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1.
提出了扩展雅可比椭圆函数方法,来求得Petviashvili方程的精确解析解.Petviashvili方程被视为正压准地转位涡度方程的非地转扩展,应用该方法可以得到很多二维非线性Rossby波的周期波解,在取极限情况下,也可以得到二维Rossby孤立子解.  相似文献   

2.
针对描述非线性Rossby波的正压准地转位涡方程,设计了一个隐式差分迭代格式,通过数值解与精确解对比的方法,验证了差分迭代格式的精度和稳定性.首先将正压准地转位涡方程简化为Couette流方程,对比了Couette流精确解和数值解,验证了差分格式对线性方程数值计算的精度和稳定性;然后通过构造精确解和修改原方程的方法,验...  相似文献   

3.
本文从正压流体的准地转位涡方程出发,考虑到Rossby波随时间、空间演变的多尺度特性,采用多重尺度和摄动展开的方法推导了在线性缓变下垫面和耗散共同作用下的非线性Rossby波包演变满足推广的非线性Schdinger方程,并得到单个包络的孤立波解.通过分析包络的孤立波解,指出在耗散与下垫面共同作用下,大气中会出现双曲正割形状的Rossby孤立波包.同时得到,在切变基本流存在的情况下,地形强迫和耗散对Rossby包络孤立波的传播速度、波数和频率均有影响的结论.  相似文献   

4.
本文在正压流体中,从包含完整Coriolis参数的准地转位涡方程出发,在弱非线性长波近似下,采用多时空尺度和摄动方法,推导出大气非线性Rossby波振幅演变满足带有地形强迫的非线性Zakharov-Kuznetsov(ZK)-Burgers方程.结果分析表明:地球旋转的水平分量、β效应、地形效应和耗散都是诱导二维Rossby波产生的重要因子.  相似文献   

5.
正压流体中,从准地转位涡方程出发采用摄动方法和时空伸长变换推导了在缓变地形下β效应的Rossby代数孤立波方程,得到Rossby波振幅满足带有缓变地形非齐次Benjamin-Davis-Ono(BDO)方程的结论.通过分析孤立Rossby波振幅的演变,指出了β效应、地形效应是诱导Rossby孤立波产生的重要因素,说明了在缓变地形强迫效应和非线性作用相平衡的假定下,Rossby孤立波振幅的演变满足非齐次BDO方程,给出在切变基本气流下缓变地形和正压流体中Rossby波的相互作用.  相似文献   

6.
Rossby波的螺旋斑图   总被引:1,自引:0,他引:1       下载免费PDF全文
应用描写大气大尺度运动的准地转方程组,求得了大气Rossby波的三维定常流场以及相应的位温场、涡度场和散度场,其中的三维流场构成了物理空间的一个非线性自治动力系统. 研究表明,Rossby波具有  相似文献   

7.
具有非线性地形的正压流体中孤立Rossby波的mKdV方程   总被引:1,自引:1,他引:0       下载免费PDF全文
正压流体中,采用摄动方法将准地转位涡方程推导出地形效应的mKdV方程,得到Rossby波振幅的演变满足地形效应的mKdV方程的结论,说明地形效应是诱导Rossby孤立波的重要因素.  相似文献   

8.
在正压流体中,从准地转正压涡度方程出发,运用时空伸长变换和摄动法推导了在完整Coriolis力作用下的非线性Rossby孤立波包振幅的演变满足非齐次非线性Schrodinger方程的结论.结果分析表明,完整Coriolis力中的水平分量对Rossby孤立波产生一定的影响,同时,β效应和地形效应也是诱导Rossby孤立波产生的重要因素.  相似文献   

9.
在正压流体中从包含地形的准地转位涡出发,利用行波变换和约化摄动法导出了弱二次切变基本流下β变化和地形共同作用的正压Rossby孤立波振幅满足非齐次KdV方程.并计算了非齐次KdV方程的系数,说明弱二次切变基本气流、β变化和地形对Rossby孤立波的作用.  相似文献   

10.
旋转流场中的格子波耳兹曼模型   总被引:2,自引:1,他引:2       下载免费PDF全文
在大尺度的旋转流场中,由于存在哥氏力,使流体的流动出现了一系列复杂的动力学现象.在原格子Boltzmann模型研究的基础上,引入了哥氏力效应,发展了一个旋转流场中的格子Boltzmann模型.从该模型出发可导出地球流体力学方程,用这一模型对理想边界条件下的北半球大气环流进行了数值计算.数值结果很好地再现了大尺度地转流的流动特征.从理论和数值实验上验证了该模型的适用性.  相似文献   

11.
Abstract

The mutual interaction of fields induced by spatially separated potential vorticity sources in a quasi-geostrophic barotropic flow is investigated using the weakly nonlinear approach. It is found that a powerful nonlinear response can be triggered by Rossby lee waves. This resonance phenomenon which dominates all other nonlinear corrections depends on certain global resonance conditions and on the change in the phase of the Rossby lee wave across the distance separating the sources. The response is particularly strong for topographic forcing possessing δ-function characterisitics.  相似文献   

12.
Abstract

The adjustment of a nonlinear, quasigeostrophic, stratified ocean to an impulsively applied wind stress is investigated under the assumption that barotropic advection of vortex tube length is the most important nonlinearity. The present study complements the steady state theories which have recently appeared, and extends earlier, dissipationless, linear models.

