What is a lifting function and how is it used in fluid dynamics?

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SUMMARY

A lifting function is utilized in fluid dynamics, particularly in conjunction with the Navier-Stokes equation, to convert complex boundary conditions into a body force. This technique is essential for addressing non-standard boundary conditions that do not adhere to the non-slip condition. The discussion references foundational concepts such as Stokes' theorem and the divergence theorem, which are integral to understanding the application of lifting functions in fluid dynamics.

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  • Knowledge of the divergence theorem
  • Basic principles of fluid dynamics
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What is a "lifting function"?

Hi,

I was reading a journal article and they mentioned something called a "lifting function". It was apparently used with the Navier-Stokes equation to translate the boundary conditions (which were complicated, and NOT non-slip), into a body force.

It looks like think technique could be useful, so I wanted to find out what it was. The problem is that they reference given in the article was some lecture series from the 1950s, which I can't get a hold of.

So, could anyone here explain what a lifting function is, or hopefully point me to a good explanation?


(I notice that there is something called a lifting function used in topology, but I assume it's unrelated.)
 
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I don't recognize the term "lifting function" itself but such things as "Stoke's theorem":
[tex]\int_C \vec{f}\cdot \vec{ds}= \int\int_S \nabla\times\vec{f}\cdot\vec{dS}[/tex]
Where C is the one-dimensional boundary of the two-dimensional surface S
and the "divergence theorem"
[tex]\int\int_S \vec{F}\cdot\vec{dS}= \int\int\int_V \nabla\cdot\vec{F} dV[/itex]<br /> Where S is the two-dimensional surface of the three-dimensional region V seem to be what you are talking about.[/tex]
 


Thanks, HoI. The divergence theorem could well be what they meant.
 

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