OPUS LOOP
Presented by-
DR. PARAG
DESHMUKH
Introductin:
• Closing loops are used in orthodontics with both segmental
and continuous archwires to generate the desired forces and
moments to move teeth in a predictable manner.
• Many closing loop shapes are being used, such as vertical or
teardrop loops, T-loops, L-loops, Gjessing springs, and others.
• In the literature, moment-toforce ratios of approximately 10/1
and 7/1 mm are indicated for translation and controlled
tipping, respectively.
• At these relatively high moment-to-force ratio levels,
stresses reportedly distribute more evenly through the
entire root with minimal changes in the mechanical
properties during activation; this reduces injuries to teeth
and surrounding tissues.
OPUS LOOP :
• Developed by Raymond E. Siatkowski in 1997.
• He designed a new spring which delivers a non varying target M/F ratio
within the range of 8.0-9.0 mm inherently, without adding residual
moments by twist or bends anywhere in the arch wire or loop before
insertion.
Raymond E, Siatkowski , Am J Orthod Dentofac Orthop 1997;112:393-402.)
Physical properties:
• During loop activation, an external load application
causes its deformation. The deformed spring produces a
force during deactivation as it tries to regain its original
form, based on its springback ability.
• When the loop is activated it absorbs and store energy
and gets deformed, as it tries to regain its original form
during deactivation, it will release the same energy by
generating an equivalent force that gradually reduces,
F/D :
Opus loop
During activation:
• Refers to amount of load needed for unit deflection of
spring.
• Numerically calculated as amount of load divided by
amount of deflection.
During deactivation:
• It will loose the same amount of force per unit
deactivation.
• While deactivating, it will generate force of 500 gm,
which will be felt at both ends.
• If we were to use another loop which requires a force of
100 gm for 5 mm activation, its load deflection rate would
be 20 gm/mm.
• During deactivation, it will initially generate a force of 100
gm and its force will drop by 20 gm for every 1 mm
movement of cuspid.
Opus loop
 From clinical point of view orthodontic spring should have :
• A large range of activation so that frequent activations are
not needed.
• A large allowable working load.
• A low load deflection rate.
Momenttoforceratio
• If a force is applied to a body &
the force does not act through
the center of resistance, it
causes the body to rotate.
• Rotation is the movement of a
body where no two points on
the body move the same
amount in same direction.
• Moment: The tendency to
rotate is called a moment.
force
Moment
d
Mf = F x d
M
The direction of moment is
found by following the line Of
action around the centre of
rotation toward the point of
origin.
F
Siatkowski RE. Force system analysis of V-bend sliding mechanics. J Clin Orthod 28(9):543, 1994.
Siatkowski RE. Force system analysis of V-bend sliding mechanics. J Clin Orthod 28(9):543, 1994.
• No closing loop design previously has been capable of
delivering M/F at these levels, most having inherent M/F
of 4-5 mm or less.
• To achieve net translation, orthodontists have had to
add residual moments to the closing loop arch wire with
angulation bends (gable bends) anterior and posterior to
the loop.
Disadvantages of adding residual
moments:
1. The teeth must cycle through controlled tipping to
translation to root movement to achieve net translation
(lower Young's Modulus materials go through fewer of these
cycles for a given distance of space closure).
2. The correct residual moments are difficult to achieve.
3. The resulting ever-changing PDL stress distributions may
not yield the most rapid, least traumatic method of space
closure.
• If a closing loop design capable of achieving inherent,
constant M/F of 8.0 to 9.1 mm without residual
moments were available, en masse space closure with
uniform PDL stress distributions could be achieved.
• Such a mechanism would be less demanding of
operator skill to apply clinically and might provide more
rapid tooth movement with less chance of traumatic
side effects.
• Evidence from animal studies shows that intermittent
force systems may produce more efficient tooth
movement, perhaps 1 hour of force system application
followed by 7 hours of rest.
Gibson JM, King GJ, Keeling SD. Long-term orthodontic tooth movement response to short-term force in
the rat. Angle Orthod 1992.
• A mechanism based on micromotor technology could be
designed in the future to activate/deactivate closing loops
on a time schedule, but it would require loops without
residual moments to produce a true rest period.
Design
Raymond E, Siatkowski Am J Orthod Dentofac Orthop 1997;112:393-402.)
• The loop can be fabricated from .016X.022 or .018x.025 SS or .017x.025
inch TMA or SS wire.
• The design of the loop calls for an off centre positioning with the loop 1.5
mm from the canine bracket.
Activation:
• It can be activated by tightening it distally behind the molar tube and
can be adjusted to produce maximal ,moderate and minimal incisor
retraction, but like all closing mechanisms long range of action, must be
monitored carefully.
Opus loop
Raymond E, Siatkowski Am J Orthod Dentofac Orthop 1997;112:393-402.)
• Opus loop is capable of delivering a non-varying target M/F within the
range of 8.0 to 9.1 mm inherently, without adding residual moments via
twist or bends (commonly gable bends) anywhere in the arch wire or loop
before insertion.
• The resulting precise force systems delivered with non varying M/F can
move groups of teeth more accurately to achieve predetermined position.
Continues arch wire closing loop
ADVANTAGESOFOPUSLOOP
• Only the opus loop has a range of 8.0 to 9.1mm without gable
bends, no loop generates this M/F ratio.
• The opus loop maintains the desired M/F range when
positioned off-center.
• The posterior and anterior moments are in opposite direction
,decreasing the tendency to change occlusal plane.
RELATED ARTICLES
Continuous arch wire closing and verification loop
design, optimization. Part I.
