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dissertation global and local fracture properties of metal matrix ...

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Section 2<br />

2.2. The influence <strong>of</strong> the <strong>global</strong> microstructure <strong>and</strong> the <strong>matrix</strong> condition on the <strong>global</strong><br />

mechanical <strong>properties</strong> in <strong>metal</strong> <strong>matrix</strong> composites<br />

The influence <strong>of</strong> the <strong>global</strong> microstructural parameters such as the particle volume fraction,<br />

the average particle size, etc., on the <strong>global</strong> mechanical <strong>properties</strong> has been already<br />

investigated in detail. The experimental results can be roughly generalized as follows [7]:<br />

With increasing particle volume fraction, the yield strength <strong>and</strong> the ultimate tensile strength<br />

increase, the ductility <strong>and</strong> the <strong>fracture</strong> toughness decrease, e.g., [8]. For a constant particle<br />

volume fraction, the tensile strength tends to increase with decreasing particle size, e.g.,<br />

[9,10]. No such simple pictures have been found for the more complex <strong>properties</strong> <strong>fracture</strong><br />

toughness <strong>and</strong> fatigue resistance; ambiguous results have been reported here [7, 11-12].<br />

Stronger <strong>matrix</strong> alloys produce stronger composites, e. g. [13,14]; the increase in strength due<br />

to the reinforcement decreases with increasing <strong>matrix</strong> strength; in the case <strong>of</strong> very high<br />

strength alloys, reinforcements may even lead to a reduction in strength [15]. Therefore, one<br />

<strong>of</strong> most important factors affecting the mechanical <strong>properties</strong> <strong>of</strong> MMCs is the heat treatment.<br />

In [16], the effect <strong>of</strong> the heat treatment on mechanical <strong>properties</strong> <strong>of</strong> the PM-MMC Al7093-<br />

15%SiC was investigated. An increase <strong>of</strong> the yield strength with increasing aging time up to<br />

the peak aged condition was found. A further increase <strong>of</strong> aging time led to a slight decrease <strong>of</strong><br />

the yield strength. The dependence <strong>of</strong> the <strong>fracture</strong> strain <strong>and</strong> the strain hardening coefficient<br />

on the aging time demonstrated an opposite character. A good correlation between the<br />

<strong>fracture</strong> strain <strong>and</strong> the strain hardening coefficient was found. It was shown that the <strong>fracture</strong><br />

toughness has an inverse dependence on strength <strong>and</strong> correlates well to the strain hardening<br />

coefficient. Fracture surface inspection revealed the dominance <strong>of</strong> the particle <strong>fracture</strong> for the<br />

solution treated, under-aged, peak-aged, <strong>and</strong> slightly over-aged conditions <strong>of</strong> the <strong>matrix</strong><br />

whereas, in the highly overaged condition, (near-)interface debonding failure dominated.<br />

In [17], a model was proposed to predict the <strong>fracture</strong> toughness in this material. This model is<br />

based on a prediction proposed by Hahn <strong>and</strong> Rosenfield [18],<br />

8<br />

1<br />

2<br />

1 ⎡<br />

⎤ 1<br />

3 −<br />

⎢ ⎛π<br />

⎞<br />

6<br />

= 2σ<br />

E⎜<br />

⎟ d⎥<br />

f . (2.1)<br />

⎢ ⎝ 6 ⎠ ⎥<br />

⎣<br />

⎦<br />

K IC<br />

y<br />

In Eq. 2.1 σy is the yield strength <strong>of</strong> material, E the Young modulus, d the particle size, <strong>and</strong> f<br />

the particle volume fraction. It was shown in [17] that Eq. 2.1 significantly overestimates the

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