In terms of Sverdrup transport, the equation for baroclinic evolution is a forced advection-diffusion equation. Solutions of this equation subject to a “tilted disk” Ekman divergence are obtained analytically for the case of no diffusion and numerically otherwise. The similarity between the present equation and that of a forced barotropic fluid with bottom topography is shown.

Barotropic flow, which is assumed to mature instantly, can reverse the tendency for westward propagation, and thus produce regions of closed geostrophic contours. Inside these regions, dissipation, or equivalently the eddy field, plays a central role. We assume that eddy mixing effects a lateral, down-gradient diffusion of potential vorticity; hence, within the closed geostrophic contours, our model approaches a state of uniform potential vorticity. The solutions also extend the steady-state theories, which require weak diffusion, by demonstrating that homogenization occurs for moderately strong diffusion.

The evoiution of potential vorticity and the thermocline are examined, and it is shown that the adjustment time of the model is governed by dissipation, rather than baroclinic wave propagation as in linear theories. If dissipation is weak, spin-up of a nonlinear ocean may take several times that predicted by linear models, which agrees with analyses of eddy-resolving general circulation models. The inclusion of a western boundary current may accelerate this process, although dissipation will still play a central role.  相似文献   

13.
ABSTRACT

A framework of variational principles for stochastic fluid dynamics was presented by Holm, and these stochastic equations were also derived by Cotter, Gottwald and Holm. We present a conforming finite element discretisation for the stochastic quasi-geostrophic equation that was derived from this framework. The discretisation preserves the first two moments of potential vorticity, i.e. the mean potential vorticity and the enstrophy. Following the work of Dubinkina and Frank, who investigated the statistical mechanics of discretisations of the deterministic quasi-geostrophic equation, we investigate the statistical mechanics of our discretisation of the stochastic quasi-geostrophic equation. We compare the statistical properties of our discretisation with the Gibbs distribution under assumption of these conserved quantities, finding that there is an agreement between the statistics under a wide range of set-ups.  相似文献   

14.
The characteristics of the disturbances in the atmosphere and oceans and in other stably stratified and rotating fluids are analyzed according to their phase and group velocities. It is shown that both stable stratification and rotation augment the velocity of the sound waves, and that the internal gravity waves and inertial waves are mutually exclusive when the Brunt-Väisälä frequency is different from the Coriolis parameter. It is also shown that both the barotropic and the internal Rossby waves are well separated from the gravity waves and that they can be represented accurately by the quasi-geostrophic potential vorticity equation, even close to the equator, except for the one member withn=0 which is coupled with an eastward propagating gravity wave.  相似文献   

15.
Within the framework of the quasi-geostrophic approximation, the interactions of two identical initially circular vortex patches are studied using the contour dynamics/surgery method. The cases of barotropic vortices and of vortices in the upper layer of a two-layer fluid are considered. Diagrams showing the end states of vortex interactions and, in particular, the new regime of vortex triplet formation are constructed for a wide range of external parameters. This paper shows that, in the nonlinear evolution of two such (like-signed) vortices, the filaments and vorticity fragments surrounding the merged vortex often collapse into satellite vortices. Therefore, the conditions for the formation and the quasi-steady motions of a new type of triplet-shaped vortex structure are obtained.  相似文献   

16.
Abstract

Merilees and Warn's (1975) nonlinear interaction analysis of two-dimensional nondivergent flow is extended to examine the quasi-geostrophic two-layer model. Two sets of triads exist in this model (Salmon, 1978). The purely barotropic triads are the same as the triads examined by Merilees and Warn. Baroclinic-barotropic triads are found to exchange more energy or potential enstrophy with smaller or larger scales depending on the scale of motion as compared with the internal Rossby deformation radius and the relative wavenumber position of baroclinic and barotropic components.  相似文献   

17.
Zusammenfassung Es wurde versucht mittels der numerischen Integration der zweidimensionalen homogenen Wellengleichung bei bekannter Phasengeschwindigkeit Niveauänderungen im 500 mb Niveau vorherzusagen. Gleichzeitig wurde das Ergebnis mit der prognostizierten Niveauänderung, die mittels graphischer Integration der barotropen Wirbelgleichung gewonnen wurde, verglichen. Dabei hat es sich gezeigt, dass die Übereinstimmung der beiden vorhergesagten Änderungen sowohl untereinander, als auch mit der tatsächlich eingetroffenen Änderung recht gut ist. Offenbar kann man in einfachen Fällen die physikalischen Vorgänge in der Atmosphäre mittels der homogenen Wellengleichung beschreiben.
Summary The attempt is made to forecast height changes of the 500 mb contours by a numerical integration of the twodimensional homogenous wave equation provided the phase velocity is known. The result is compared with a forecast obtained by graphical integration of the barotropic vorticity equation. In the case investigated both methods show almost the same accuracy with respect to the contour changes with have actually occured. Appearently in some case it is possible to discribe height variations of an isobaric surface with the aid of the linear twodimensional wave equation with the same success as using the nonlinear vorticity equation.
  相似文献   

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