Raymond E. Siatkowski, DMD (Am J Orthod Dentofac Orthop 1997)
 AIM:
• To systematically derive and verify a closing loop design capable of
delivering the required M/F inherently, without adding residual
moments, so that more precise force systems with non varying
translatory M/F can be delivered by dosing loops in a continuous arch.
Introduction :
• The design process uses Castigliano's theorem to derive
equations for moment-to-force ratio (M/F) in terms of loop
geometry.
• Further refinements are performed with finite element
simulations of designs.
• Experimental data are presented illustrating the improved
performance of the new design over standard available
designs.
• Two approaches can be used in space-closing movement
I. supplying the appropriate moments to the teeth via a
continuous arch wire that passes through orthodontic
brackets.
• As tooth move forces decreases applied moment can
increase or decrease, dependent on the arch wire
configuration.
• Therefore, the M/F changes as the tooth moves, and the
tooth responds, typically progressing from controlled
tipping (center of rotation at the root apex) to translation
to root movement.
• second approach involves bending arch wire loops of
various configurations,in a arch wire (to deliver the desired
M/F to several teeth).
• Brackets are not sliding along the arch wire during the
process.
 MATERIAL AND METHODS:
• Theoretical investigations using Castigliano's theorem were
undertaken for vertical loops, T-loops, and L-loops.
• Detailed use of the mathematical trends suggested a new
design, the "Opus loop."
• Specific vertical loops and Opus loops were then simulated by
use of FEM software.
 Result:
• Equations were independently derived for M/F for vertical
loop with apical helix, T-loops and L-loops using the
Castigliano's theorem.
• Greatest effect on raising M/F is to increase loop height.
Increasing the number of apical helices has a lesser effect.
• For equal loop heights, theory predicts increased inherent
M/F for a T-loop configuration and even more for an L-loop
configuration.
• This trend suggested placing a helix somewhere in the apical
portion of the "L" to increase M/F further.
• The position choosen is practical in bending the loop in a
continuous arch.
Opus loop
• The anterior end was fixed and the posterior end
13 mm distal.
• When centered in the interbracket distance, the
M/F at the bracket connected to the helix end of
the loop always exhibited at least three times the
M/F of the other end.
• Angulation of the vertical legs was then varied in 5-degree
increments until M/F was equal at both ends.
• This occurred when the legs were angled at 70 degrees to
the plane of the brackets.
• The M/F increased as the loop was positioned closer to
one bracket than the other and more when the helix end
was closer.
• An activated symmetric closing loop acts as a V-bend located
at the loop's center.
• The systematic theoretical derivation of the new closing loop
design requires verification.
• True verification requires load, deflection, and moment
measurements of actual samples of the loop.
Continuous arch wire closing loop design,
optimization and verification. Part II
MATERIAL AND METHODS:
• Test runs of the various loops were performed on the experimental
apparatus including load cells and moment transducer
• The load cell measures pure force and is insensitive to moments.
• The moment transducer measures pure moment.
• Activation is performed by the digital micrometer transmitted to the
load cell end with no vertical play.
• The moment transducer can twist horizontally, but its center is
constrained from moving vertically.
• Closing loops made in stainless steel and TMA wire were
tested
• Wire sizes were 0.017 × 0.025 inch in TMA and primarily
0.016 × 0.022 inch in stainless steel, although some tests
were performed with 0.018 × 0.025 inch s.s. wire.
• Interbracket distance (IBD) was varied in 2 mm steps
between 13 and 7 mm, simulating space closure.
• Each loop was tested at the center of the IBD and then
off-centered with one vertical leg 1.5 mm from the
moment transducer bracket.
• A test run consisted of incremental activations, measuring
displacements (loop activations) for applied loads of 50,
100, 150, and 200 gm; simultaneous measurements of
activation force were made via the load cell at its end and
moment at the other end.
• The loop was then reversed and all test runs were
repeated to measure the moment at the loop's other end
so that M/F could be determined at both brackets for
each test.
• Each test run was repeated at least once. If values
differed, that run was repeated yet again and calculated
mean values were used.
Result:
• Neither the 8 mm vertical loop with one 3.5 mm diameter
helix nor the 10 mm high, 10 mm long T-loop can achieve
the desired M/F range in any position without inducing
residual moments
• The gabled T and vertical loops generate posterior
moments that are in the same direction as the moments at
the anterior ends, whereas the Opus 70 loop's posterior
moment is in the opposite direction.
• Therefore, the sum of the moments have
the potential to express as occlusal plane
change of the entire arch
• If gabled loops are left tied in for a very
long time, the anterior and posterior
segments will eventually begin to form
two occlusal planes at an angle
approaching the total of the gable bends'
angles.
• Opus 70 loop total moment is the
difference between the moments at the
two ends they being in opposite
directions, decreasing the tendency to
change occlusal plane.
• sum of the moments are additive for the T and vertical
loops, increasing the total moment attempting to change
occlusal plane, whereas the Opus 70 loop total moment is
the difference between the moments at the two ends
they being in opposite directions, decreasing the
tendency to change occlusal plane.
• The Opus 70 loop
exceeds the "safe"
maximum beyond 170
gm activation whereas
the gabled T-loop
exceeds it beyond 110
gm.
• T-loop exceeds the
desired M/F range at less
than 80 gm activation;
the gabled T-loop has a
very narrow range of
acceptable performance
(80-110 gm in s.s. at 13
mm IBD) when used in a
continuous arch.
M/F at each bracket as a function of activation force while varying IBD (13, 11,9, 7
mm) for off-centered 0.016 x 0.022 inch s.s. Opus 70 (without residual moments,
by definition).
