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Thixoforming : Semi-solid Metal Processing

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are the strain rate concentration tensors associated with the liquid and <strong>solid</strong> particles,<br />

respectively. The overall response, namely the overall stresses, is calculated by<br />

averaging conditions on stresses:<br />

SB ¼ f s<br />

Bss s<br />

B þ 1 f B slB Introducing local constitutive equations and concentrations relations leads to<br />

SB ¼ f s<br />

Bss s<br />

B þ 1 f B sl B<br />

ð7:15Þ<br />

ð7:16Þ<br />

SB ¼ f s<br />

BmsB T s s<br />

B þ 1 f B mlB T l B _ EB ð7:17Þ<br />

The effective viscosity is thus defined by the following implicit equation:<br />

m B ¼ f s<br />

B ms B<br />

5m B<br />

3mB þ 2ms þ 1 f<br />

B<br />

s<br />

B ml B<br />

5m B<br />

3m B þ 2m l B<br />

ð7:18Þ<br />

7.3.2.2 Step b<br />

As done previously, the mechanical interactions between the coated inclusions are<br />

solved by a self-consistent scheme. However, the mathematical form of the strain<br />

rate concentration tensors is different from that given in Equations 7.13 and 7.14<br />

because now we have to account for the specific spatial distribution of the inclusion<br />

and the active zone. In other words, we have to account for the fact that the inclusion<br />

is surrounded by the active zone. Following the work of Christensen and Lo [27] and<br />

Cherkaoui et al. [28], the effective viscosity mSS of the semi-<strong>solid</strong> is thus determined by<br />

the following equation:<br />

where<br />

mSS ¼ f AmAT A þ f ImIT I ¼ mA þ f IðmImAÞTI ð7:19Þ<br />

T I ¼<br />

3m SS þ 2m I þ 1 f I<br />

f I<br />

5m SS<br />

6<br />

5 mI m ð AÞ<br />

mSS mA 1<br />

ð7:20Þ<br />

where f I ¼ R3 = ðRþDRÞ 3 , R being the radius of the spherical inclusion and DR the<br />

thickness of the coating.<br />

7.4<br />

Results and Discussion<br />

7.4.1<br />

Isothermal Steady-state Behaviour<br />

7.4 Results and Discussionj229<br />

In this section, the micro–macro model is applied to the case of Sn–15wt%Pb alloys<br />

having a globular-like morphology for the <strong>solid</strong> phase and <strong>solid</strong> fractions ranging<br />

from 0.4 to 0.7. Calculations are compared with experimental results found in the

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