Effect of apical portion of T-, sloped L-, and reversed L-closing loops on their force systems
To investigate the effect of the position of the apical portion of closing loops on the force system at both loop ends. T-loops were compared with backward-sloped L-loops (SL) and reversed L-loops (RL). SL-loops were directed toward the anterior side; RL-loops were directed toward the posterior side...
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Veröffentlicht in: | The Angle orthodontist 2017-01, Vol.87 (1), p.104-110 |
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description | To investigate the effect of the position of the apical portion of closing loops on the force system at both loop ends.
T-loops were compared with backward-sloped L-loops (SL) and reversed L-loops (RL). SL-loops were directed toward the anterior side; RL-loops were directed toward the posterior side. Loop response to loop pulling was determined with finite element analysis at six positions of the apical loop portion for 12-mm interbracket distance and 8-mm loop length and height. Three-dimensional models of the closing loops were created using beam elements with the properties of stainless steel. Loop responses (horizontal load/deflection, vertical force, and moment-to-force ratio) at both loop ends were calculated as well as at 100 g and 200 g activation forces.
T-, SL-, and RL-loops with the same position of the apical portion showed approximately the same force system at both loop ends. This behavior was found across the investigated range through which the loops were moved (interbracket center to posterior bracket).
The center of the apical portion determined the force system of the closing loops regardless of the position of the loop legs. The centers of the apical portion of the T-, SL-, and RL-loops acted like V-bend positions. |
doi_str_mv | 10.2319/020316-95.1 |
format | Article |
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T-loops were compared with backward-sloped L-loops (SL) and reversed L-loops (RL). SL-loops were directed toward the anterior side; RL-loops were directed toward the posterior side. Loop response to loop pulling was determined with finite element analysis at six positions of the apical loop portion for 12-mm interbracket distance and 8-mm loop length and height. Three-dimensional models of the closing loops were created using beam elements with the properties of stainless steel. Loop responses (horizontal load/deflection, vertical force, and moment-to-force ratio) at both loop ends were calculated as well as at 100 g and 200 g activation forces.
T-, SL-, and RL-loops with the same position of the apical portion showed approximately the same force system at both loop ends. This behavior was found across the investigated range through which the loops were moved (interbracket center to posterior bracket).
The center of the apical portion determined the force system of the closing loops regardless of the position of the loop legs. The centers of the apical portion of the T-, SL-, and RL-loops acted like V-bend positions.</description><identifier>ISSN: 0003-3219</identifier><identifier>EISSN: 1945-7103</identifier><identifier>DOI: 10.2319/020316-95.1</identifier><identifier>PMID: 27434617</identifier><language>eng</language><publisher>United States: Edward H. Angle Society of Orthodontists</publisher><subject>Biomechanical Phenomena ; Dental Alloys ; Dentistry ; Finite Element Analysis ; Humans ; Materials Testing ; Mechanical Phenomena ; Original ; Orthodontic Appliance Design ; Orthodontic Wires ; Stainless Steel ; Stress, Mechanical ; Tooth Movement Techniques - instrumentation</subject><ispartof>The Angle orthodontist, 2017-01, Vol.87 (1), p.104-110</ispartof><rights>2017 by The EH Angle Education and Research Foundation, Inc. 2017</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c381t-28cdc369b316578c653a498c19d0591e5cc609553b4250b93f65f5cc808be2df3</citedby><cites>FETCH-LOGICAL-c381t-28cdc369b316578c653a498c19d0591e5cc609553b4250b93f65f5cc808be2df3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.ncbi.nlm.nih.gov/pmc/articles/PMC8388594/pdf/$$EPDF$$P50$$Gpubmedcentral$$H</linktopdf><linktohtml>$$Uhttps://www.ncbi.nlm.nih.gov/pmc/articles/PMC8388594/$$EHTML$$P50$$Gpubmedcentral$$H</linktohtml><link.rule.ids>230,315,728,781,785,865,886,27929,27930,53796,53798</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27434617$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Techalertpaisarn, Paiboon</creatorcontrib><creatorcontrib>Versluis, Antheunis</creatorcontrib><title>Effect of apical portion of T-, sloped L-, and reversed L-closing loops on their force systems</title><title>The Angle orthodontist</title><addtitle>Angle Orthod</addtitle><description>To investigate the effect of the position of the apical portion of closing loops on the force system at both loop ends.
T-loops were compared with backward-sloped L-loops (SL) and reversed L-loops (RL). SL-loops were directed toward the anterior side; RL-loops were directed toward the posterior side. Loop response to loop pulling was determined with finite element analysis at six positions of the apical loop portion for 12-mm interbracket distance and 8-mm loop length and height. Three-dimensional models of the closing loops were created using beam elements with the properties of stainless steel. Loop responses (horizontal load/deflection, vertical force, and moment-to-force ratio) at both loop ends were calculated as well as at 100 g and 200 g activation forces.
T-, SL-, and RL-loops with the same position of the apical portion showed approximately the same force system at both loop ends. This behavior was found across the investigated range through which the loops were moved (interbracket center to posterior bracket).
