Effect of wire size on maxillary arch force/couple systems for a simulated high canine malocclusion

To better understand the effects of copper nickel titanium (CuNiTi) archwire size on bracket-archwire mechanics through the analysis of force/couple distributions along the maxillary arch. The hypothesis is that wire size is linearly related to the forces and moments produced along the arch. An Orth...

Full description

Saved in:
Bibliographic Details
Published inJournal of orthodontics Vol. 41; no. 4; p. 285
Main Authors Major, Paul W, Toogood, Roger W, Badawi, Hisham M, Carey, Jason P, Seru, Surbhi
Format Journal Article
LanguageEnglish
Published England 01.12.2014
Subjects
Online AccessGet more information

Cover

Loading…
More Information
Summary:To better understand the effects of copper nickel titanium (CuNiTi) archwire size on bracket-archwire mechanics through the analysis of force/couple distributions along the maxillary arch. The hypothesis is that wire size is linearly related to the forces and moments produced along the arch. An Orthodontic Simulator was utilized to study a simplified high canine malocclusion. Force/couple distributions produced by passive and elastic ligation using two wire sizes (Damon 0.014 and 0.018 inch) measured with a sample size of 144. The distribution and variation in force/couple loading around the arch is a complicated function of wire size. The use of a thicker wire increases the force/couple magnitudes regardless of ligation method. Owing to the non-linear material behaviour of CuNiTi, this increase is less than would occur based on linear theory as would apply for stainless steel wires. The results demonstrate that an increase in wire size does not result in a proportional increase of applied force/moment. This discrepancy is explained in terms of the non-linear properties of CuNiTi wires. This non-proportional force response in relation to increased wire size warrants careful consideration when selecting wires in a clinical setting.
ISSN:1465-3133
DOI:10.1179/1465313314Y.0000000099