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Dr Abbas Naseem
drabbasnaseem@gmail.com
abbas_naseem@yahoo.com
BASIC
Learning Outcomes ……..
1. Basic Terminology
2. Mechanical properties of orthodontic wire
3. Elastic properties of orthodontic wire
4. Properties of ideal orthodontic wire
5. What are the ideal orthodontic alloys
6. Characteristics/factors that influence selection of desirable
orthodontic wire
• Wire cross-section
• Wire length
• Amount of wire
• Selection of proper wire (Alloy and Cross Section)
7. History/Evolution of archwires
8. Types of archwires
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Basic Terms
Stress: Force per unit area.
Stress is the internal distribution of the load.
Strain: Deflection per unit length.
Internal distortion produced by the load.
Reference:
1. Orthodontics, the art and science, 4th Edition, S.I.Bhalaji
2. Textbook of orthodontics, 2nd Edition, Gurkeerat singh
Basic Terms
Stiffness: The presence of low stiffness provides the ability to apply lower forces and a
more constant force over time. ¹
Stiffness / Load defection rate:
This is the force magnitude delivered by an appliance and is proportional to modulus of
elasticity (E). ²
Low stiffness leads to an ability to apply lower forces, a more constant force to be delivered
overtime and greater ease and accuracy in applying a given force.
Spring back: It is the measure of how far a wire can be deflected without causing permanent
deformation. It is also called elastic deflection. The archwire should ideally
possess high springback, which results in an increase in its range of action. ¹
Spring back / maximum elastic deflection / working range:
ratio of yield strength(YS) to modulus of elasticity(E) of the material. ²
Higher springback provides ability to apply large activations with a resultant increase in
working time of appliance, thus decreasing number of archwire changes.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
The range is the distance along the X-axis to the point at which permanent deformation occurs
(usually taken as the yield point, at which 0.1%permanent deformation has occurred).
Basic Terms
Stress and strain are internal characteristics that can be calculated from measurements of
force and deflection, so the general shapes of force–deflection and stress–strain curves are
similar.
The stiffness of the material is given by the
slope of the linear portion of the curve.
Clinically useful springback occurs if the
wire is deflected beyond the yield point (as
to the point indicated here as “arbitrary
clinical loading”), but it no longer returns to
its original shape.
Reference:
1. Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
2. Orthodontics, the art and science, 4th Edition, S.I.Bhalaji
Basic Terms
Resilience: Area under the stress-strain curve out to the proportional limit.
Represents the energy storage capacity of wire, which is a combination of strength
and springiness. ¹
Resilience is the amount of force the wire can withstand before permanent deformation.
Archwires should exhibit high resilience so as to increase working range of appliance.²
Formability: Amount of permanent deformation that a wire can withstand before failing.
Represents the amount of permanent bending the wire will tolerate before it
breaks. ¹
The archwire material should exhibit high formability so as to bend the arch wire into desired
configuration such as coils, loops without fracturing the wire. ²
Reference:
• Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:8-9)
Resilience:
The energy absorbed by a material in undergoing
elastic deformation up to the elastic limit.
Toughness:
The total amount of energy which a material can
absorb upto point of fracture.
Basic Terms
Reference:
• Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:11)
Stress & Strain Relationship (Cause and
effect Relationship)• Use to characterise the mechanical properties of materials.
• The application of an external force, producing a stress within a material, results in a
change in dimension or strain within the body.
P: Propotional Limit: Linear relationship
between stress and strain upto point P.
• Further increases in stress cause
proportionally greater increases in strain
until the material fractures at point T.
E: Yield Stress
• Corresponds to the stress beyond which
strains are not fully recovered.
• Maximum stress which a material can
withstand without undergoing some
permanent deformation.
T: fracture stress (Tensile/Compressive strength)
Reference:
1. Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:11)
2. Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Yield stress is difficult to characterise experimentally… ¹
It requires a series of experiments in which stress is gradually increased then
released and observations on elastic recovery made.
