Characterization and control of the fiber-matrix interface in ceramic ...
Characterization and control of the fiber-matrix interface in ceramic ...
Characterization and control of the fiber-matrix interface in ceramic ...
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148<br />
The resultant <strong>fiber</strong>s are composed <strong>of</strong> approximately 55 wt %<br />
silicon,<br />
30 wt % carbon, <strong>and</strong> 15 wt % oxygen. These elements are present as<br />
60 wt % /?-Sic, 30 wt % amorphous Si02, <strong>and</strong> 10 wt % amorphous free carbon,<br />
<strong>and</strong> <strong>the</strong> <strong>fiber</strong>s have a measured density <strong>of</strong> 2.55 g/cm3. The oxygen content<br />
is a consequence <strong>of</strong> <strong>the</strong> cur<strong>in</strong>g cycle <strong>and</strong> is partially responsible for <strong>the</strong><br />
<strong>the</strong>rmal <strong>in</strong>stability <strong>of</strong> <strong>the</strong> Nicalon Si-C-0 <strong>fiber</strong>s.<br />
The mechanisms <strong>of</strong> <strong>fiber</strong> degradation have been a topic <strong>of</strong> debate<br />
for a number <strong>of</strong> years (119-135).<br />
The manufacturer quotes a strength <strong>of</strong><br />
2500 MPa for <strong>the</strong> material; however, extensive evaluation has shown <strong>the</strong><br />
ultimate strength <strong>of</strong> <strong>fiber</strong> tows to be about 2100 MPa (see Table 10.3).<br />
Heat<strong>in</strong>g <strong>the</strong> <strong>fiber</strong>s <strong>in</strong> any atmosphere to temperatures above 1075 K results<br />
<strong>in</strong> a reduction <strong>in</strong> <strong>fiber</strong> strength. This is <strong>the</strong> major disadvantage <strong>of</strong> <strong>the</strong><br />
Nicalon <strong>fiber</strong>s, <strong>and</strong> this degradation <strong>of</strong> properties has been attributed to<br />
factors such as gra<strong>in</strong> growth, carbo<strong>the</strong>rmal reduction <strong>of</strong> Si02 to form Sic<br />
<strong>and</strong> CO gas, composition changes, etc.<br />
The composition <strong>and</strong> structure <strong>of</strong> <strong>the</strong> <strong>fiber</strong>s have been analyzed us<strong>in</strong>g<br />
many analytical techniques (119-134). From <strong>the</strong> <strong>in</strong>vestigations, <strong>the</strong><br />
<strong>fiber</strong>s appear to be composed <strong>of</strong> ultraf<strong>in</strong>e 1.7-nm gra<strong>in</strong>s <strong>of</strong> /?-Sic bonded<br />
toge<strong>the</strong>r by an amorphous silica <strong>matrix</strong>. Nuclear magnetic resonance has<br />
revealed <strong>the</strong> presence <strong>of</strong> bond<strong>in</strong>g that is characteristic <strong>of</strong> silicon<br />
oxycarbide, suggest<strong>in</strong>g that this material acts as a transition layer at<br />
<strong>the</strong> surface <strong>of</strong> <strong>the</strong> gra<strong>in</strong>s. O<strong>the</strong>rs (135) have also hypo<strong>the</strong>sized that <strong>the</strong><br />
Sic particles are surrounded by a carbon layer. Regardless, <strong>the</strong> Nicalon<br />
<strong>fiber</strong>s are damaged by heat<strong>in</strong>g to elevated temperatures, <strong>and</strong> many factors<br />
exacerbate <strong>the</strong> problem. The strength <strong>of</strong> Nicalon <strong>fiber</strong>s subjected to a<br />
variety <strong>of</strong> treatments was given <strong>in</strong> Table 10.3.