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An experimental investigation of spin-up from rest of a stratified fluid

机译:剩余分层流体中自旋的实验研究

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We examine the spin-up from rest of a stratified fluid with initial Brunt-Vaisala frequency N bound within a cylindrical container of height 2H and radius R which is set to rotate impulsively with angular speed f/2. Particular attention is given to characterizing the dependence of the form of the resulting flow on the governing parameters. Our experimental study reveals a wealth of flow behaviours and instabilities. In all experiments, the initial phase of motion is marked by the establishment of mixed axisymmetric corner regions fed by radial Ekman transport, a process detailed in Flor et al. (Flor, J.B., Ungarish, M. and Bush, J.W.M., "Spin-up from rest of a stratified fluid: boundary flows'', J. Fluid Mech., 472, 51-82 (2002).).The subsequent evolution of the central vortex depends critically on the Burger number B-core=NcH/(fR), where N-c=N(1-0.2B(-1))(1/2) is the buoyancy frequency of the central core following the establishment of the corner regions. For B>1.0, the axisymmetry of the system is retained throughout the spin-up process: the central vortex attains a state of near solid body rotation by the diffusion of vorticity from the sidewalls. For B<1.0, the central core becomes baroclinically unstable, and its streamlines strained from circles into ellipses. Subsequently, for N-c/f<1 (and B<1.0), the symmetry of the central core is broken in a manner reminiscent of the elliptical instability. For short tanks (2H/R<1), the instability is marked by a simple tip-over of the central core in the laboratory frame that is resisted by the core stratification. For 2H/R>1, the centreline of the stratified core is deflected into a helical form before the core breaks into a series of stacked vortices. A Burger number criterion, B=NH/(fR)<1.0, for the baroclinic instability of the central core is derived and found to be consistent with the experimental observations.
机译:我们检查了剩余层状流体的自旋,其初始Brunt-Vaisala频率N限制在高度为2H且半径为R的圆柱容器中,该容器设置为以角速度f / 2脉冲旋转。要特别注意表征结果流的形式对控制参数的依赖性。我们的实验研究揭示了许多流动行为和不稳定性。在所有实验中,运动的初始阶段都以通过径向埃克曼输运为基础的混合轴对称角区域的建立为标志,这一过程在Flor等人的论文中有详细介绍。 (Flor,JB,Ungarish,M。和Bush,JWM,“从其余分层流体中旋转:边界流”,J。Fluid Mech。,472,51-82(2002)。)。中心涡的强度主要取决于汉堡数B-core = NcH /(fR),其中Nc = N(1-0.2B(-1))(1/2)是建立后中心核的浮力频率对于B> 1.0,在整个旋转过程中,系统的轴对称性得以保留:中心涡旋通过侧壁上涡旋的扩散而达到接近固体旋转的状态;对于B <1.0,则B中心核变得斜压不稳定,并且它的流线从圆弧形变为椭圆形,随后,对于Nc / f <1(且B <1.0),中心核的对称性以椭圆不稳定的方式被打破。 (2H / R <1),不稳定性的特征是中心框架在中心框架上的简单翻倒,但被核心分层所抵制。对于2H / R> 1,在核心分裂成一系列堆叠的涡流之前,分层核心的中心线会偏转为螺旋形式。推导了用于中央核的斜压不稳定性的Burger数准则,B = NH /(fR)<1.0,并发现与实验观察结果一致。

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