Graphical visualization of vortical flows by means of helicity

Helicity density and normalized helicity are introduced as important tools for the graphical representation of three-dimensional flowfields that contain concentrated vortices. The use of these two quantities filters out the flowfield regions of low vorticity, as well as regions of high vorticity but low speed where the angle between the velocity and vorticity vectors is large (such as in the boundary layer). Their use permits the researcher to identify and accentuate the concentrated vortices, differentiate between primary and secondary vortices, and mark their separation and reattachment lines. The method also allows locating singular points in the flowfield and tracing the vortex-core streamlines that emanate from them. Nomenclature H = helicity Hd = helicity density Hn — normalized helicity MOO = freestream Mach number ReD = Reynolds number V = velocity a = angle of attack co = vorticity

[1]  P. Glansdorff,et al.  On a general evolution criterion in macroscopic physics , 1964 .

[2]  H. K. Moffatt,et al.  The degree of knottedness of tangled vortex lines , 1969, Journal of Fluid Mechanics.

[3]  K. Wang Boundary layer over a blunt body at high incidence with an open-type of separation , 1974, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[4]  R. F. Warming,et al.  An implicit finite-difference algorithm for hyperbolic systems in conservation-law form. [application to Eulerian gasdynamic equations , 1976 .

[5]  J. Steger Implicit finite difference simulation of flow about arbitrary geometries with application to airfoils , 1977 .

[6]  R. F. Warming,et al.  An Implicit Factored Scheme for the Compressible Navier-Stokes Equations , 1977 .

[7]  I. Faux,et al.  Computational Geometry for Design and Manufacture , 1979 .

[8]  David J. Peake,et al.  Topology of Three-Dimensional Separated Flows , 1982 .

[9]  A. Tsinober,et al.  On the helical nature of three-dimensional coherent structures in turbulent flows , 1983 .

[10]  Arkady Tsinober,et al.  On the role of helical structures in three-dimensional turbulent flow , 1983 .

[11]  D. Degani Numerical Algorithm Conjugating Steady and Transient, Separated, Compressible Flow and a Solid Body Having Arbitrarily Distributed Heat Sources , 1984 .

[12]  P. G. Buning,et al.  Graphics and flow visualization in computational fluid dynamics , 1985 .

[13]  S. Orszag,et al.  On the role of helicity in complex fluid flows , 1985 .

[14]  R. Pelz,et al.  The helical nature of unforced turbulent flows , 1986 .

[15]  G. T. Chapman,et al.  Topological classification of flow separation on three-dimensional bodies , 1986 .

[16]  J. Lewalle On a variational property of helicity in incompressible flows , 1987 .

[17]  J. Steger,et al.  A numerical study of three-dimensional separated flow past a hemisphere cylinder , 1987 .

[18]  Lewis B. Schiff,et al.  Numerical prediction of subsonic turbulent flows over slender bodies at high incidence , 1991 .

[19]  Lewis B. Schiff,et al.  Computational investigation of a pneumatic forebody flow control concept , 1991 .

[20]  D. Degani,et al.  Effect of geometrical disturbance on vortex asymmetry , 1991 .

[21]  D. Degani,et al.  Effect of splitter plate on unsteady flows around a body of revolution at incidence , 1991 .

[22]  Yuval Levy,et al.  ASYMMETRIC TURBULENT VORTICAL FLOWS OVER SLENDER BODIES , 1992 .