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The effects of third-order torque and self - Saint Louis University

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steel wires could be a result <strong>of</strong> the relative roughness <strong>of</strong><br />

the contacting wire <strong>and</strong> slot surfaces. 5,18,23<br />

Kusy et al. 37 used a laser-spectrometer <strong>and</strong> the<br />

specular-reflectance technique to measure surface-<br />

roughnesses <strong>of</strong> wires <strong>of</strong> four materials, <strong>and</strong> found the<br />

surface <strong>of</strong> a nickel-titanium alloy wire to be the roughest<br />

followed, in <strong>order</strong>, by wire surfaces <strong>of</strong> ß-titanium,<br />

chromium-cobalt, <strong>and</strong> orthodontic stainless steel alloys.<br />

Using the same procedure, Kusy <strong>and</strong> Whitley 38 assessed the<br />

effect <strong>of</strong> surface topography on coefficients <strong>of</strong> friction<br />

for these alloys, <strong>and</strong> concluded that low wire surface<br />

roughness was not a sufficient condition for a small<br />

frictional coefficient. Prososki, Bagby <strong>and</strong> Erickson 11<br />

showed similar results, finding no statistically<br />

significant correlation between surface-roughness <strong>and</strong><br />

frictional resistance from as-received archwires <strong>of</strong> common<br />

alloys. Although the surface <strong>of</strong> a ß-titanium archwire is<br />

less rough than that <strong>of</strong> nickel-titanium alloys, researchers<br />

have consistently shown greater in-slot frictional<br />

resistance to sliding from the former wire. 11,24,38,39<br />

Burstone <strong>and</strong> Farzin-Nia 40 have suggested that the relative<br />

s<strong>of</strong>tness <strong>of</strong> the ß-titanium alloy wire-surface compared to<br />

the harder stainless steel surface is a reason for the<br />

former’s greater frictional resistance.<br />

12

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