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use of metal templates for microcavity formation in alumina

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addition, the cavity <strong>for</strong>mation is considered to be the result <strong>of</strong> the Kirkendall effect,<br />

where due to the dom<strong>in</strong>at<strong>in</strong>g diffusion conditions, the Kirkendall porosity l<strong>in</strong>e foc<strong>use</strong>s<br />

on the center <strong>of</strong> the Ti wire rather than at the boundary between the Ti and alum<strong>in</strong>a<br />

samples. As a result <strong>of</strong> EDS analysis <strong>of</strong> the samples, Al and Ti are seen <strong>in</strong> the diffusion<br />

region, and an <strong>in</strong>termediate phase <strong>of</strong> Al2TiO5 is <strong>for</strong>med <strong>in</strong> the middle <strong>of</strong> the diffusion<br />

region.<br />

Accord<strong>in</strong>g to SEM observation <strong>of</strong> the alum<strong>in</strong>a samples, which <strong>use</strong>d sta<strong>in</strong>less<br />

steel wire, it is noticed that the sta<strong>in</strong>less steel has wholly diff<strong>use</strong>d <strong>in</strong>to the alum<strong>in</strong>a and<br />

this diffusion region is approximately 100µm.<br />

S<strong>in</strong>tered microstructure <strong>of</strong> the alum<strong>in</strong>a sample, which <strong>use</strong>d copper wire, was<br />

exam<strong>in</strong>ed from polished surfaces. Accord<strong>in</strong>g to EDS analysis <strong>of</strong> the sample, Al and O is<br />

<strong>in</strong> the alum<strong>in</strong>a matrix while Cu is not. At 1350 o C, copper has almost completely<br />

melted.<br />

Titanium plate is sandwiched between two alum<strong>in</strong>a pellets <strong>in</strong> the diffusion<br />

couple test and the diffusion after s<strong>in</strong>ter<strong>in</strong>g was exam<strong>in</strong>ed. As a result <strong>of</strong> SEM<br />

observation <strong>of</strong> the sample, it is observed that approximately 130µm expansion <strong>for</strong><br />

titanium <strong>in</strong> alum<strong>in</strong>a occurred while 4 hours soak<strong>in</strong>g time. The Kirkendall porosity by<br />

Ti +4 diffus<strong>in</strong>g through the fundamentally tough and motionless oxygen sublattice with<strong>in</strong><br />

the TiO2 and <strong>in</strong>to the surround<strong>in</strong>g Al2O3 without an equal and opposite flux <strong>of</strong> Al +3 to<br />

balance it, is probably the reason <strong>for</strong> observed porosity. In these particular<br />

circumstances, the Kirkendall porosity is consolidated <strong>in</strong>to a cont<strong>in</strong>uous cavity rather<br />

than distributed pores (Goodshaw et al., 2009). Observations <strong>of</strong> the concentration <strong>of</strong><br />

Kirkendall porosity <strong>in</strong>to cont<strong>in</strong>uous cavities appear to have been first reported by<br />

Ald<strong>in</strong>ger (Ald<strong>in</strong>ger, 1974).<br />

In this thesis, the gr<strong>in</strong>d<strong>in</strong>g process is not applied to the alum<strong>in</strong>a powders. As a<br />

result <strong>of</strong> this, <strong>microcavity</strong> <strong>for</strong>mation was not observed after titanium diffusion <strong>in</strong>to<br />

alum<strong>in</strong>a. As a further study, if the gr<strong>in</strong>d<strong>in</strong>g process is applied to alum<strong>in</strong>a powders <strong>for</strong><br />

long periods, it can be expected that micro-cavity <strong>for</strong>mation would be provided with<strong>in</strong><br />

the alum<strong>in</strong>a matrix by us<strong>in</strong>g titanium <strong>templates</strong>. In addition to that, the mechanism and<br />

k<strong>in</strong>etics <strong>of</strong> cavity <strong>for</strong>mation can be <strong>in</strong>vestigated further.<br />

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