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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 11 (1999), S. 1512-1520 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Using a novel numerical method at unprecedented resolution, we demonstrate that structures of small to intermediate scale in rotating, stratified flows are intrinsically three-dimensional. Such flows are characterized by vortices (spinning volumes of fluid), regions of large vorticity gradients, and filamentary structures at all scales. It is found that such structures have predominantly three-dimensional dynamics below a horizontal scale L(approximate)〈fraction SHAPE="CASE"〉12LR, where LR is the so-called Rossby radius of deformation, equal to the characteristic vertical scale of the fluid H divided by the ratio of the rotational and buoyancy frequencies f/N. The breakdown of two-dimensional dynamics at these scales is attributed to the so-called "tall-column instability" [D. G. Dritschel and M. de la Torre Juárez, J. Fluid. Mech. 328, 129 (1996)], which is active on columnar vortices that are tall after scaling by f/N, or, equivalently, that are narrow compared with LR. Moreover, this instability eventually leads to a simple relationship between typical vertical and horizontal scales: for each vertical wave number (apart from the vertically averaged, barotropic component of the flow) the average horizontal wave number is equal to f/N times the vertical wave number. The practical implication is that three-dimensional modeling is essential to capture the behavior of rotating, stratified fluids. Two-dimensional models are not valid for scales below LR. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 5 (1993), S. 173-186 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A new computational method extending the contour dynamics/surgery (CS) algorithm is announced which gives typical speed-up factors of two orders of magnitude in calculations of flows involving many interacting vortices. The method makes use of an alternative expression for the velocity field in the exterior of a vortex that takes the form of a rapidly convergent series. Each term in this series can be expressed as a complex coefficient divided by the complex distance x+iy from the vortex center. The complex coefficient, or moment, is a real number pair that describes shape characteristics of the vortex (e.g., circulation, eccentricity, etc.). In numerical calculations, where accuracy is necessarily limited, it is frequently sufficient to retain only the leading-order terms in this series, particularly for a gas of well-separated vortices. The real computational gain is made, however, by reexpanding the series of all vortices that are sufficiently separated from a given vortex as a single, truncated series in positive powers of the complex distance from this vortex's center. The coefficients of this series involve only the moments of the other vortices and their centroid separation from the given vortex. The leading-order truncation, for instance, simply gives point vortex dynamics, except that self- or close-range interactions are computed using the full contour integral expression of contour dynamics (hence, all vortices retain nontrivial spatial structure, vital to a proper dynamical description of close-range interactions). In general, the optimal truncation depends on a dynamic balance between the cost of all moment computations and the cost of all contour integrations. This method, called "moment-accelerated contour surgery,'' which is briefly outlined above for the planar case, has a direct analog in spherical geometry. There are also extensions to generalized two-dimensional (2-D) flows having more general linear operator relationships between streamfunction and vorticity. Details are provided for quasigeostrophic flow.
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  • 3
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 5 (1993), S. 984-997 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Novel physical-space vortex properties of nearly inviscid, unforced two-dimensional (2-D) turbulence are presented. They are obtained from the analysis of a large ensemble of calculations all beginning with a random distribution of vortex patches of equal vorticity magnitude on a spherical surface. The numerical method (MACS) is a combination of contour dynamics/surgery (CD/CS) and a moment expansion for calculating separated vortex interactions. This method calculates approximately 100 times faster than CD/CS thereby permitting the formation of a large database for obtaining meaningful statistics. The numerical method can resolve a much wider range of spatial scales than conventional (pseudospectral) methods, and it is found that the statistical vortex properties produced differ in significant respects from those obtained previously. This conclusion is drawn from not just one set of calculations, but three at different spatial resolutions. While algebraic decay of basic flow statistics (e.g., enstrophy, vortex population) is observed at late times, the decay exponents are smaller than previously obtained and furthermore do not come in the ratios suggested by the recently proposed "universal scaling theory.'' In addition, the vortex number density distribution is not found to be self-similar but steepens continuously and appreciably with decreasing vortex size. This forces a reevaluation of the nature of 2-D turbulence in the inviscid limit. A proper description of this limit needs (more) quantitative information concerning the most probable vortex interactions. Such interactions will not be between just two vortices, as is commonly supposed.