Opus loop
Activation (mm) necessary to achieve various activation
forces for the Opus 70 loop formed in 0.016 × 0.022 s.s.,
0.018 x 0.025 s.s., and 0.017 × 0.025 inch TMA wires
CASE REPORT
• A 20-year old Japanese woman transfer patient previously
had impacted maxillary canines extracted near the final
stage of treatment with zero overjet but with 3 mm
spacing distal to the maxillary lateral incisors bilaterally
and the buccal teeth in Class III relationships.
• The maxillary spaces needed to be closed by protraction
of the maxillary posterior teeth with no anterior retraction
allowed.
• The Opus 90 option was chosen, protracting four
premolars and four molars without retracting four
incisors.
• The loop was activated 1 mm every 5 weeks, and the
protraction was completed in three visits.
• Superimposition of a cephalometric radiograph taken at
the time of transfer (the beginning of protraction
mechanics) with that at the end of treatment revealed no
change in incisor position or inclination or any other
structures other than protracted maxillary posterior teeth.
Opus loop
Opus loop
RELATED ARTICLES
Mechanical properties of Opus closing loops, L-
loops, and T-loops investigated with finite element
analysis
Paiboon Techalertpaisarna and Antheunis Versluisb Bangkok, Thailand, and Memphis, Tenn
Am J Orthod Dentofacial Orthop 2013;143:675-83)
• The objective of this research was to investigate the mechanical
properties at both sides of Opus closing loops by analyzing the
effects of loop shape, loop position, coil position, and tipping of
the vertical legs.
Methods:
• Opus loops were compared with L-loops (with and without a coil) and a T-
loop by using finite element analysis.
• Both upright and tipped vertical loop legs (70) were tested.
• Loop response to loop pulling was simulated at 5 loop positions for a 12-
mm interbracket distance and 10-mm loop lengths and heights.
• Three-dimensional models of the closing loops were created by using
beam elements with stainless steel properties.
• The L-loops and Opus loops were directed toward the anterior side. Loop
properties (horizontal load/deflection, vertical force, and moment-to-
force ratio) at both loop ends were recorded at activation forces of 100
and 200 g.
Opus loop
Results:
Opus loop
Opus loop
Opus loop
Opus loop
Conclusions:
• Similarities in the mechanical properties between Opus70 and
T-loops were demonstrated.
• Loop properties varied with loop configuration and position.
• Clinicians should understand the specific characteristics of
each loop configuration to most effectively exploit them for
the desired tooth movements.
Evaluation and comparison of biomechanical properties of snail
loop with that of opus loop and teardrop loop for En mass
retraction of anterior teeth. – A FEM study.
Rao PR, Shrivastav SS, Joshi RA. J Ind Orthod Soc 2013;47(2):62-67.
Introduction:
• In retraction loop mechanics the only known disadvantage is
that, the loop may fail to produce ideal expected results in
practice due to the complexity of loop fabrication and some
unknown factors.
• Teardrop loop is very simple to fabricate, but the inherent M/F
ratio of loop is inadequate for causing translatory motion of
the teeth. Opus loop design inherently produces M/F ratio
close to 10:1.
• A blend of both the designs is seen to be integrated in snail
loop.
• It has got design configuration similar to teardrop loop and
additionally has got a helix in its design similar to opus loop.
• For any retraction loop to be made universally acceptable a
complete knowledge of its biomechanical properties are
very essential.
Aim:
• To evaluate the biomechanical properties of snail loop and
compare it with teardrop loop and opus loop.
Materials and methods:
• Based on the dimensions prescribed by the respective authors
a total of 13 FEM models were constructed and 14 analyses
were conducted in the study.
• The horizontal length of all the loop models (distance between
the anterior and the posterior node) were kept 13mm
considering the interbracket distance from the second
premolar midpoint to the canine midpoint considering a first
premolar extraction case.
• Both TMA and SS wires of both 0.017 × 0.025 inch and 0.019 ×
0.025 inch wire dimensions were used.
Opus loop
Opus loop
 Following 13 FEM models were prepared for the study:
• Three models for snail loop were prepared in 0.017 × 0.025 inch TMA
wire with 0°, 10° and 20° preactivation bends.
• Two models for snail loop were prepared in 0.017 × 0.025 inch SS wire
with 0° and 10° preactivation bend.
• Four models for snail loop were prepared in 0.019 × 0.025 inch TMA wire
with 0°, 5°, 10° and 20° preactivation bends.
• Two models of snail loop were prepared in 0.019 × 0.025 inch SS wire
with 0° and 10° preactivation bend.
• One model each of teardrop loop and opus loop was generated in 0.019 ×
0.025 inch TMA wire without any preactivation bends.
RESULTS:
 Finite element analysis was carried out for different FEM models and
MCSPD code was given to different models prepared, where
• M represents material types (TMA or SS)
• C represents configurations of loops (teardrop, Tr, opus, Op and snail, Sn
loops)
• S represents size of wire ( 0.017 × 0.025 inch as S1 and 0.019 × 0.025 inch
as S2)
• P represents preactivation angle alpha (zero degree as 0°, five degrees as
5°, ten degrees as 10°, twenty degrees as 20°)
• D represents displacement, the amount of activation of the given loop
model (1 mm as D1 and 2 mm as D2).
Opus loop
Opus loop
Conclusion:
• Snail loop has a definite advantage over teardrop loop in
all respects of biomechanical characters but less
advantageous when compared to opus loop.
• Snail loop with incorporation of gable bends is very
efficient to deliver M/F ratio similar to that of opus loop.
Finer shape morphology of snail loop provides ease of
fabrication and prevents tissue impingement which is a
drawback of opus loop.
Conclusion:
• Opus loop is found to have desirable biomechanical properties
which will provide less traumatic and more desired tooth
movement with minimal side effects.
• Though the opus loop is promising to the orthodontist care
should be taken while fabrication to avoid undesirable effects.
