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Thixoforming : Semi-solid Metal Processing

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and liquid are both assumed to be isotropic and incompressible so that their flow<br />

behaviour can be expressed by means of a single modulus, namely the viscosity m,by<br />

the following equations:<br />

s l ij ¼ 2ml _eij with m l ¼ K l<br />

s s ij ¼ 2ms _eeq _eij with m s ¼ K s _eeq<br />

for the Newtonian liquid ð7:8Þ<br />

m 1<br />

for the viscoplastic <strong>solid</strong> ð7:9Þ<br />

where the superscripts l and s refer to the liquid and <strong>solid</strong> phase, respectively, sij is the<br />

deviatoric stress tensor, _eij is the deviatoric strain rate tensor, K is the consistency and<br />

m is the strain rate sensitivity parameter.<br />

Actually, one may distinguish the constitutive equation for the entrapped and nonentrapped<br />

liquid and for the <strong>solid</strong> particles and the <strong>solid</strong> bonds by using different<br />

values for the consistency and the strain rate sensitivity parameter. In the following<br />

sections, as a first approximation, we assume that the entrapped and non-entrapped<br />

liquids have the same properties. Concerning the <strong>solid</strong> phase, we assume that the<br />

consistencies of the <strong>solid</strong> bonds and the <strong>solid</strong> particles are different. This choice<br />

implies that the strength of the <strong>solid</strong> bonds may be adjusted to account for the effect<br />

of rest time or temperature on the semi-<strong>solid</strong> microstructure and mechanical<br />

features.<br />

7.3.2<br />

Homogenized Estimate of the <strong>Semi</strong>-<strong>solid</strong> Viscosity: Concentration<br />

and Homogenization Steps<br />

As illustrated in Figure 7.2 and discussed previously, the semi-<strong>solid</strong> is represented by<br />

a spherical coated inclusion . The inclusion and the coating, also called the active<br />

zone, are both composed of liquid and <strong>solid</strong>. Therefore, the determination of the<br />

effective properties of the semi-<strong>solid</strong> requires first the evaluation of the overall<br />

behaviour of the inclusion and of the coating from the behaviour of the <strong>solid</strong> and<br />

liquid phases. The effective viscosity mSS of the coated inclusion, representing the<br />

semi-<strong>solid</strong> material, is then determined from the previous results. To do so, we use<br />

the self-consistent approximation. This approach implies that each particle of liquid<br />

(<strong>solid</strong> or coated inclusion) feels the surroundings (i.e. the neighbouring particles)<br />

through a fictitious homogeneous medium having the effective properties of the<br />

heterogeneous material (Figure 7.4).<br />

7.3.2.1 Step a<br />

The effective viscosities of the inclusion and the active zone are defined by<br />

Equation 7.10 using the same formalism as for local behaviours (Equation 7.9):<br />

SB ¼ 2m B _ EB<br />

7.3 Modelling <strong>Semi</strong>-<strong>solid</strong> Behaviourj227<br />

ð7:10Þ<br />

The suffix B is equal to I when it refers to the inclusion and to A for the active zone.<br />

S B and _ EB are the overall stress and strain rate tensors of the medium B. We assume<br />

that the medium B is submitted to boundary conditions _ EB. It is now required to

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