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Thixoforming : Semi-solid Metal Processing

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200j 6 Modelling the Flow Behaviour of <strong>Semi</strong>-<strong>solid</strong> <strong>Metal</strong> Alloys<br />

equations in differential form are then integrated over each control volume. Interpolation<br />

profiles are then assumed in order to describe the variation of the concerned<br />

variable between cell centroids. The resulting equation is called the discretized or<br />

discretization equation. In this manner, the discretization equation expresses the<br />

conservation principle for the variable inside the control volume.<br />

The method is used in many computational fluid dynamics packages. The most<br />

compelling feature of the FVM is that the resulting solution satisfies the conservation<br />

of quantities such as mass, momentum, energy and species. This is exactly satisfied<br />

for any control volume and also for the whole computational domain and for any<br />

number of control volumes. Even a coarse grid solution exhibits exact integral<br />

balances. Therefore, FVM is the ideal method for computing discontinuous solutions<br />

arising in compressible flows. Since finite volume methods are conservative, they<br />

automatically satisfy the jump conditions and hence give physically correct weak<br />

solutions. FVM is also preferred while solving partial differential equations containing<br />

discontinuous coefficients.<br />

In the finite element method approach, the actual structure is assumed to be divided<br />

into a set of unstructured discrete subregions or elements which are interconnected<br />

only at a finite number of nodal points. The distinguishing feature of the finite<br />

element method is that the equations are multiplied by a weight function before they<br />

are integrated over the whole domain. The properties of the complete structure are<br />

found by evaluating the properties of the individual finite elements and superposing<br />

them appropriately. Due to the ability to model and solve large complicated structures<br />

and to deal with arbitrary geometries, the method is widely used in computational<br />

science.<br />

6.2.3<br />

Software Packages Used<br />

Within this work, the well-known commercial software packages FLUENT, Flow-3D<br />

and MAGMASOFT were used, in addition to the home-made numerical solver<br />

PETERA and LARSTRAN/SHAPE.<br />

. FLUENT is a CFD software package to simulate fluid flow problems. It uses the<br />

finite-volume method to solve the governing equations for a fluid. It provides the<br />

capability to use different physical models such as incompressible or compressible,<br />

inviscid or viscous, laminar or turbulent and so on. To determine the phase<br />

boundary in multiphase flows, and in particular free surface (or wave) flows, the<br />

so-called volume of fluid (VOF) model is used. Motion of fluid interfaces based on<br />

the solution of a conservative transport equation for the fractional volume of fluid<br />

in a grid cell is the method employed in FLUENT.<br />

. Flow-3D is a general-purpose CFD program with many capabilities, claiming to be<br />

particularly good for free surface flows. Finite-difference or finite-volume approximations<br />

to the equations of motion are used to compute the spatial and temporal<br />

evolution of the flow variables. In FLOW-3D, free surfaces are modelled with the<br />

VOF technique, incorporating some improvements beyond the original VOF

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