The center of the apical portion determined the force system of the closing loops regardless of the position of the loop legs. The centers of the apical portion of the T-, SL-, and RL-loops acted like V-bend positions.</description><subject>Biomechanical Phenomena</subject><subject>Dental Alloys</subject><subject>Dentistry</subject><subject>Finite Element Analysis</subject><subject>Humans</subject><subject>Materials Testing</subject><subject>Mechanical Phenomena</subject><subject>Original</subject><subject>Orthodontic Appliance Design</subject><subject>Orthodontic Wires</subject><subject>Stainless Steel</subject><subject>Stress, Mechanical</subject><subject>Tooth Movement Techniques - instrumentation</subject><issn>0003-3219</issn><issn>1945-7103</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNpVkc1LAzEQxYMotlZP3iVHQVfzsckmF0FK_YCCl3o1ZLNJu5Ju1mRb6H_v1taipxle3vwmwwPgEqM7QrG8RwRRzDPJ7vARGGKZs6zAiB6DIUKIZpRgOQBnKX0iRBjLySkYkCKnOcfFEHxMnLOmg8FB3dZGe9iG2NWh2Sqz7BYmH1pbwWnf6qaC0a5tTD-C8SHVzRz6ENoE-4luYesIXYjGwrRJnV2mc3DitE_2Yl9H4P1pMhu_ZNO359fxYw-hAncZEaYylMuyP4QVwnBGdS6FwbJCTGLLjOFIMkbLnDBUSuo4c70okCgtqRwdgYcdt12VS1sZ23RRe9XGeqnjRgVdq_8vTb1Q87BWggrBZN4DrveAGL5WNnVqWSdjvdeNDauksCC8IIIh3ltvdlYTQ0rRusMajNQ2EbVLREmmcO---vuzg_c3AvoN1ROFdw</recordid><startdate>20170101</startdate><enddate>20170101</enddate><creator>Techalertpaisarn, Paiboon</creator><creator>Versluis, Antheunis</creator><general>Edward H. Angle Society of Orthodontists</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>5PM</scope></search><sort><creationdate>20170101</creationdate><title>Effect of apical portion of T-, sloped L-, and reversed L-closing loops on their force systems</title><author>Techalertpaisarn, Paiboon ; Versluis, Antheunis</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c381t-28cdc369b316578c653a498c19d0591e5cc609553b4250b93f65f5cc808be2df3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Biomechanical Phenomena</topic><topic>Dental Alloys</topic><topic>Dentistry</topic><topic>Finite Element Analysis</topic><topic>Humans</topic><topic>Materials Testing</topic><topic>Mechanical Phenomena</topic><topic>Original</topic><topic>Orthodontic Appliance Design</topic><topic>Orthodontic Wires</topic><topic>Stainless Steel</topic><topic>Stress, Mechanical</topic><topic>Tooth Movement Techniques - instrumentation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Techalertpaisarn, Paiboon</creatorcontrib><creatorcontrib>Versluis, Antheunis</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>The Angle orthodontist</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Techalertpaisarn, Paiboon</au><au>Versluis, Antheunis</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of apical portion of T-, sloped L-, and reversed L-closing loops on their force systems</atitle><jtitle>The Angle orthodontist</jtitle><addtitle>Angle Orthod</addtitle><date>2017-01-01</date><risdate>2017</risdate><volume>87</volume><issue>1</issue><spage>104</spage><epage>110</epage><pages>104-110</pages><issn>0003-3219</issn><eissn>1945-7103</eissn><abstract>To investigate the effect of the position of the apical portion of closing loops on the force system at both loop ends.
T-loops were compared with backward-sloped L-loops (SL) and reversed L-loops (RL). SL-loops were directed toward the anterior side; RL-loops were directed toward the posterior side. Loop response to loop pulling was determined with finite element analysis at six positions of the apical loop portion for 12-mm interbracket distance and 8-mm loop length and height. Three-dimensional models of the closing loops were created using beam elements with the properties of stainless steel. Loop responses (horizontal load/deflection, vertical force, and moment-to-force ratio) at both loop ends were calculated as well as at 100 g and 200 g activation forces.
T-, SL-, and RL-loops with the same position of the apical portion showed approximately the same force system at both loop ends. This behavior was found across the investigated range through which the loops were moved (interbracket center to posterior bracket).
The center of the apical portion determined the force system of the closing loops regardless of the position of the loop legs. The centers of the apical portion of the T-, SL-, and RL-loops acted like V-bend positions.</abstract><cop>United States</cop><pub>Edward H. Angle Society of Orthodontists</pub><pmid>27434617</pmid><doi>10.2319/020316-95.1</doi><tpages>7</tpages><oa>free_for_read</oa></addata></record> |
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source | MEDLINE; DOAJ Directory of Open Access Journals; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; PubMed Central |
subjects | Biomechanical Phenomena Dental Alloys Dentistry Finite Element Analysis Humans Materials Testing Mechanical Phenomena Original Orthodontic Appliance Design Orthodontic Wires Stainless Steel Stress, Mechanical Tooth Movement Techniques - instrumentation |
title | Effect of apical portion of T-, sloped L-, and reversed L-closing loops on their force systems |
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