• Opus loop still needs detailed clinical trials to understand its
mechanism more correctly and in future, which will be useful
for timely activation of this loop using new technology.
References:
• Continuous arch wire closing loop design, optimization, and
verification - Part I Raymond E. Siatkowski, American Journal of Orthodontics
and Dentofacial Orthopedics October 1997
• Continuous arch wire closing loop design, optimization and
verification. Part – II Raymond E. Siatkowski, American Journal of
Orthodontics and Dentofacial Orthopedics November 1997
• Mechanical properties of Opus closing loops, L-loops, and T-loops
investigated with finite element analysis, Paiboon Techalertpaisarn
American Journal of Orthodontics and Dentofacial Orthopedics May 2013 Vol 143
Issue 5.
• essential of orthodontics biomechanics – by Vijay Jayde andChetan
Jayade.
THANK YOU

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Opus loop

  • 2. Introductin: • Closing loops are used in orthodontics with both segmental and continuous archwires to generate the desired forces and moments to move teeth in a predictable manner. • Many closing loop shapes are being used, such as vertical or teardrop loops, T-loops, L-loops, Gjessing springs, and others. • In the literature, moment-toforce ratios of approximately 10/1 and 7/1 mm are indicated for translation and controlled tipping, respectively.
  • 3. • At these relatively high moment-to-force ratio levels, stresses reportedly distribute more evenly through the entire root with minimal changes in the mechanical properties during activation; this reduces injuries to teeth and surrounding tissues.
  • 4. OPUS LOOP : • Developed by Raymond E. Siatkowski in 1997. • He designed a new spring which delivers a non varying target M/F ratio within the range of 8.0-9.0 mm inherently, without adding residual moments by twist or bends anywhere in the arch wire or loop before insertion. Raymond E, Siatkowski , Am J Orthod Dentofac Orthop 1997;112:393-402.)
  • 5. Physical properties: • During loop activation, an external load application causes its deformation. The deformed spring produces a force during deactivation as it tries to regain its original form, based on its springback ability. • When the loop is activated it absorbs and store energy and gets deformed, as it tries to regain its original form during deactivation, it will release the same energy by generating an equivalent force that gradually reduces,
  • 8. During activation: • Refers to amount of load needed for unit deflection of spring. • Numerically calculated as amount of load divided by amount of deflection.
  • 9. During deactivation: • It will loose the same amount of force per unit deactivation. • While deactivating, it will generate force of 500 gm, which will be felt at both ends.
  • 10. • If we were to use another loop which requires a force of 100 gm for 5 mm activation, its load deflection rate would be 20 gm/mm.
  • 11. • During deactivation, it will initially generate a force of 100 gm and its force will drop by 20 gm for every 1 mm movement of cuspid.
  • 13.  From clinical point of view orthodontic spring should have : • A large range of activation so that frequent activations are not needed. • A large allowable working load. • A low load deflection rate.
  • 14. Momenttoforceratio • If a force is applied to a body & the force does not act through the center of resistance, it causes the body to rotate. • Rotation is the movement of a body where no two points on the body move the same amount in same direction. • Moment: The tendency to rotate is called a moment. force Moment
  • 15. d Mf = F x d M The direction of moment is found by following the line Of action around the centre of rotation toward the point of origin. F
  • 16. Siatkowski RE. Force system analysis of V-bend sliding mechanics. J Clin Orthod 28(9):543, 1994.
  • 17. Siatkowski RE. Force system analysis of V-bend sliding mechanics. J Clin Orthod 28(9):543, 1994.
  • 18. • No closing loop design previously has been capable of delivering M/F at these levels, most having inherent M/F of 4-5 mm or less. • To achieve net translation, orthodontists have had to add residual moments to the closing loop arch wire with angulation bends (gable bends) anterior and posterior to the loop.
  • 19. Disadvantages of adding residual moments: 1. The teeth must cycle through controlled tipping to translation to root movement to achieve net translation (lower Young's Modulus materials go through fewer of these cycles for a given distance of space closure). 2. The correct residual moments are difficult to achieve. 3. The resulting ever-changing PDL stress distributions may not yield the most rapid, least traumatic method of space closure.
  • 20. • If a closing loop design capable of achieving inherent, constant M/F of 8.0 to 9.1 mm without residual moments were available, en masse space closure with uniform PDL stress distributions could be achieved. • Such a mechanism would be less demanding of operator skill to apply clinically and might provide more rapid tooth movement with less chance of traumatic side effects.
  • 21. • Evidence from animal studies shows that intermittent force systems may produce more efficient tooth movement, perhaps 1 hour of force system application followed by 7 hours of rest. Gibson JM, King GJ, Keeling SD. Long-term orthodontic tooth movement response to short-term force in the rat. Angle Orthod 1992. • A mechanism based on micromotor technology could be designed in the future to activate/deactivate closing loops on a time schedule, but it would require loops without residual moments to produce a true rest period.
  • 22. Design Raymond E, Siatkowski Am J Orthod Dentofac Orthop 1997;112:393-402.) • The loop can be fabricated from .016X.022 or .018x.025 SS or .017x.025 inch TMA or SS wire. • The design of the loop calls for an off centre positioning with the loop 1.5 mm from the canine bracket.
  • 23. Activation: • It can be activated by tightening it distally behind the molar tube and can be adjusted to produce maximal ,moderate and minimal incisor retraction, but like all closing mechanisms long range of action, must be monitored carefully.
  • 25. Raymond E, Siatkowski Am J Orthod Dentofac Orthop 1997;112:393-402.)