As a consequence of these experimental difficulties, the proportional limit is
often used to give an approximation to the value of the yield stress.
Hence, High value of proportional limit indicates a sample of material is more
likely to withstand applied stress without permanent deformation.
Proportional limit VS. Yield stress
Precisely determining proportional point can be difficult, so a more
practical indicator is the yield strength. ²
True elastic limit ?
Reference:
• Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:11)
• Rigid
• Strong
• Tough
• Ductile
• Rigid
• Strong
• Brittle
• Flexible
• Weak
• Brittle
• Flexible
• Tough
• Rigid
• Weak
• Brittle
• Flexible
• Resilient
“Stress and strain relationship used to characterise the mechanical
properties of materials.”
- Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:8)
The Basic Properties of Elastic Materials – “The elastic behavior of
any material is defined in terms of its stress–strain response to an
external load.”
- Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. (Chapter:9. page:312)
MECJANICAL PROPERTIES
VS.
ELASTIC PROPERTIES
Reference:
• http://en.wikipedia.org/wiki/List_of_materials_properties
MECHANICAL
PROPERTIES
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
The mechanical properties of an alloy to be used in an
orthodontic wire can be described on at least three levels.
1. Observational level
2. Stress-strain level
3. Atomic and molecular level
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• Basic Behavior of Alloys
• Elastic Limit
• Modulus of Elasticity
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Active and Reactive Members
The active member is the part involved in tooth movement.
The reactive member serves as anchorage and involves the teeth that will not be displaced.
Specifically of interest are three important characteristics involving
active and reactive members:
1. Moment-to-Force Ratio
2. Load-deflection Rate / Torque Twist Rate
3. Maximum elastic load / moment
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
All three of the important characteristics of an
orthodontic appliance
1. Moment-to-Force Ratio
2. Load-deflection Rate / Torque Twist Rate
3. Maximum elastic load / moment
are found within the elastic range of an orthodontic
wire and therefore may be called spring
characteristics.
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
On the subclinical level the three primary objectives:
1. Control the center of rotation of the tooth.
2. Produce desirable stress levels in the PDL.
3. Maintain a relatively constant level of stress.
At the clinical level of observation:
the focus becomes the forces and moments produced by an
orthodontic appliance.
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
1. Moment-to-Force Ratio
Mechanical Properties of
the Orthodontic wires
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Force—a load applied to an object that will tend to move it to a different position in space.
Moment—a measure of the tendency to rotate an object around some point.
A moment is generated by a force acting at a distance.
Mechanical Properties of
the Orthodontic wires
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Couple—two forces equal in magnitude and opposite in direction. The result of applying two
forces in this way is a pure moment, since the translatory effect of the forces
cancels out.
A couple will produce pure rotation, spinning the object around its center of resistance.
Mechanical Properties of
the Orthodontic wires
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Center of resistance—The center of resistance (CR) for any tooth is at the approximate
midpoint of the embedded portion of the root.
Center of rotation—The point around which rotation actually occurs when an object is being
moved.
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
1. Moment-to-Force Ratio
Mechanical Properties of
the Orthodontic wires
• To produce different types of tooth movement, the ratio between the applied moment
and the force on the crown must be changed.
• As the M/F ratio is altered, the center of rotation changes.
• Crown tipping, translation, and root movement are examples of different types of
tooth movement that can be produced with the proper M/F ratio.
• The M/F ratio determines the control the orthodontic appliance
has over the active and reactive units.
• Specifically, it controls the center of rotation of the tooth or a
group of teeth.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
2. Load-deflection Rate / Torque Twist Rate
Mechanical Properties of
the Orthodontic wires
• Force produced per unit activation.
OR The force required per unit deflection.
• is a factor in the delivery of a relatively constant force.
• As the load deflection rate declines for a tooth that is moving under a continuous
force, the change in force value is reduced.
