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“Influence of Si, Sb and Sr Additions on the Microstructure ...

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Chapter 4: Results <str<strong>on</strong>g>and</str<strong>on</strong>g> Discussi<strong>on</strong><br />

solid soluti<strong>on</strong> streng<strong>the</strong>ning to precipitati<strong>on</strong> hardening. Then prol<strong>on</strong>ged exposure<br />

leads to <strong>the</strong> coarsening <str<strong>on</strong>g>of</str<strong>on</strong>g> precipitates <str<strong>on</strong>g>and</str<strong>on</strong>g> it looses its ability to pin both <strong>the</strong><br />

dislocati<strong>on</strong>s <str<strong>on</strong>g>and</str<strong>on</strong>g> boundary. As it is clear that <strong>the</strong> Mg17Al12 precipitates has low<br />

melting point (43 7°C) <str<strong>on</strong>g>and</str<strong>on</strong>g> aluminum has higher diffusivity in magnesium, coarsening<br />

takes place very easily <str<strong>on</strong>g>and</str<strong>on</strong>g> faster. Moreover <strong>the</strong> decompositi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> Mg;7Al|; at grain<br />

boundary during elevated temperature exposure increases <strong>the</strong> aluminum c<strong>on</strong>tent in<br />

local areas. Subsequently this reduces <strong>the</strong> solidus temperature <str<strong>on</strong>g>and</str<strong>on</strong>g> hence increases <strong>the</strong><br />

homologous temperature [3l6]. This represents <strong>the</strong> tertiary stage <str<strong>on</strong>g>of</str<strong>on</strong>g> creep. As l<strong>on</strong>g as<br />

<strong>the</strong> hardening mechanism dominates <strong>the</strong> creep rate decreases. Whereas, when<br />

s<str<strong>on</strong>g>of</str<strong>on</strong>g>tening mechanisms become dominant, <strong>the</strong> creep rate increases. The minimum<br />

creep rate measured is <strong>the</strong> point <str<strong>on</strong>g>of</str<strong>on</strong>g> balance between hardening <str<strong>on</strong>g>and</str<strong>on</strong>g> s<str<strong>on</strong>g>of</str<strong>on</strong>g>tening<br />

mechanisms, which happens during sec<strong>on</strong>dary stage <str<strong>on</strong>g>of</str<strong>on</strong>g> creep.<br />

Apart from <strong>the</strong> coarsening effect, <strong>the</strong> massive Mg|-,Al12 particles are also<br />

involved in cavity formati<strong>on</strong>. Figure 4.63 also shows most <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> Mg]-;Al1;> particles<br />

suffer from sever cracking <str<strong>on</strong>g>and</str<strong>on</strong>g> cavity formati<strong>on</strong> at <strong>the</strong> matrix — precipitate interface.<br />

These cavities develop al<strong>on</strong>g <strong>the</strong> grain boundary since more coarse disc<strong>on</strong>tinuous<br />

precipitates are present in <strong>the</strong> grain boundary <str<strong>on</strong>g>and</str<strong>on</strong>g> finally introduce matrix cracking.<br />

One <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> major reas<strong>on</strong>s for <strong>the</strong> formati<strong>on</strong> cavity is <strong>the</strong> weak interface between<br />

matrix <str<strong>on</strong>g>and</str<strong>on</strong>g> Mg17Al12 intermetallic. It is well known that <strong>the</strong> crystallographic lattices<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> Mg matrix <str<strong>on</strong>g>and</str<strong>on</strong>g> Mg17Al|2 are different: <strong>the</strong> magnesium matrix has an hcp lattice,<br />

while <strong>the</strong> |3-MgnAl12 precipitates have a cubic lattice. It is also known that<br />

dislocati<strong>on</strong>s cannot pass as easily through hard precipitates as through <strong>the</strong> matrix. ln<br />

such cases pileups <str<strong>on</strong>g>of</str<strong>on</strong>g> dislocati<strong>on</strong>s near <strong>the</strong> precipitates lead to increase in local stress<br />

c<strong>on</strong>centrati<strong>on</strong> <str<strong>on</strong>g>and</str<strong>on</strong>g> resulted in cracking. Moreover cavity may forms at <strong>the</strong> grain<br />

boundary triple points. One such cavity at triple point in creep ruptured AZ91 alloy at<br />

150°C is shown in <strong>the</strong> Figure 4.65. According to Regev [29], <strong>the</strong> intergranular<br />

cavitati<strong>on</strong> <str<strong>on</strong>g>and</str<strong>on</strong>g> cracking also indirectly c<strong>on</strong>tributes to <strong>the</strong> s<str<strong>on</strong>g>of</str<strong>on</strong>g>tening process during<br />

creep. From dislocati<strong>on</strong> <strong>the</strong>ory, it is well known that cavitati<strong>on</strong> enables dislocati<strong>on</strong>s to<br />

leave <strong>the</strong> bulk <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> grain to <strong>the</strong> free surface without being blocked by obstacles. This<br />

prevents <strong>the</strong> activity <str<strong>on</strong>g>of</str<strong>on</strong>g> dislocati<strong>on</strong> sources <str<strong>on</strong>g>and</str<strong>on</strong>g> hence, <strong>the</strong> number <str<strong>on</strong>g>of</str<strong>on</strong>g> pileups is<br />

reduced [29].<br />

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