  • 26. • Opus loop is capable of delivering a non-varying target M/F within the range of 8.0 to 9.1 mm inherently, without adding residual moments via twist or bends (commonly gable bends) anywhere in the arch wire or loop before insertion. • The resulting precise force systems delivered with non varying M/F can move groups of teeth more accurately to achieve predetermined position. Continues arch wire closing loop
  • 27. ADVANTAGESOFOPUSLOOP • Only the opus loop has a range of 8.0 to 9.1mm without gable bends, no loop generates this M/F ratio. • The opus loop maintains the desired M/F range when positioned off-center. • The posterior and anterior moments are in opposite direction ,decreasing the tendency to change occlusal plane.
  • 28. RELATED ARTICLES Continuous arch wire closing and verification loop design, optimization. Part I. Raymond E. Siatkowski, DMD (Am J Orthod Dentofac Orthop 1997)
  • 29.  AIM: • To systematically derive and verify a closing loop design capable of delivering the required M/F inherently, without adding residual moments, so that more precise force systems with non varying translatory M/F can be delivered by dosing loops in a continuous arch.
  • 30. Introduction : • The design process uses Castigliano's theorem to derive equations for moment-to-force ratio (M/F) in terms of loop geometry. • Further refinements are performed with finite element simulations of designs. • Experimental data are presented illustrating the improved performance of the new design over standard available designs.
  • 31. • Two approaches can be used in space-closing movement I. supplying the appropriate moments to the teeth via a continuous arch wire that passes through orthodontic brackets. • As tooth move forces decreases applied moment can increase or decrease, dependent on the arch wire configuration. • Therefore, the M/F changes as the tooth moves, and the tooth responds, typically progressing from controlled tipping (center of rotation at the root apex) to translation to root movement.
  • 32. • second approach involves bending arch wire loops of various configurations,in a arch wire (to deliver the desired M/F to several teeth). • Brackets are not sliding along the arch wire during the process.
  • 33.  MATERIAL AND METHODS: • Theoretical investigations using Castigliano's theorem were undertaken for vertical loops, T-loops, and L-loops. • Detailed use of the mathematical trends suggested a new design, the "Opus loop." • Specific vertical loops and Opus loops were then simulated by use of FEM software.
  • 34.  Result: • Equations were independently derived for M/F for vertical loop with apical helix, T-loops and L-loops using the Castigliano's theorem. • Greatest effect on raising M/F is to increase loop height. Increasing the number of apical helices has a lesser effect. • For equal loop heights, theory predicts increased inherent M/F for a T-loop configuration and even more for an L-loop configuration. • This trend suggested placing a helix somewhere in the apical portion of the "L" to increase M/F further. • The position choosen is practical in bending the loop in a continuous arch.
  • 36. • The anterior end was fixed and the posterior end 13 mm distal. • When centered in the interbracket distance, the M/F at the bracket connected to the helix end of the loop always exhibited at least three times the M/F of the other end.
  • 37. • Angulation of the vertical legs was then varied in 5-degree increments until M/F was equal at both ends. • This occurred when the legs were angled at 70 degrees to the plane of the brackets. • The M/F increased as the loop was positioned closer to one bracket than the other and more when the helix end was closer.
  • 38. • An activated symmetric closing loop acts as a V-bend located at the loop's center.
  • 39. • The systematic theoretical derivation of the new closing loop design requires verification. • True verification requires load, deflection, and moment measurements of actual samples of the loop.
  • 40. Continuous arch wire closing loop design, optimization and verification. Part II
  • 41. MATERIAL AND METHODS: • Test runs of the various loops were performed on the experimental apparatus including load cells and moment transducer • The load cell measures pure force and is insensitive to moments. • The moment transducer measures pure moment. • Activation is performed by the digital micrometer transmitted to the load cell end with no vertical play. • The moment transducer can twist horizontally, but its center is constrained from moving vertically.
  • 42. • Closing loops made in stainless steel and TMA wire were tested • Wire sizes were 0.017 × 0.025 inch in TMA and primarily 0.016 × 0.022 inch in stainless steel, although some tests were performed with 0.018 × 0.025 inch s.s. wire. • Interbracket distance (IBD) was varied in 2 mm steps between 13 and 7 mm, simulating space closure. • Each loop was tested at the center of the IBD and then off-centered with one vertical leg 1.5 mm from the moment transducer bracket.
  • 43. • A test run consisted of incremental activations, measuring displacements (loop activations) for applied loads of 50, 100, 150, and 200 gm; simultaneous measurements of activation force were made via the load cell at its end and moment at the other end. • The loop was then reversed and all test runs were repeated to measure the moment at the loop's other end so that M/F could be determined at both brackets for each test. • Each test run was repeated at least once. If values differed, that run was repeated yet again and calculated mean values were used.
  • 45. • Neither the 8 mm vertical loop with one 3.5 mm diameter helix nor the 10 mm high, 10 mm long T-loop can achieve the desired M/F range in any position without inducing residual moments • The gabled T and vertical loops generate posterior moments that are in the same direction as the moments at the anterior ends, whereas the Opus 70 loop's posterior moment is in the opposite direction.
  • 46. • Therefore, the sum of the moments have the potential to express as occlusal plane change of the entire arch • If gabled loops are left tied in for a very long time, the anterior and posterior segments will eventually begin to form two occlusal planes at an angle approaching the total of the gable bends' angles. • Opus 70 loop total moment is the difference between the moments at the two ends they being in opposite directions, decreasing the tendency to change occlusal plane.
  • 47. • sum of the moments are additive for the T and vertical loops, increasing the total moment attempting to change occlusal plane, whereas the Opus 70 loop total moment is the difference between the moments at the two ends they being in opposite directions, decreasing the tendency to change occlusal plane.
