Second molar intrusion: Continuous arch or loop mechanics?
Autor(a) principal: | |
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Data de Publicação: | 2018 |
Outros Autores: | , , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UNESP |
Texto Completo: | http://dx.doi.org/10.1016/j.ajodo.2018.01.019 http://hdl.handle.net/11449/186461 |
Resumo: | Introduction: Our aim was to compare the load systems produced by rectangular loops and continuous arch mechanics on intrusion of a maxillary second molar. Methods: An orthodontic appliance was passively bonded from second molar to second molar on a patient's model fixed to an orthodontic force tester. The second molars were extruded by 3 mm, and 2 mechanics systems were compared: beta-titanium rectangular loops and super-elastic nickel-titanium continuous arch. Vertical (Fz) and mesial (Fy) forces, and tipping moments around the buccal axis (Mx) at the tubes were collected at every 0.5 mm of deactivation. Repeated measures analysis of variance was used to detect differences between mechanics. The net Mx was also estimated at the center of resistance of each molar.Results: Significant differences were found between the mechanics at the tubes, except for the Mx in the first molar, and more importantly, at the centers of resistance of the molars: Fz forces were greater in the continuous arch than in the rectangular loops, which, on the other hand, produced lower Fy forces than the continuous arch. In the second molar, net Mx was low initially and changed with deactivation. In the continuous arch, net Mx decreased from -3.6 N.mm of mesial crown tipping to clinically insignificant levels after 2 mm of deactivation. In the first molar, net Mx was lower on the rectangular loop than on the continuous arch during the first 2 mm of deactivation and became similar in the last millimeter of deactivation. Additionally, the net Mx decreased with deactivation with both mechanics. Conclusion: Both mechanics can intrude the second molars. Although the rectangular loop produced less tipping in large deflections, the continuous arch was a better approach when less intrusion was required. |
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Repositório Institucional da UNESP |
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2946 |
spelling |
Second molar intrusion: Continuous arch or loop mechanics?Introduction: Our aim was to compare the load systems produced by rectangular loops and continuous arch mechanics on intrusion of a maxillary second molar. Methods: An orthodontic appliance was passively bonded from second molar to second molar on a patient's model fixed to an orthodontic force tester. The second molars were extruded by 3 mm, and 2 mechanics systems were compared: beta-titanium rectangular loops and super-elastic nickel-titanium continuous arch. Vertical (Fz) and mesial (Fy) forces, and tipping moments around the buccal axis (Mx) at the tubes were collected at every 0.5 mm of deactivation. Repeated measures analysis of variance was used to detect differences between mechanics. The net Mx was also estimated at the center of resistance of each molar.Results: Significant differences were found between the mechanics at the tubes, except for the Mx in the first molar, and more importantly, at the centers of resistance of the molars: Fz forces were greater in the continuous arch than in the rectangular loops, which, on the other hand, produced lower Fy forces than the continuous arch. In the second molar, net Mx was low initially and changed with deactivation. In the continuous arch, net Mx decreased from -3.6 N.mm of mesial crown tipping to clinically insignificant levels after 2 mm of deactivation. In the first molar, net Mx was lower on the rectangular loop than on the continuous arch during the first 2 mm of deactivation and became similar in the last millimeter of deactivation. Additionally, the net Mx decreased with deactivation with both mechanics. Conclusion: Both mechanics can intrude the second molars. Although the rectangular loop produced less tipping in large deflections, the continuous arch was a better approach when less intrusion was required.Univ Estadual Paulista, Fac Odontol Araraquara, Sao Paulo, BrazilLoma Linda Univ, Biomech & Microimaging Lab, Dept Orthodont, Sch Dent, Loma Linda, CA 92350 USAUniv Estadual Paulista, Fac Odontol Araraquara, Sao Paulo, BrazilElsevier B.V.Universidade Estadual Paulista (Unesp)Loma Linda UnivMartins, Renato Parsekian [UNESP]Shintcovsk, Ricardo Lima [UNESP]Shintcovsk, Luegya KnopViecilli, RodrigoMartins, Lidia Parsekian [UNESP]2019-10-05T00:37:45Z2019-10-05T00:37:45Z2018-11-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article629-638http://dx.doi.org/10.1016/j.ajodo.2018.01.019American Journal Of Orthodontics And Dentofacial Orthopedics. New York: Mosby-elsevier, v. 154, n. 5, p. 629-638, 2018.0889-5406http://hdl.handle.net/11449/18646110.1016/j.ajodo.2018.01.019WOS:000448534600012Web of Sciencereponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengAmerican Journal Of Orthodontics And Dentofacial Orthopedicsinfo:eu-repo/semantics/openAccess2024-09-26T14:21:55Zoai:repositorio.unesp.br:11449/186461Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestrepositoriounesp@unesp.bropendoar:29462024-09-26T14:21:55Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false |