For active members a low load-deflection rate is desirable for two important reasons:
1. Maintains a more desirable stress level in the PDL because the force on a tooth does
not radically change magnitude every time the tooth has been displaced.
2. Offers greater accuracy in controlling force magnitude.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
2. Load-deflection Rate / Torque Twist Rate
Mechanical Properties of
the Orthodontic wires
The reactive member it should have a high load-deflection rate. (should be relatively
rigid)
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
3. Maximum elastic load / moment
Mechanical Properties of
the Orthodontic wires
Greatest force or moment that can be applied to a member without causing
permanent deformation.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• Basic Behavior of Alloys
Mechanical Properties of
the Orthodontic wiresPmax:
• A point where load and deflection are
no longer proportionate.
• Near Pmax, permanent deformation is
being produced in the spring, which will
not return to its original shape.
• Pmax represents the highest load that can
be placed on the spring without
permanent deformation; that is, the
maximal elastic load.
Hooke’s Law
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Mechanical Properties of
the Orthodontic wiresElastic Limit (EL) The EL is the greatest
stress that can be applied to the alloy
without permanent deformation.
Modulus of elasticity (E) this
mechanical property determines the
load-deflection rate of a spring.
Stress in a wire is force per unit area applied to a cross section.
Strain is deflection per unit length of the wire.
Modulus of elasticity (E) is the ratio of stress to strain.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Mechanical Properties of
the Orthodontic wires
The EL is analogous to the maximal elastic load (Pmax) and therefore is the mechanical
property that determines the ability of a member to withstand permanent deformation.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Mechanical Properties of
the Orthodontic wires
A number of other terms describe this general part of the curve (O-
EL), such as yield point, yield strength, and proportional limit;
these points are close to the EL, although they differ by definition.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Fundamentally, elastic behavior involves interatomic bonding.
Because atoms are pulled apart, a fairly definite relationship exists
between stress and strain.
However, plastic behavior involves displacement along slip planes,
which are molecular, not atomic.
Plastic behavior therefore is not as linear as elastic behavior.
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Elastic Limit (EL):
• The EL is the greatest stress that can be
applied to the alloy without permanent
deformation.
• The EL determines the maximal elastic load
(Pmax) of a configuration.
• With respect only to the mechanical
properties of the wire, the maximal elastic
load varies directly and linearly with the EL.
Mechanical Properties of
the Orthodontic wires
In a given alloy (e.g., 18-8 stainless steel), a number of factors determine the
elastic limit.
1. Cold working
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Mechanical Properties of
the Orthodontic wiresCold working
The amount of work hardening produced during cold drawing of the wire sharply influences
the EL.
• Wires that have been considerably cold worked have a hard temper and therefore a
high EL.
• Small, round wires may have particularly high ELs because the percentage of reduction
by cold working is high.
• Also, the cold worked outer core becomes proportionately greater in a wire of smaller
cross section.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Mechanical Properties of
the Orthodontic wiresCold working
Too much work hardening, however, produces a structurally undesirable wire that becomes
highly brittle and may fracture during normal use in the mouth.
Far better is to have a slightly lower EL so that an orthodontic member can deform
permanently rather than break under accidental loading.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Mechanical Properties of
the Orthodontic wiresWork hardening VS. Anodic reduction
Because the work hardening required to reduce the diameter of a wire increases the EL,
Anodic reduction is a poor method for reducing the size of the wire.
Anodic reduction does not cold work a metal; therefore, the wire produced by that method
has a lower EL than a work-hardened one, a circumstance that could lead to permanent
deformation.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Raising EL
Many orthodontic alloys, such as Elgiloy and gold, can be heat treated to raise the EL,
but the most commonly used alloy, 18-8 stainless steel, cannot.
Stress relief process at 8508°F for 3 minutes or longer raises the apparent elastic limit of 18-8
stainless steel.
Stress relief removes undesirable residual stress introduced during manufacturing and during
fabrication by the orthodontist.
