface temperature increases by the same magnitude as the SST. 相似文献
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The possibility of using a nonlinear empirical atmospheric model for hybrid coupled atmosphere-ocean modelling has been examined
by using a neural network (NN) model for predicting the contemporaneous wind stress field from the upper ocean state. Upper
ocean heat content (HC) from a 6-layer ocean model was a better predictor of the wind stress than the (observed or modelled)
sea surface temperature (SST). Our results showed that the NN model generally had slightly better skills in predicting the
contemporaneous wind stress than the linear regression (LR) model in the off-equatorial tropical Pacific and in the eastern
equatorial Pacific. When the wind stresses from the NN and LR models were used to drive the ocean model, slightly better SST
skills were found in the off-equatorial tropical Pacific and in the eastern equatorial Pacific when the NN winds were used
instead of the LR winds. Better skills for the model HC were found in the western and central equatorial Pacific when the
NN winds were used instead of the LR winds. Why NN failed to show more significant improvement over LR in the equatorial Pacific
for the wind stress and SST is probably because the relationship between the surface ocean and the atmosphere in the equatorial
Pacific over the seasonal time scale is almost linear.
Received: 2 March 1999 / Accepted: 13 July 2000 相似文献
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二维的大气CO2——大西洋碳循环模式 总被引：5，自引：1，他引：5
本文描述了一个二维（纬度×深度）的大西洋碳循环模式，模拟了大气和海洋间CO2的交换以及碳在海洋中的输送过程。模式在运行时使用了一个12层的三维动力学模拟的海洋环流的结果。大西洋被划分成397个网格箱，每个箱子中各种形式的碳的含量、总碱度、溶解的无机营养物和溶解氧的浓度以及几种14C(碳14)同位素的值分别得到求解。模式稳定状态的计算采用解大型稀疏线性方程组的直接解法。计算结果与“地球化学的海洋研究（GEOSECS）”的实际观测数据对比，表明模式较好地再现了实际大西洋中几种化学量的分布。 相似文献
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Inorganic carbon in the ocean is modelled as a passive tracer advected by a three-dimensional current field computed from a dynamical global ocean circulation model. The carbon exchange between the ocean and atmosphere is determined directly from the (temperature-dependent) chemical interaction rates in the mixed layer, using a standard CO2 flux relation at the air-sea interface. The carbon cycle is closed by coupling the ocean to a one-layer, horizontally diffusive atmosphere. Biological sources and sinks are not included. In this form the ocean carbon model contains essentially no free tuning parameters. The model may be regarded as a reference for interpreting numerical experiments with extended versions of the model including biological processes in the ocean (Bacastow R and Maier-Reimer E in prep.) and on land (Esser G et al in prep.). Qualitatively, the model reproduces the principal features of the observed CO2 distribution bution in the surface ocean. However, the amplitudes of surface pCO2 are underestimated in upwelling regions by a factor of the order of 1.5 due to the missing biological pump. The model without biota may, nevertheless, be applied to compute the storage capacity of the ocean to first order for anthropogenic CO2 emissions. In the linear regime, the response of the model may be represented by an impulse response function which can be approximated by a superposition of exponentials with different amplitudes and time constants. This provides a simple reference for comparison with box models. The largest-amplitude (0.35) exponential has a time constant of 300 years. The effective storage capacity of the oceans is strongly dependent on the time history of the anthropogenic input, as found also in earlier box model studies. 相似文献
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A sequence of numerical experiments is conducted using a linear, semi-spectral equatorial ocean model and an advanced data assimilation scheme. The numerical model is based on decomposition of the oceanic fields into Kelvin and Rossby waves belonging to the baroclinic modes of a stratified equatorial ocean. The assimilation procedure finds that solution to the model equations that best fits, in the generalized least-squares sense, all observations made within some specified space-time interval. All experiments are of the ‘identical twin’ type; synthetic data are generated by sampling the observable fields produced by a control run of the model, then the data are assimilated using the same model. The sequence of numerical experiments serves two purposes; to demonstrate the performance of the assimilation procedure in the context of a fully three-dimensional, time-varying equatorial ocean model; and to examine the utility of specified data sets, in particular, observations of sea level, in estimating the state of the equatorial ocean. The results indicate that the assimilation procedure works very well when sufficient data are provided. However, sea-level data alone are not sufficient and must be supplemented with subsurface observations if more than a few baroclinic modes are allowed in the model ocean. The required amount of supplementary subsurface data (in the form of density profiles in these experiments) can be reduced by imposing smoothness contraints on the recovered model solution. 相似文献
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Tamara L. Townsend Harley E. Hurlburt Patrick J. Hogan 《Dynamics of Atmospheres and Oceans》2000,32(3-4)