  • 48. • The Opus 70 loop exceeds the "safe" maximum beyond 170 gm activation whereas the gabled T-loop exceeds it beyond 110 gm. • T-loop exceeds the desired M/F range at less than 80 gm activation; the gabled T-loop has a very narrow range of acceptable performance (80-110 gm in s.s. at 13 mm IBD) when used in a continuous arch.
  • 49. M/F at each bracket as a function of activation force while varying IBD (13, 11,9, 7 mm) for off-centered 0.016 x 0.022 inch s.s. Opus 70 (without residual moments, by definition).
  • 51. Activation (mm) necessary to achieve various activation forces for the Opus 70 loop formed in 0.016 × 0.022 s.s., 0.018 x 0.025 s.s., and 0.017 × 0.025 inch TMA wires
  • 52. CASE REPORT • A 20-year old Japanese woman transfer patient previously had impacted maxillary canines extracted near the final stage of treatment with zero overjet but with 3 mm spacing distal to the maxillary lateral incisors bilaterally and the buccal teeth in Class III relationships. • The maxillary spaces needed to be closed by protraction of the maxillary posterior teeth with no anterior retraction allowed. • The Opus 90 option was chosen, protracting four premolars and four molars without retracting four incisors.
  • 53. • The loop was activated 1 mm every 5 weeks, and the protraction was completed in three visits. • Superimposition of a cephalometric radiograph taken at the time of transfer (the beginning of protraction mechanics) with that at the end of treatment revealed no change in incisor position or inclination or any other structures other than protracted maxillary posterior teeth.
  • 56. RELATED ARTICLES Mechanical properties of Opus closing loops, L- loops, and T-loops investigated with finite element analysis Paiboon Techalertpaisarna and Antheunis Versluisb Bangkok, Thailand, and Memphis, Tenn Am J Orthod Dentofacial Orthop 2013;143:675-83) • The objective of this research was to investigate the mechanical properties at both sides of Opus closing loops by analyzing the effects of loop shape, loop position, coil position, and tipping of the vertical legs.
  • 57. Methods: • Opus loops were compared with L-loops (with and without a coil) and a T- loop by using finite element analysis. • Both upright and tipped vertical loop legs (70) were tested. • Loop response to loop pulling was simulated at 5 loop positions for a 12- mm interbracket distance and 10-mm loop lengths and heights. • Three-dimensional models of the closing loops were created by using beam elements with stainless steel properties. • The L-loops and Opus loops were directed toward the anterior side. Loop properties (horizontal load/deflection, vertical force, and moment-to- force ratio) at both loop ends were recorded at activation forces of 100 and 200 g.
  • 64. Conclusions: • Similarities in the mechanical properties between Opus70 and T-loops were demonstrated. • Loop properties varied with loop configuration and position. • Clinicians should understand the specific characteristics of each loop configuration to most effectively exploit them for the desired tooth movements.
  • 65. Evaluation and comparison of biomechanical properties of snail loop with that of opus loop and teardrop loop for En mass retraction of anterior teeth. – A FEM study. Rao PR, Shrivastav SS, Joshi RA. J Ind Orthod Soc 2013;47(2):62-67.
  • 66. Introduction: • In retraction loop mechanics the only known disadvantage is that, the loop may fail to produce ideal expected results in practice due to the complexity of loop fabrication and some unknown factors. • Teardrop loop is very simple to fabricate, but the inherent M/F ratio of loop is inadequate for causing translatory motion of the teeth. Opus loop design inherently produces M/F ratio close to 10:1.
  • 67. • A blend of both the designs is seen to be integrated in snail loop. • It has got design configuration similar to teardrop loop and additionally has got a helix in its design similar to opus loop. • For any retraction loop to be made universally acceptable a complete knowledge of its biomechanical properties are very essential.
  • 68. Aim: • To evaluate the biomechanical properties of snail loop and compare it with teardrop loop and opus loop.
  • 69. Materials and methods: • Based on the dimensions prescribed by the respective authors a total of 13 FEM models were constructed and 14 analyses were conducted in the study. • The horizontal length of all the loop models (distance between the anterior and the posterior node) were kept 13mm considering the interbracket distance from the second premolar midpoint to the canine midpoint considering a first premolar extraction case. • Both TMA and SS wires of both 0.017 × 0.025 inch and 0.019 × 0.025 inch wire dimensions were used.
  • 72.  Following 13 FEM models were prepared for the study: • Three models for snail loop were prepared in 0.017 × 0.025 inch TMA wire with 0°, 10° and 20° preactivation bends. • Two models for snail loop were prepared in 0.017 × 0.025 inch SS wire with 0° and 10° preactivation bend. • Four models for snail loop were prepared in 0.019 × 0.025 inch TMA wire with 0°, 5°, 10° and 20° preactivation bends. • Two models of snail loop were prepared in 0.019 × 0.025 inch SS wire with 0° and 10° preactivation bend. • One model each of teardrop loop and opus loop was generated in 0.019 × 0.025 inch TMA wire without any preactivation bends.
  • 73. RESULTS:  Finite element analysis was carried out for different FEM models and MCSPD code was given to different models prepared, where • M represents material types (TMA or SS) • C represents configurations of loops (teardrop, Tr, opus, Op and snail, Sn loops) • S represents size of wire ( 0.017 × 0.025 inch as S1 and 0.019 × 0.025 inch as S2) • P represents preactivation angle alpha (zero degree as 0°, five degrees as 5°, ten degrees as 10°, twenty degrees as 20°) • D represents displacement, the amount of activation of the given loop model (1 mm as D1 and 2 mm as D2).
