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

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sizes <strong>of</strong> forces delivered to the crowns by the wire during<br />

deactivation, especially with a light leveling wire. <strong>The</strong><br />

authors concluded that careful ligation to minimize<br />

friction was important for delivery <strong>of</strong> expected force<br />

magnitudes. It is as early as placement <strong>of</strong> this initial<br />

wire that friction becomes a concern to the orthodontist.<br />

<strong>The</strong> classical laws <strong>of</strong> friction <strong>of</strong>fer only a partial<br />

explanation <strong>of</strong> friction in orthodontic systems. <strong>The</strong><br />

original theories by Amontons <strong>and</strong> Coulomb were derived from<br />

dry friction mechanics with distinct static <strong>and</strong> kinetic<br />

frictional phases, defined by zero velocity <strong>and</strong> constant<br />

velocity, respectively. Tooth movement in orthodontics,<br />

however, occurs at such low velocities, that these two<br />

phases are clinically interrelated. 3 Although the first two<br />

laws <strong>of</strong> friction would be unaffected by this application,<br />

the <strong>third</strong> law <strong>of</strong> friction may not accurately describe<br />

orthodontic friction in vivo. As the velocity <strong>of</strong> tooth<br />

movement approaches zero, instability in steady sliding is<br />

likely, due to interlocking <strong>and</strong> shearing <strong>of</strong> asperities, the<br />

peaks <strong>of</strong> microscopic surface irregularities. This effect<br />

is evident in the phenomenon known as “stick-slip motion”;<br />

a cycle involves a “stick state” where elastic loading<br />

occurs, <strong>and</strong> a “slip” where sudden sliding <strong>and</strong> stress-<br />

relaxation occur. 3,8 Nonetheless, Rossouw’s group 3 concluded<br />

8

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