dc.title.none.fl_str_mv |
Second molar intrusion: Continuous arch or loop mechanics? |
title |
Second molar intrusion: Continuous arch or loop mechanics? |
spellingShingle |
Second molar intrusion: Continuous arch or loop mechanics? Martins, Renato Parsekian [UNESP] |
title_short |
Second molar intrusion: Continuous arch or loop mechanics? |
title_full |
Second molar intrusion: Continuous arch or loop mechanics? |
title_fullStr |
Second molar intrusion: Continuous arch or loop mechanics? |
title_full_unstemmed |
Second molar intrusion: Continuous arch or loop mechanics? |
title_sort |
Second molar intrusion: Continuous arch or loop mechanics? |
author |
Martins, Renato Parsekian [UNESP] |
author_facet |
Martins, Renato Parsekian [UNESP] Shintcovsk, Ricardo Lima [UNESP] Shintcovsk, Luegya Knop Viecilli, Rodrigo Martins, Lidia Parsekian [UNESP] |
author_role |
author |
author2 |
Shintcovsk, Ricardo Lima [UNESP] Shintcovsk, Luegya Knop Viecilli, Rodrigo Martins, Lidia Parsekian [UNESP] |
author2_role |
author author author author |
dc.contributor.none.fl_str_mv |
Universidade Estadual Paulista (Unesp) Loma Linda Univ |
dc.contributor.author.fl_str_mv |
Martins, Renato Parsekian [UNESP] Shintcovsk, Ricardo Lima [UNESP] Shintcovsk, Luegya Knop Viecilli, Rodrigo Martins, Lidia Parsekian [UNESP] |
description |
Introduction: Our aim was to compare the load systems produced by rectangular loops and continuous arch mechanics on intrusion of a maxillary second molar. Methods: An orthodontic appliance was passively bonded from second molar to second molar on a patient's model fixed to an orthodontic force tester. The second molars were extruded by 3 mm, and 2 mechanics systems were compared: beta-titanium rectangular loops and super-elastic nickel-titanium continuous arch. Vertical (Fz) and mesial (Fy) forces, and tipping moments around the buccal axis (Mx) at the tubes were collected at every 0.5 mm of deactivation. Repeated measures analysis of variance was used to detect differences between mechanics. The net Mx was also estimated at the center of resistance of each molar.Results: Significant differences were found between the mechanics at the tubes, except for the Mx in the first molar, and more importantly, at the centers of resistance of the molars: Fz forces were greater in the continuous arch than in the rectangular loops, which, on the other hand, produced lower Fy forces than the continuous arch. In the second molar, net Mx was low initially and changed with deactivation. In the continuous arch, net Mx decreased from -3.6 N.mm of mesial crown tipping to clinically insignificant levels after 2 mm of deactivation. In the first molar, net Mx was lower on the rectangular loop than on the continuous arch during the first 2 mm of deactivation and became similar in the last millimeter of deactivation. Additionally, the net Mx decreased with deactivation with both mechanics. Conclusion: Both mechanics can intrude the second molars. Although the rectangular loop produced less tipping in large deflections, the continuous arch was a better approach when less intrusion was required. |
publishDate |
2018 |
dc.date.none.fl_str_mv |
2018-11-01 2019-10-05T00:37:45Z 2019-10-05T00:37:45Z |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://dx.doi.org/10.1016/j.ajodo.2018.01.019 American Journal Of Orthodontics And Dentofacial Orthopedics. New York: Mosby-elsevier, v. 154, n. 5, p. 629-638, 2018. 0889-5406 http://hdl.handle.net/11449/186461 10.1016/j.ajodo.2018.01.019 WOS:000448534600012 |
url |
http://dx.doi.org/10.1016/j.ajodo.2018.01.019 http://hdl.handle.net/11449/186461 |
identifier_str_mv |
American Journal Of Orthodontics And Dentofacial Orthopedics. New York: Mosby-elsevier, v. 154, n. 5, p. 629-638, 2018. 0889-5406 10.1016/j.ajodo.2018.01.019 WOS:000448534600012 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
American Journal Of Orthodontics And Dentofacial Orthopedics |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
629-638 |
dc.publisher.none.fl_str_mv |
Elsevier B.V. |
publisher.none.fl_str_mv |
Elsevier B.V. |
dc.source.none.fl_str_mv |
Web of Science reponame:Repositório Institucional da UNESP instname:Universidade Estadual Paulista (UNESP) instacron:UNESP |
instname_str |
Universidade Estadual Paulista (UNESP) |
instacron_str |
UNESP |
institution |
UNESP |
reponame_str |
Repositório Institucional da UNESP |
collection |
Repositório Institucional da UNESP |
repository.name.fl_str_mv |
Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP) |
repository.mail.fl_str_mv |
repositoriounesp@unesp.br |
_version_ |
1828315375765291008 |