Mechanical Properties of
the Orthodontic wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Modulus of Elasticity(E):
• Modulus of elasticity (E) is the
ratio of stress to strain.
• The mechanical property that
determines the load-deflection
rate of an orthodontic member is
the modulus of elasticity (E).
Mechanical Properties of
the Orthodontic wires
Load-deflection varies directly and linearly with Modulus of elasticity (E).
(in torsion, linearly and directly as the modulus of rigidity).
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Modulus of Elasticity(E):
• Steel has an Modulus of elasticity
(E) approximately 1.8 times
greater than that of gold.
• Unlike the Elastic limit (EL), the
Modulus of elasticity (E) is
constant for a given alloy and is
not influenced by work hardening
or heat treatment.
Mechanical Properties of
the Orthodontic wires
ELASTIC
PROPERTIES
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
The Basic Properties of Elastic Materials
The elastic behavior of any material is defined in terms of its stress–strain response to an
external load.
For orthodontic purposes, three major properties of beam materials are critical in defining
their clinical usefulness: strength, stiffness (or its inverse, springiness), and range.
Elastic Properties of the
Orthodontic wires
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
1.Strength
2.Stiffness/Springiness
3. Range
4.Resilience
5.Formability
The Basic Properties of Elastic Materials
First three major properties have an
important relationship:
Strength = Stiffness X Range
Elastic Properties of the
Orthodontic wires
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
The Basic Properties of Elastic Materials
1. Strength:
Three different points on a stress–strain diagram can be taken as representative of the
strength of a material.
1. Proportional
limit
2. Yield strength
3. Ultimate tensile
strength
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
2. Stiffness:
Stiffness and springiness are reciprocal properties:
Each is proportional to the slope of the elastic portion of the force–deflection curve.
The more vertical the slope, the stiffer the wire;
The more horizontal the slope, the springier the wire.
The Basic Properties of Elastic Materials
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
3. Range:
Range is defined as the distance that the wire will bend elastically before
permanent deformation occurs. (distance is measured in millimeters)
The Basic Properties of Elastic Materials
• If the wire is deflected beyond this point, it will not return to its original shape, but
clinically useful springback will occur unless the failure point is reached.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
The relative strength, stiffness, and range for stainless steel, TMA, and M-NiTi
wires (which would be the same for any wire size).
The Basic Properties of Elastic Materials
• Note that both TMA and M-NiTi have half the strength of steel;
• M-NiTi has slightly less stiffness but much more range than TMA.
Reference:
1. Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
2. Orthodontics, the art and science, 4th Edition, S.I.Bhalaji
4. Resilience: Area under the stress-strain curve out to the proportional limit.
Represents the energy storage capacity of wire, which is a combination of
strength and springiness. ¹
Resilience is the amount of force the wire can withstand before permanent deformation.
Archwires should exhibit high resilience so as to increase working range of appliance.²
5. Formability: Amount of permanent deformation that a wire can withstand before failing.
Represents the amount of permanent bending the wire will tolerate before it
breaks. ¹
The archwire material should exhibit high formability so as to bend the arch wire into desired
configuration such as coils, loops without fracturing the wire. ²
The Basic Properties of Elastic Materials
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Each of the major elastic properties—strength, stiffness, and
range—is substantially affected by the geometry of a beam.
Both the cross-section (whether the beam is circular, rectangular, or
square) and the length of a beam are of great significance in
determining its properties.
Geometry:
• Size and Shape (changes are independent of the material)
• Length and attachment
Effects on Elastic Properties of Beams
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Changing the diameter (d) of a beam, no matter how it is supported,
greatly affects its properties.
Doubling the diameter of a cantilever beam makes it 8 times as strong, but it is then only
1/16 as springy and has half the range.
Effects on Elastic Properties of Beams
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Changing either the length of a beam (whatever its size or the
material from which it is made ) OR the way in which it is attached
dramatically affects its properties.