In studies of large-scale ocean dynamics, often quoted values of Sverdrup transport are computed using the Hellerman–Rosenstein wind stress climatology. The Sverdrup solution varies, however, depending on the wind set used. We examine the differences in the large-scale upper ocean response to different surface momentum forcing fields for the North Atlantic Ocean by comparing the different Sverdrup interior/Munk western boundary layer solutions produced by a 1/16° linear numerical ocean model forced by 11 different wind stress climatologies. Significant differences in the results underscore the importance of careful selection of a wind set for Sverdrup transport calculation and for driving nonlinear models. This high-resolution modeling approach to solving the linear wind-driven ocean circulation problem is a convenient way to discern details of the Sverdrup flow and Munk western boundary layers in areas of complicated geometry such as the Caribbean and Bahamas. In addition, the linear solutions from a large number of wind sets provide a well-understood baseline oceanic response to wind stress forcing and thus, (1) insight into the dynamics of observed circulation features, by themselves and in conjunction with nonlinear models, and (2) insight into nonlinear model sensitivity to the choice of wind-forcing product.The wind stress products are evaluated and insight into the linear dynamics of specific ocean features is obtained by examining wind stress curl patterns in relation to the corresponding high-resolution linear solutions in conjunction with observational knowledge of the ocean circulation. In the Sverdrup/Munk solutions, the Gulf Stream pathway consists of two branches. One separates from the coast at the observed separation point, but penetrates due east in an unrealistic manner. The other, which overshoots the separation point at Cape Hatteras and continues to flow northward along the continental boundary, is required to balance the Sverdrup interior transport. A similar depiction of the Gulf Stream is commonly seen in the mean flow of nonlinear, eddy-resolving basin-scale models of the North Atlantic Ocean. An O(1) change from linear dynamics is required for realistic simulation of the Gulf Stream pathway. Nine of the eleven Sverdrup solutions have a C-shaped subtropical gyre, similar to what is seen in dynamic height contours derived from observations. Three mechanisms are identified that can contribute to this pattern in the Sverdrup transport contours. Along 27°N, several wind sets drive realistic total western boundary current transport (within 10% of observed) when a 14 Sv global thermohaline contribution is added (COADS, ECMWF 10 m re-analysis and operational, Hellerman–Rosenstein and National Centers for Environmental Prediction (NCEP) surface stress re-analysis), a few drive transport that is substantially too high (ECMWF 1000 mb re-analysis and operational and Isemer–Hasse) and Fleet Numerical Meteorology and Oceanography Center (FNMOC) surface stresses give linear transport that is slightly weaker than observed. However, higher order dynamics are required to explain the partitioning of this transport between the Florida Straits and just east of the Bahamas (minimal in the linear solutions vs. 5 Sv observed east of the Bahamas). Part of the Azores Current transport is explained by Sverdrup dynamics. So are the basic path of the North Atlantic Current (NAC) and the circulation features within the Intra-Americas Sea (IAS), when a linear rendition of the northward upper ocean return flow of the global thermohaline circulation is added in the form of a Munk western boundary layer. 相似文献
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Abstract The European Space Agency ERS‐1 C‐band V‐V polarization synthetic aperture radar (SAR) and the Russian Almaz S‐band H‐H polarization SAR are compared for their wavenumber response to ocean wave fields existing on 23 November 1991 at the Grand Banks site of the North American ERS‐1 SAR Wave Spectra Validation Experiment. Two‐dimensional wave spectra from two Wavec heave, pitch and roll buoys and a Canadian CV‐580 aircraft C‐band V‐V polarization SAR are used to condition a linear modulation transfer model of wave imaging with SAR. A model of hydrodynamic modulation is included with the velocity bunching and tilt imaging mechanisms to better understand wind and wave interactions. Krogstad's quasi‐linear formulation of Hasselmann's ocean‐SAR integral transform is applied to model SAR velocity bunching and azimuth smearing. Narrow and broad bandwidth components of azimuth wavenumber response for the aircraft SAR are associated with, respectively, non‐linear and incoherent velocity smearing during Doppler resolution of the radar scene. The stationary resolutions of the SAR systems are compared for homogeneous scenes of wind‐roughened, but fetch‐limited, sea surfaces. This comparison is conducted in the Chesapeake Bay of Maryland using ERS‐1 and Almaz satellite imagery collected on 9 May 1992 and 14 May 1991, respectively. The results confirm that SAR imaging of ocean waves can be improved by flying platforms with low R/V (range/velocity) ratios to alleviate the azimuth velocity smear, and near‐nadir incidence angles to increase the effect of tilt modulation. 相似文献
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In this paper we explore the impact of atmospheric nonlinearities on the optimal growth of initial condition error of El Niño and the Southern Oscillation (ENSO) prediction using singular vector (SV) analysis. This is performed by comparing and analyzing SVs of two hybrid coupled models (HCMs), one composed of an intermediate complexity dynamical ocean model coupled with a linear statistical atmospheric model, and the other one with the same ocean model coupled with a nonlinear statistical atmosphere. Tangent linear and adjoint models for both HCMs are developed. SVs are computed under the initial conditions of seasonal background and actual ENSO cycle simulated by the ocean model forced with the real wind data of 1980–1999. The optimization periods of 3, 6 and 9 months are individually considered. The results show that the first SVs in both HCMs are very similar to each other, characterized by a central east-west dipole pattern spanning over the entire tropical Pacific. The spatial patterns of the leading SV in both HCMs are not sensitive to optimization periods and initial time. However, the first singular value, indicating the optimal growth rate of prediction error, displays considerable differences between the two HCMs, indicating a significant impact of atmospheric nonlinearities on the optimal growth of ENSO prediction error. These differences are greater with increasing optimization time, suggesting that the impact of atmospheric nonlinearities on the optimal growth of prediction error becomes larger for a longer period of prediction. 相似文献