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- From: a722756@roper.mc.ti.com (W. Donald Rolph)
- Subject: Re: Theory about Fluid-Structure ?
- Message-ID: <1993Jan21.131854@roper.mc.ti.com>
- Originator: a722756@roper.mc.ti.com
- Sender: usenet@pan.mc.ti.com (USENET News System)
- Organization: Texas Instruments / Attleboro Mass / USA
- References: <1993Jan21.115722.29874@dutrun2.tudelft.nl>
- Date: Thu, 21 Jan 1993 18:18:54 GMT
- Lines: 57
-
-
- In article <1993Jan21.115722.29874@dutrun2.tudelft.nl>, rcpshdb@dutrun2.tudelft.nl (Han de Bruijn) writes:
- |> In article <1993Jan20.120623.18611@dutrun2.tudelft.nl>, I wrote:
- |> > Wouldn't it help if people first _unify_ F.V. (fluid) and F.E. (solid)
- |> > methods?
- |>
- |> In article <1993Jan20.162622@roper.mc.ti.com> W. Donald Rolph (hi, Don!):
- |> > ................... (pardon Han!) the requirement here is that the shape or
- |> > trial functiosa [ he means: functions ] across the interface be compatible.
- |> > Under these conditions (oh well here we go again) the FV for the fluid
- |> > becomes essentially indistinguishable from FEA for the fluid, certainly at
- |> > the boundaries at least, and the problem easily reduces to a tractable form.
- |>
- |> Oh yeah? Let's take a combustion engine as an example. I have a the solid parts
- |> modeled with MARC, and the fluid parts modeled with PHOENICS. According to Don,
- |> it would be a "tractable" matter now to roast the beef.
- |>
- |> Or else, let's start from the basics: take some F.E. ingredients for the solid
- |> parts, take some F.V ingredients for the fluid parts. Then ... take a BIG MAMA,
- |> and "the problem easily reduces to a tractable form".
- |>
- |> One world or no world. Once F.V. and F.E. have been unified into ONE universal
- |> numerical method, the true practical problems will remain hard enough to solve.
- |> --
- |> * Han de Bruijn; Applications&Graphics | "A little bit of Physics * No
- |> * TUD Computing Centre; P.O. Box 354 | would be NO idleness in * Oil
- |> * 2600 AJ Delft; The Netherlands. | Mathematics" (HdB). * for
- |> * E-mail: Han.deBruijn@RC.TUDelft.NL --| Fax: +31 15 78 37 87 ----* Blood
-
- I agree completely with Han. I pose however, that at least at first pass, the fv
- formulation could be established for the fluid matched by trial functions to the
- solid with fea and in one single program solve the problem. Since as posed the
- variables would be continuous accross the boundary, the problem is indeed
- tractable, as for example Olsen and Bathe Journal of Computer and Structures 21,
- 1985.
-
- I still pose further, however, that properly posed the fea equations for the
- fluids themselves become indistinguishable form the fv equations for thes fluid
- themselves. Han you have brought up upwind differencing for the convective term
- before. I reference Zienkiewicz 1977 starting on page 633 where he discusses
- applying upwind differencing for the convective term using fea procedures. If
- these equations are consistent with your fv upwind differencing, then since you
- already conceded that for the pure diffusion problem fea and fv can reduce to the
- same form, a common ground would appear to exist.
-
- If the above paragraph sustains critical review, then my position is an even more
- optimistic one than yours, that is to say yes we need a merging of the two
- techniques - I agree completely, but further that the math to merge the two
- techniques already exists. ONE universal numercal method can be achieved today!
-
- You thoughts Han?
-
- --
-
- Regards.
-
- Don Rolph a722756@pan.mc.ti.com WD3 MS10-13 (508)-699-1263
-