Deviance information criterion: Difference between revisions

From formulasearchengine
Jump to navigation Jump to search
No edit summary
 
en>Monkbot
Line 1: Line 1:
They contact me Emilia. South Dakota is exactly where me and my spouse reside. Hiring has been my profession for some time but I've already utilized for another 1. To gather coins is what her family and her appreciate.<br><br>Feel free to visit my web blog :: [http://www.siccus.net/blog/15356 at home std testing]
The '''Rankine vortex''' is a model of a [[vortex]] in a [[Viscosity|viscous]] fluid. A swirling flow in a viscous fluid can be characterized by a [[Vortex#Forced (rotational) vortex|forced vortex]] in its central core, surrounded by a [[free vortex]]. On the other hand, in an inviscid fluid the flow consists entirely of the free vortex with an infinite velocity at its center replacing the low velocity core. The tangential velocity<ref>{{cite book
  | title = Elementary Fluid Dynamics
  | author = D. J. Acheson
  | publisher = [[Oxford University Press]]
  | year = 1990
  | isbn = 0-19-859679-0
  }}</ref>
of a Rankine [[vortex]] with [[Circulation (fluid dynamics)|circulation]] <math>\Gamma</math> and radius <math>R</math> is
 
:<math>u_\theta(r) = \begin{cases} \Gamma r/(2 \pi R^2) & r \le R, \\ \Gamma/(2 \pi r) & r > R. \end{cases}</math>
 
The remainder of the velocity components are identically zero, so that the total velocity field is <math>\mathbf{u} = u_\theta\ \mathbf{e_\theta}</math>.
 
== See also ==
* [[Vortex]]
* [[Viscosity]]
* [[Wingtip vortices]]
 
==External links==
*[http://www.atmos.washington.edu/~durrand/animations/vort505/vortanim1.html Streamlines vs. Trajectories in a Translating Rankine Vortex]: an example of a Rankine vortex imposed on a constant velocity field, with animation.
 
==Notes==
{{reflist}}
 
[[Category:Equations of fluid dynamics]]
[[Category:Vortices]]
 
{{fluiddynamics-stub}}

Revision as of 18:04, 16 January 2014

The Rankine vortex is a model of a vortex in a viscous fluid. A swirling flow in a viscous fluid can be characterized by a forced vortex in its central core, surrounded by a free vortex. On the other hand, in an inviscid fluid the flow consists entirely of the free vortex with an infinite velocity at its center replacing the low velocity core. The tangential velocity[1] of a Rankine vortex with circulation Γ and radius R is

uθ(r)={Γr/(2πR2)rR,Γ/(2πr)r>R.

The remainder of the velocity components are identically zero, so that the total velocity field is u=uθeθ.

See also

External links

Notes

43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro.

Template:Fluiddynamics-stub

  1. 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

    My blog: http://www.primaboinca.com/view_profile.php?userid=5889534