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

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Section 4<br />

4.2. The effect <strong>of</strong> the heat treatment on the mechanism <strong>of</strong> void initiation<br />

The <strong>fracture</strong> surfaces <strong>of</strong> the MMCs are studied in detail in the SEM LEO 440. The regions<br />

near the crack front in the mid-section <strong>of</strong> the specimens, where plane-strain condition<br />

prevails, are investigated. Ductile <strong>fracture</strong> by micro-void coalescence is observed in all<br />

materials.<br />

The images <strong>of</strong> the analysed regions for all investigated materials are given in Appendix 9<br />

(Figs. 9.1-9.25). For each investigated material, from 10 to 20 particles located closely in<br />

front <strong>of</strong> the crack tip are investigated. For each particle, the mechanism <strong>of</strong> void initiation<br />

either particle <strong>fracture</strong> or particle/<strong>matrix</strong> decohesion is determined from stereo image pairs.<br />

For instance, when the particle is observed only on a single half <strong>of</strong> the broken specimen, it is<br />

probable that the particle/<strong>matrix</strong> decohesion has occurred. On the contrary, if broken parts <strong>of</strong><br />

a particle are found on both specimen halves, particle <strong>fracture</strong> can be assumed.<br />

The study <strong>of</strong> the <strong>fracture</strong> surfaces <strong>of</strong> the casdt MMCs reveals a change <strong>of</strong> the mechanism <strong>of</strong><br />

void nucleation with increasing aging condition: a clear tendency to increasing probability <strong>of</strong><br />

particle/<strong>matrix</strong> decohesion mechanism can be noted (see Table 4.8 on p. 65). For instance, in<br />

Specimen Al2O3-10%-200h, 12 <strong>of</strong> 15 considered particles formed dimple by particle/<strong>matrix</strong><br />

decohesion, whereas in Specimen Al2O3-10%-RT, 13 <strong>of</strong> 16 considered particles are <strong>fracture</strong>d.<br />

Although only particles near the crack front are considered in this statistic, these data reflect<br />

the situation on whole <strong>fracture</strong> surface, as well.<br />

In Fig. 4.10a, a typical broken alumina particle is shown (Particle 4 <strong>of</strong> Specimen Al2O3-10-RT<br />

from Fig. 9.1 taken at higher magnification). It is seen that the particle <strong>fracture</strong> surface has a<br />

smooth view. Fig. 4.10b shows a debonded particle 13 in Specimen Al2O3-10-200h. The<br />

particle/<strong>matrix</strong> interface is rough <strong>and</strong> bumpy: very small dimples having a size less than 1 µm<br />

are observed at the debonded interface. These small dimples are initiated by the MgAl2O4<br />

spinel phases formed at the alumina particle/<strong>matrix</strong> interface [21, 71-72]. It has been<br />

suggested that the spinel phase can be formed at the interface both during the fabrication <strong>of</strong><br />

MMCs <strong>and</strong> during the following heat treatment. The following possible reactions with large<br />

enough thermodynamic driving forces to form the MgAl2O4 phase have been proposed in<br />

[71]:<br />

40

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