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Computational engineering for wind-exposed thin-walled structures

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2 Ansgar Halfmann et al.<br />

large umbrellas (Fig. 1 [10]), the most demanding <strong>engineering</strong> task is to<br />

dimension the construction so that it will resist <strong>wind</strong> loads. Following the<br />

Davenport-Wind-Load-Chain an assumed local <strong>wind</strong> prole <strong>for</strong> a given terrain<br />

can be established according to the European Design Code EC 1 [5].<br />

This <strong>wind</strong> distribution causes a pressure eld on the structure. If simplied,<br />

conventional load assumptions <strong>for</strong> this pressure distribution are made, the<br />

<strong>structures</strong> may be strongly over-designed. Yet, also an under-design with the<br />

danger of a collapse may result from this simplied procedure, as the mutual<br />

inuence of neighbouring constructions could change the <strong>wind</strong> pressure eld<br />

dramatically. There<strong>for</strong>e, todays standard of practice are time-consuming and<br />

costly experiments in <strong>wind</strong> tunnels. A model of the construction is considered<br />

and <strong>wind</strong> pressure elds on its surface are measured to be used <strong>for</strong> later<br />

numerical structural analysis. One of the major drawbacks of this mixed computational<br />

and experimental approach is the diculty toquickly change the<br />

geometry of the model construction <strong>for</strong> the <strong>wind</strong> tunnel experiment. There<strong>for</strong>e,<br />

it would be highly desirable to have a'numerical <strong>wind</strong> tunnel' available,<br />

being directly integrated in the civil <strong>engineering</strong> design and analysis process,<br />

and enabling to investigate a structure also under the inuence of neighbouring<br />

constructions. Several steps in this direction have been per<strong>for</strong>med by the<br />

authors in a joint research project during the past two years and will be<br />

presented in this contribution.<br />

2 Software architecture<br />

The software architecture shown in Fig. 2 is inuenced by the idea of a loose<br />

coupling strategy based on highly specialized and well evaluated simulation<br />

codes, each developed <strong>for</strong> the special eld of the interacting system. In a<br />

rst step, the structural model is dened, using a classical CAD environment<br />

onaPCoraworkstation. Toconsider<br />

dierent stress distributions<br />

in a membrane, it is possible to<br />

compute the geometric shape of<br />

pure membrane <strong>structures</strong> in a<br />

<strong>for</strong>mnding process [2]. Thereby<br />

the de<strong>for</strong>med shape of the structure<br />

under dead load is computed<br />

by a nite element analysis starting<br />

from an inital geometry. Using<br />

special membrane elements<br />

and assuming an initial stiness<br />

caused by isotropic prestressing<br />

PC / workstation<br />

supercomputer<br />

STL-file<br />

ICEM-CFD<br />

fluid-simulation<br />

FASTEST-3D<br />

Geometrical Model<br />

+boundary conditions<br />

AutoCAD / SOFiPLUS<br />

<strong>for</strong>mfinding process<br />

MpCCI<br />

SOFiMESH<br />

DO_MESH<br />

structure-simulation<br />

ASE<br />

creates<br />

PC / workstation TECPLOT / Explorer Wingraf / Animator<br />

CDBASE<br />

Fig. 2. Software structure<br />

and neglecting any bending stiness, the de<strong>for</strong>med shape will lead to the<br />

soap lm <strong>for</strong>m with its constant isotropic stress distribution. All geometric<br />

in<strong>for</strong>mation is stored in a database describing a b-rep (boundary repre-

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