Doubling the length of a cantilever beam cuts its strength in half (?) but makes
it 8 times as springy and gives it 4 times the range.
Effects on Elastic Properties of Beams
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Changing either the length of a beam OR the way in which it is
attached dramatically affects its properties.
If a beam is rigidly attached on both ends, it is twice as strong but only one-fourth as springy
as a beam of the same material and length that can slide over the abutments.
For this reason, the elastic properties of an orthodontic archwire are affected by whether it is
tied tightly or held loosely in a bracket.
Effects on Elastic Properties of Beams
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
The best balance of strength, springiness,
and range must be sought among the almost
innumerable possible combinations of beam
materials, diameters, and lengths.
IDEAL
ORTHODONTIC
WIRE
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Properties of Ideal Orthod
It should possess:
1) High Strength
2) Low Stiffness (in most applications)
3) High Range
4) High Formabililty
5) Material should be weldable or solderable
6) Reasonable in cost
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Properties of Ideal Orthod
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Ideal orthodontic wire for an active member:
gives a high maximal elastic load and a low load-
deflection rate.
What are Ideal
Orthodontic Alloys?
The orthodontist should look for alloys that have a
high EL and a low E.
In the reactive member of an appliance:
however, not only is a sufficiently high EL required,
but also a high E is desirable.
The ratio between the EL and E determines the desirability of the alloy:
the higher the ratio, the better the spring properties (M/F ratio, Load deflection
rate/Torque twist rate, Maximum elastic load/ moment) of the wire.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Four other properties of wire should be considered when evaluating an orthodontic wire:
1. resistant to corrosion
2. sufficiently ductile
3. fabricated in a soft state and later heat treated to hard temper.
4. easy soldering of attachments
What are Ideal
Orthodontic Alloys?
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Factors / Characteristics
that influence Selection of
desirable orthodontic wire
?
1. Wire Cross Section
2. Wire Length
3. Amount of Wire
4. Selection of the Proper Wire (Alloy
and Cross Section)
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
1. Wire Cross Section
Small changes in cross section can influence the maximal elastic load
and the load-deflection rate greatly.
The maximal elastic load varies directly as the third power of the
diameter of round wire, and the load deflection rate varies directly
as the fourth power of the diameter.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
The fact that the load-deflection rate varies as the fourth power of the diameter in round
wires suggests the crucial importance of selecting a proper cross section.
In selecting a proper cross section for the rigid reactive members of
an appliance, the load-deflection rate, rather than the maximal
elastic load, is the prime consideration.
Drawbacks to round wire:
1. Round wire must be properly oriented or activations may not operate in the intended
plane.
2. Round wire may rotate in the bracket and if certain loops are incorporated into the
configuration, these can roll into the gingiva or the cheek.
1. Wire Cross Section
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
What is the optimal cross section for a flexible member?
Generally, for multidirectional activations in which the
structural axis is bent in more than one plane, a circular
cross section is the structure of choice.
1. Wire Cross Section
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• Many orthodontic wire configurations undergo unidirectional
bending.
For example, an edgewise vertical loop used for anterior retraction has a structural axis
that bends in only one plane.
• For unidirectional bending, flat wire is the cross
section of choice.
• More energy can be absorbed into a spring made of a flat wire
than with any other cross section.
1. Wire Cross Section
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Advantages of Flat wires:
• Problem of orientation is much easier to solve than with a round
cross section.
• Can be anchored definitely into a tube or bracket so that it will not
spin during deactivation of a given spring.
• Can also be used in certain situations when considerable tooth
movement is required in one plane but limited tooth movement is
needed in the other.
1. Wire Cross Section
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
For the reactive member, square or rectangular wire is
superior to round wire because of the ease of orientation
and greater multidirectional rigidity of the former, which
leads to more definite control of the anchorage units.
In the edgewise mechanism the assumption may be made that greater rigidity is needed
buccolingually or labiolingually than occlusogingivally because an edgewise wire is used.