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  • 4
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 3 (1991), S. 855-869 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In Part I [Phys. Fluids A 3, (square, solid)(square, solid)(square, solid) (1991)] approximate equations were developed describing the basic evolution of vortices in a general strain field. These equations take the form of a set of coupled, nonlinear ordinary differential equations describing the time evolution of the centroids, aspect ratios, and orientations of a nested set of elliptical contours representing each vortex. Here, in Part II, the model is extended to include disturbances to the elliptical shape of each contour, disturbances that are excited naturally by the interaction with other vortices. This interaction is worked out explicitly for the first time. The final equations obtained decouple into sets of equations for each mode symmetry, allowing for a very simple description of the disturbance evolution. Numerical tests show remarkable agreement between the elliptical model and the full equations of motion in four problems: (1) the equilibrium contour shapes of a multicontour family of vortices, (2) the linear stability of this family, (3) the equilibrium, nonelliptical shapes of two corotating vortex patches, and (4) the interaction between two symmetrical vortex patches, including merging.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 8 (1996), S. 1252-1256 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A powerful feature-tracking tool is applied to several high-resolution, very long-duration, regularized contour dynamics (contour surgery) simulations of unforced nearly-inviscid two-dimensional turbulence (2DT) on the surface of a sphere. Particularly low density gases of vortices (i.e. on average, very widely separated vortices) are examined to ascertain the nature of their interactions. The simplest (minimal) model system is studied, namely a set of vortex patches of just two vorticity values, ±ω0, whose total circulation is zero. The areas of the patches are selected initially from a pre-assigned, stable (nearly time invariant) power-law distribution. When the vorticity occupation fraction f(approximately-greater-than)0.01, often more than three vortices are found relatively close together at the onset of a strong interaction. But, when f(approximately-less-than)0.01, all such interactions involve only three nearby vortex patches, not all having the same sign of vorticity. This is related to the well-known collapse of three singular (point) vortices. Thus, under these conditions, isolated two-vortex interactions, which have figured in recent ad hoc theories and models for decaying 2DT, cannot occur. Taking into account these results, we propose an asymptotically-motivated and computationally-efficient "reduced'' model. © 1996 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 3954-3962 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This paper studies the erosion of a monotonically distributed vortex by the joint action of inviscid stripping, induced by an externally imposed adverse shear, and viscous diffusion, either in the form of Newtonian viscosity or hyperviscosity. It is shown that vortex erosion is greatly amplified by the presence of diffusion; abrupt vortex breakup or gradual quasi-equilibrium evolution depend crucially on the strain to peak vorticity ratio and on the Reynolds number. Peculiar, unexpected effects are observed when hyperviscosity is used in place of Newtonian viscosity. © 1994 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 3 (1991), S. 845-854 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An approximate model of nonaxisymmetric vortices in a two-dimensional fluid is developed in which each vortex is assumed to consist of a nested stack of elliptical regions of uniform vorticity. The model is governed by a set of coupled nonlinear ordinary differential equations for the aspect ratio, orientation, and centroid of the bounding contour of each region. It also admits a Hamiltonian formulation and possesses all the invariants of the original system. In Part II [Phys. Fluids A 3, XXX (1991)], the model is extended to include disturbances to the elliptical shape of each contour.
    Type of Medium: Electronic Resource
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  • 8
    Publication Date: 2018-03-01
    Print ISSN: 0043-1397
    Electronic ISSN: 1944-7973
    Topics: Architecture, Civil Engineering, Surveying , Geography
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  • 9
    Publication Date: 2016-06-10
    Description: The diabatic contour-advective semi-Lagrangian (DCASL) algorithms previously constructed for the shallow-water and multilayer Boussinesq primitive equations are extended to multilayer non-Boussinesq equations on the sphere using a hybrid terrain-following–isentropic (σ–θ) vertical coordinate. It is shown that the DCASL algorithms face challenges beyond more conventional algorithms in that various types of damping, filtering, and regularization are required for computational stability, and the nonlinearity of the hydrostatic equation in the σ–θ coordinate causes convergence problems with setting up a semi-implicit time-stepping scheme to reduce computational cost. The prognostic variables are an approximation to the Rossby–Ertel potential vorticity Q, a scaled pressure thickness, the horizontal divergence, and the surface potential temperature. Results from the DCASL algorithm in two formulations of the σ–θ coordinate, differing only in the rate at which the vertical coordinate tends to θ with increasing height, are assessed using the baroclinic instability test case introduced by Jablonowski and Williamson in 2006. The assessment is based on comparisons with available reference solutions as well as results from two other algorithms derived from the DCASL algorithm: one with a semi-Lagrangian solution for Q and another with an Eulerian grid-based solution procedure with relative vorticity replacing Q as the prognostic variable. It is shown that at intermediate resolutions, results comparable to the reference solutions can be obtained.
    Print ISSN: 0027-0644
    Electronic ISSN: 1520-0493
    Topics: Geography , Geosciences , Physics
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  • 10
    Publication Date: 1993-04-01
    Print ISSN: 0899-8213
    Topics: Physics
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