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

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Section 7<br />

1) The Poisson distribution which corresponds to the homogeneous particle distribution<br />

[83]<br />

r<br />

µ<br />

P(<br />

r)<br />

= exp( −µ<br />

) , (7.9)<br />

r!<br />

where P(r) is the probability, µ the mean value <strong>of</strong> the number <strong>of</strong> particles per quadrat, <strong>and</strong> r a<br />

variable (the number <strong>of</strong> particles per quadrat);<br />

2) The negative binomial distribution which corresponds to the clustered particle<br />

distribution [83]<br />

85<br />

r<br />

⎛ ( k + r −1)!<br />

⎞⎛<br />

p ⎞ ⎛ 1 ⎞<br />

P( r)<br />

= ⎜ ⎟⎜<br />

⎟ ⎜ ⎟ , (7.10)<br />

⎝ ( k −1)!<br />

r!<br />

⎠⎝1<br />

+ p ⎠ ⎝1<br />

+ p ⎠<br />

where k <strong>and</strong> p are parameters determined according to [83].<br />

7.4. The effect <strong>of</strong> ECAP on the particle distribution, the <strong>global</strong> <strong>and</strong> <strong>local</strong> <strong>fracture</strong><br />

<strong>properties</strong> in MMCs with severe clustered particle distribution<br />

7.4.1. The effect <strong>of</strong> ECAP on the microstructure<br />

The uniformity <strong>of</strong> the particle distribution increases with the number <strong>of</strong> ECAP passes (Fig.<br />

7.4). For the as-fabricated MMC, clusters elongated in the extrusion direction are observed.<br />

The clusters have a size <strong>of</strong> up to 40 µm in the direction perpendicular to the extrusion<br />

direction. Large particle free zones, having a size <strong>of</strong> up to 200 µm in the extrusion direction<br />

<strong>and</strong> up to 40 µm in the perpendicular direction, are located between particle clusters (Fig.<br />

7.4a). From Fig. 7.5a, it is seen that the histogram corresponding to the particle distribution<br />

for the as-fabricated material seems to follow the negative binomial distribution indicating a<br />

clustering. After 4 ECAP passes, particle free zones become smaller <strong>and</strong> the particle clusters<br />

start to scatter (Fig. 7.4b). For this material condition, a deviation from the negative binomial<br />

distribution to the Poisson distribution can be noted in the histogram (Fig. 7.5b). Almost<br />

complete declustering <strong>and</strong> an absence <strong>of</strong> particle free zones are observed for the MMC after 7<br />

ECAP passes (Fig. 7.4c). The histogram <strong>of</strong> the particle distribution follows the Poisson<br />

distribution confirming the particle declustering, as well (Fig. 7.5c). Thus, these observations<br />

prove the validity <strong>of</strong> proposed Eq. 7.8.<br />

k

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