  • 76. Conclusion: • Snail loop has a definite advantage over teardrop loop in all respects of biomechanical characters but less advantageous when compared to opus loop. • Snail loop with incorporation of gable bends is very efficient to deliver M/F ratio similar to that of opus loop. Finer shape morphology of snail loop provides ease of fabrication and prevents tissue impingement which is a drawback of opus loop.
  • 77. Conclusion: • Opus loop is found to have desirable biomechanical properties which will provide less traumatic and more desired tooth movement with minimal side effects. • Though the opus loop is promising to the orthodontist care should be taken while fabrication to avoid undesirable effects. • Opus loop still needs detailed clinical trials to understand its mechanism more correctly and in future, which will be useful for timely activation of this loop using new technology.
  • 78. References: • Continuous arch wire closing loop design, optimization, and verification - Part I Raymond E. Siatkowski, American Journal of Orthodontics and Dentofacial Orthopedics October 1997 • Continuous arch wire closing loop design, optimization and verification. Part – II Raymond E. Siatkowski, American Journal of Orthodontics and Dentofacial Orthopedics November 1997 • Mechanical properties of Opus closing loops, L-loops, and T-loops investigated with finite element analysis, Paiboon Techalertpaisarn American Journal of Orthodontics and Dentofacial Orthopedics May 2013 Vol 143 Issue 5. • essential of orthodontics biomechanics – by Vijay Jayde andChetan Jayade.

Editor's Notes

  • #3: First point: To move teeth in a predictable manner with desired forces and moments loops have been introduced into orthodontics. After second point: These loop types can be further modified by adding a coil, tipping the vertical legs, and so on.
  • #4: Researchers and clinicians, therefore, have tried to design and refine loop geometry to obtain as high moment-to-force ratios as possible and have designed such a loop fulfilling this criteria which is opus loop.
  • #5: Second point: Other loop designs available, were having insufficient inherent M/F, are clinically difficult to apply and can bring about undesirable changes.
  • #6: Second point: Similar to the elastic deformation of an archwire the deformation of a loop is also elastic initially. When the loop is activated it absorbs and store energy and gets deformed, as it tries to regain its original form during deactivation, it will release the same energy by generating an equivalent force that gradually reduces,we make use of this force for tooth movement.
  • #7: Besides configuring the looped arch wire to deliver proper M/F to achieve the direction of tooth movement desired, the loop's load-deflection rate(F/D) have added importance. Load deflection is also known as spring gradient. It is the load needed to produce unit deformation in elastic range. Its counterpart is F/D which is the force which the deformed spring expends per unit recovery of deflection during deactivation. Now in this graph stiffness given by slope of linear portion of curve. Range is the distance along the x axis to the point at which permanent deformation occurs (yield point0.1 mm deformation occured), clinically usefull springback occurs if the wire is deflected beyond the yield point(point of arbitory clinical loading), but it no londer returns to its original shape, at the failure point wire breaks.
  • #8: Loop properties: Spring gradient or load deflection is 2 divided by 1. Load and deformation have a proportionate relationship up to the point of maximum elastic deformation both during activation and deactivation. Beyond this point spring will start experiencing permanent deformation . In this phase relationship between load and deformation is no longer linear
  • #9: Let us assume that one end is engaged in molar tube and on application of increasing load it stretches by 1 mm till at 5 mm of stretch till its other end could be engaged in the cuspid bracket. After last point: The load deflection rate for this spring is 500 gm divided by 5 mm i.e. 100 gm/mm.
  • #10: Assuming the molar is stabilized, the force will drop by 100 gm for every 1 mm movement of cuspid. Hence the force deflection rate is force delivered by the loop per unit deactivation.
  • #12: After first point: in contrast to 100 gm of drop for the previously mentioned loop. Obviously the second loop is preferable not only because its initial force level is lower but also because the drop of force during deactivation is least steep causing more constant force.
  • #15: Second point: so that the spring is sufficiently strong and does not get permanently deformed before storing enough energy to release desired force level.
  • #16: Thus moment is a kind of side effect of the force applied. By changing the moment to force ratio we can decide the type of tooth and root movement we want , like controlled tipping , uncontrolled tipping, translation . 12:1 – root movement 10:1 translation 5:1 controlled tipping 0:1 uncontrolled tipping
  • #17: Moment to a force is calculated by multiplying the distance between the center of resistance of tooth and point of application of force.
  • #19: Bowley et al. laid the groundwork for holographic measurements and finite element analyses to determine the location of the centers of resistance for individual teeth and thereby, the M/F necessary to achieve translation. The derived M/Fs vary from 7.1 to 10.2 mm for individual tooth.
  • #20: 8.0 to 9.1 mm for groups of teeth. Bracket position alters this value i.e. more gingival placement of brackets will lower these values.
  • #21: After last point: that are alpha and beta bends.
  • #23: 1st point: If any loop design would give constant M/F of 8 to 9.1 mm without any residual bends for desirable moments en mass space closure with no traumatic forces to pdl could be achieved
  • #24: So the loop designs like opus loop have to be considered for such mechanism to come in to the picture.
  • #26: In siatoviskys original article he has given the activation for maximum anchorage after canines are retracted.
  • #28: Most of the protraction force is generated by the large anterior moment and by the intermaxillary elastics to a rigid rectangular arch wire in the opposing arch. Intermaxillary Niti closed coil springs capable of delivering 150 gm force can be substituted for the elastics.
  • #34: A systematic approach to closing loop design for use in continuous arch wires is presented.
  • #35: After Ist point Via elastomeric modules , coil springs etc we can create moments for the teeth via couples, equal and opposite noncollinear vertical forces at the mesial and distal end of the bracket. Such progression may not produce the most efficient or the least traumatic tooth movement.
