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Thixoforming : Semi-solid Metal Processing

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6<br />

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

Michael Modigell, Lars Pape, Ksenija Vasilic, Markus Hufschmidt, Gerhard Hirt,<br />

Hideki Shimahara, Rene Baadjou, Andreas B€uhrig-Polaczek, Carsten Afrath, Reiner Kopp,<br />

Mahmoud Ahmadein, and Matthias B€unck<br />

6.1<br />

Empirical Analysis of the Flow Behaviour<br />

In recent years, the demand for an industry-related and target-oriented enhancement<br />

of the semi-<strong>solid</strong> processing of metallic alloys and composites has grown. Until then,<br />

die design and process parameters such as holding time, pressure and piston velocity<br />

had been a matter of trial and error, because design rules from classical casting or<br />

forging cannot be transferred to thixoforming [1, 2].<br />

As mentioned in previous chapters, metallic alloys in the mushy state consist of<br />

<strong>solid</strong> particles suspended in a liquid matrix. Hence the flow behaviour is comparable<br />

to the one of classical suspensions and in principle the methods to evaluate and<br />

model the flow properties can be taken from classical suspension rheology. The main<br />

differences for metallic suspensions are related to changes in particle diameter due to<br />

Ostwald ripening (see Section 6.1.1) and non-isothermal effects such as <strong>solid</strong> fraction<br />

distribution during die filling (see Section 6.1.5).<br />

The flow properties of suspensions are shear-thinning and thixotropic. They depend<br />

on <strong>solid</strong> content, particle shape and particle diameter. Figure 6.1 shows the viscosity as<br />

a function of <strong>solid</strong> content for ideal particles, titanium oxide and soot. The shearthinning<br />

behaviour is displayed in Figure 6.2 for latex particles suspended in water.<br />

The shear-thinning and time-dependent flow properties of semi-<strong>solid</strong> metal alloys<br />

were first discovered by Flemings and co-workers [3] in the early 1970s for a lowmelting<br />

tin–lead alloy. Since then, numerous groups (e.g. [2, 4–9]) have determined<br />

the rheological characteristics experimentally and set up empirical models which are<br />

used for numerical simulation.<br />

The latest investigations concentrated on the flow properties of industrially<br />

relevant aluminium and steel alloys whose metallurgical characteristics are described<br />

in Chapter 2. In the following, we focus on the flow behaviour of the steel alloy<br />

A List of Symbols can be found at the end of<br />

this chapter.<br />

j169

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