I n discussing turbulent shear layers, experimentalists have divided the flow into a turbulent region, which is vortical, and a non-turbulent region, which is irrotational but unsteady. This paper introduces a theoretical method of decomposing the velocity field into potential and vortical components that is compatible with the experi-mentalists ’ viewpoint. Specifically, only potential motions will exist in the non-turbulent region, while the decomposition shows that the turbulent region consists of both potential and vortical motions. The kinematic decomposition used is called a potential/complex-lamellar decomposition. Compared with the standard Helmholtz decomposition, the complex-lamellar decomposition is not widely known, and this art...
The Burgers vortex (Burgers 1948) is described by an exact solution of the Navier-Stokes equations i...
We describe the general theory of anisotropic flow formation in quasi two- dimensional turbulence fr...
It has been shown [1, 2] that a wide class of 3D motions of in- compressible viscous fluid in Carte...
Methods of analyzing and interpreting velocity-field data (both two- and three-dimensional) to under...
The complexity of various Newtonian fluid flows encountered in nature and technology come from the c...
We consider incompressible Euler flows in terms of the stream function in two dimensions and the vec...
We consider incompressible Euler flows in terms of the stream function in two dimensions and the vec...
Theoretically, potential waves cannot generate the vortex motion, but scale considerations indicate ...
We discuss and compare different approaches to calculating the dynamics of anisotropic flow structur...
A theory is given to explain the observed dependence on Reynolds number of the decay of turbulent li...
ce a tion to predict the mean velocity. While the momentum equation is not unique due to the presenc...
We discuss and compare different approaches to calculating the dynamics of anisotropic flow structur...
The true problem of turbulence dynamics is the problem of its origin and successive development from...
The use of the complex velocity potential and the complex velocity is widely disseminated in the stu...
The role of energy and entropy in the decomposition of turbulent velocity flow-fields is shown in th...
The Burgers vortex (Burgers 1948) is described by an exact solution of the Navier-Stokes equations i...
We describe the general theory of anisotropic flow formation in quasi two- dimensional turbulence fr...
It has been shown [1, 2] that a wide class of 3D motions of in- compressible viscous fluid in Carte...
Methods of analyzing and interpreting velocity-field data (both two- and three-dimensional) to under...
The complexity of various Newtonian fluid flows encountered in nature and technology come from the c...
We consider incompressible Euler flows in terms of the stream function in two dimensions and the vec...
We consider incompressible Euler flows in terms of the stream function in two dimensions and the vec...
Theoretically, potential waves cannot generate the vortex motion, but scale considerations indicate ...
We discuss and compare different approaches to calculating the dynamics of anisotropic flow structur...
A theory is given to explain the observed dependence on Reynolds number of the decay of turbulent li...
ce a tion to predict the mean velocity. While the momentum equation is not unique due to the presenc...
We discuss and compare different approaches to calculating the dynamics of anisotropic flow structur...
The true problem of turbulence dynamics is the problem of its origin and successive development from...
The use of the complex velocity potential and the complex velocity is widely disseminated in the stu...
The role of energy and entropy in the decomposition of turbulent velocity flow-fields is shown in th...
The Burgers vortex (Burgers 1948) is described by an exact solution of the Navier-Stokes equations i...
We describe the general theory of anisotropic flow formation in quasi two- dimensional turbulence fr...
It has been shown [1, 2] that a wide class of 3D motions of in- compressible viscous fluid in Carte...