  • #36: 2nd point: As the brackets are not sliding they are free of friction Groups of teeth can therefore be moved with more accurately defined force systems for more precise anchorage control
  • #37: Perusal: Studying something carefully. Third point – T, l and helical loop and opus loop simulated by FEM.
  • #40: M/F is maximized when as much wire is placed as high as possible in the loops (H and L large, R small)
  • #41: Opus loops 10 mm high, 10 mm long, and 0.5 mm radius in 0.016 × 0.022 inch s.s. wire, 0.018 × 0.025 inch s.s. wire, and 0.017 × 0.025 inch TMA were simulated via the FEM software.
  • #43: After last point: An activated symmetric and asymmetric loop acts lyk respective V bend. The systematic theoretical derivation of the new closing loop design requires verification.
  • #44: An activated symmetric closing loop acts as a V-bend located at the loop's center andcan be visualized by examining the horizontal legs of the vertical loop (since the angles of entry at the 2 brackets are identical but facing in opposite direction moments created are opposite) An activated asymmetric loop acts as an off-centered V-bend. (here A experiances greater momentbecause angle of entry in A has increased though 2 moments are acting in opposite direction their sum total cannot become zeroand leaves residual moment, another opposing moment to this moment will be create i.e. 2 vertical forces at 2 brackets.)
  • #46: This article processes with the Experimental verification of the design criteria via load, displacement, and moment measurements of actual samples of the loop.
  • #47: Siamese twin brackets, 0.018 × 0.025 inch, were epoxied to an aluminum bracket mount threaded into the load cell and to the moment transducer.
  • #50: The greatest negative impact on M/F in the off-centered position is crossing the loop legs (Opus 90 vs. Opus 90 X-legs: 8.6 falls to 6.2) and decreasing loop height (Opus 70 vs. Opus 70, 7 mm high: 8.7 to 5.9 mm). Decreasing the loop angulation decreases M/F (Opus 70, 12 mm long vs. 12 mm long at 64 degrees: 8.7 to 7.2 ram). Dropping the anterior end of the loop decreases M/F (Opus 70 vs. Opus 70, end 9 mm high: 8.7 to 7.6 ram). Increasing loop length beyond 10 mm does not increase M/F, contrary to theoretical prediction (Opus 70 vs. Opus 70, 12 mm long) but decreasing loop length decreases M/F (Opus 70 vs. Opus 70, 8 mm long: 8.7 to 8.0 mm).
  • #51: Opus 70 loop maintains M/F within the desired range at all activation force levels without residual moments
  • #53: An activated asymmetric loop acts as an off-centered V-bend. (here A experiances greater moment because angle of entry in A has increased though 2 moments are acting in opposite direction their sum total cannot become zero and leaves residual moment, another opposing moment to this moment will be create i.e. 2 vertical forces at 2 brackets.)
  • #54: For opus range of activation is more.
  • #55: It is only beyond 150 gm at 7 mm IBD, the end of space closure, that the anterior M/F falls outside the desired range.
  • #56: The total moment exceeds the safe maximum only when the activation force is 200 gm and the IBD is greater than 9 mm. Activation force levels above 170 gm may need to be avoided at the beginning and the very end of space closure with this loop.
  • #61: loop faces posteriorly with crossed legs. The crossed legs reduce the load-deflection rate so that a clinically practical activation of 1 mm produces 75 gm/side using 0.018 × 0.025 inch s.s. wire. With legs crossed, the apical portion of the loop faces posteriorly so that the Opus 90 asymmetric moments result in the higher moment being delivered to the incisors.
  • #64: Configurations and dimensions of the 7 closing loops in this study: A, L90; B, L70; C, LC90; D, LC70; E, Opus90; F, Opus70; G, T-loop. H, Coil portions were modeled 3 dimensionally.
  • #65: load/deflection ratio was lowest when centered and highest when placed close to either end. When moved toward the canine bracket, load/deflection ratios increased and became highest close to the canine bracket side.
  • #67: vertical forces created by horizontal forces were zero when the T-loops were centered and maximal when placed close to an end
  • #69: The Opus90 achieved a higher moment-to-force ratio than did the Opus70. The highest momentto- force ratio was found for an L-loop with a coil when the loop was placed between the premolar bracket and center (a/b ratio, 0.33-0.5). Upright vertical leg L-loops reached their maximum moment-to-force ratios when their loops were placed around the center. Upright Opus loops and L-loops showed the highest moment-to-force ratios (8.5-9.3) on the canine bracket when the loop was centered.
  • #73: First point: Force system of loops can be tested in the laboratory and the clinician can then fabricate the spring in accordance. opus loop.
  • #81: F/D rate produced by snail loop models prepared in TMA wire was comparatively less when compared to models prepared in SS wire (Tables 1 and 2). Snail loop model prepared in TMA wire with dimension of S2 having 20° bend produced maximum force of 339 gm after D2 displacement, snail loop model prepared in TMA wirewith dimension of S1 having 20° produced a maximum force of 328.3 gm after D2 with acceptable M/F ratio. Forces produced by models prepared in ss were very high. For individual bodily canine retraction a force of 150 and 300 gm for anterior retraction is recommended. A force level of 70 to 120 gm is needed for bodily movement of the dentition. Force level of 100 gm is recommended for incisor retraction on each side. A force range of 320 to 350 gm for upper anteriors and 270 to 290 gm is required for lower Anteriors. A force level of 200 gm for en mass Retractio n
  • #82: Comparison between snail, teardrop and opus loop prepared in S2 dimension in TMA wire without giving any preactivation bend at D1 displacement showed that M/F ratio of opus loop was 9.8 mm, teardrop loop was 4.5 mm and for snail loop was 5.5 mm. The M/F ratio produced by all the loop models was constant throughout the period of activation