This may or may not be true, depending on the intended use of the edgewise mechanism.
1. Wire Cross Section
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
The length of a member may influence the maximal elastic load and the load-
deflection in a number of ways, depending on the configuration and loading of
the spring.
1. Loading the cantilever with a vertical force applied at the free
end.
2. Loading the cantilever with a couple applied at the free end.
2. Wire Length
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Figure 11-26 shows a cantilever attached at B with a vertical force applied at A.
The distance L represents the length of the cantilever measured parallel to its structural axis.
Load deflection rate ∝ 1/L³
Maximum elastic load ∝ 1/L
1.) Loading the cantilever with a vertical force applied at the free end:
2. Wire Length
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Increasing the length of the cantilever is a better way to reduce the
load-deflection rate than is reducing the cross section.
Increasing the length of the cantilever greatly reduces the load-deflection rate, yet the
maximal elastic load is not changed radically because it varies linearly with the length.
2. Wire Length
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
2.) Loading the cantilever by means of a couple or moment applied to the free end:
Load deflection rate ∝ 1/L²
Maximum elastic load – no effect
The length may be doubled or tripled, but the maximal elastic moment remains the same.
This is a most desirable type of loading because additional length can reduce the moment-
deflection rate, but the maximal elastic moment is not reduced. However, the principle can
be applied only if moments alone are required for a given tooth movement.
2. Wire Length
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• Additional length of wire may be incorporated in the form of loops
or helices or some other configuration. This tends to lower the load-
deflection rate and increase the range of action of the flexible
member. The maximal elastic load may or may not be affected.
• When a member is to incorporate additional wire, the parts of the
configuration where additional wire should be placed must be
located properly, and the form the additional wire should take must
be determined.
• If location and formation are done properly, lowering the load-
deflection rate without changing the maximal elastic load should be
possible merely by adding the least amount of wire that will achieve
these ends.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Consider the problem of the cantilever in relation to the placement of the additional wire.
The bending moment represents an internal moment resisting the
100-g force applied to the free end of the cantilever.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Significance of the bendingmoment:
Amount of bending at each cross section of the wire is directly
proportionate to the magnitude of the bending moment.
in other words,
The greater the bending moment at any particular cross section,
the more the wire is going to bend at that point.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
The optimal place for additional wire is at cross sections where the
bending moment is greatest.
In the case of the cantilever, the position for additional wire is at the point of
support because the bending moment is greatest there: 1000 g-mm.
• Helical coils can be used to reduce the load-deflection rate.
Figure 11-30 illustrates the proper positioning of a helical coil for this purpose.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• The load-deflection rate is maximally lowered for the amount of
wire used if the helix is placed at the point of support.
• Placement of additional coils at the point of support in a
cantilever does not change the maximal elastic load.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• A straight wire of a given length and a wire with numerous coils at
the point of support have identical maximal elastic loads,
provided they have the same length measured from the force to
the point of support.
• This should not be surprising because the maximal elastic load is
a function of this length of the configuration rather than of the
amount of wire incorporated into it.
This is true of many other configurations as well: the load-deflection rate can be lowered
without changing the maximal elastic load if additional wire is incorporated properly.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
How to Determine where the bending moment is greatest?
A practical way of deciding where these parts of a wire might be is to activate a
configuration and see where most of the bending or torsion occurs.
The sections where the bending or torsional moments are greatest are the cross sections
with the greatest stress.
The configuration of the additional wire should be such that maximal advantage can be
taken of the bending and torsional properties of the wire.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
• In short, the amount of wire used is not what is important in
achieving a desirably flexible member, but rather the placement
of the additional wire and its form.
• Additional wire should not be used in reactive or rigid members.
Loops and other types of configurations diminish the rigidity of
the wire and thus may be responsible for some loss of control
over the anchor units.
3. Amount of wire
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Selection of the proper size wire should be based:
1. Primarily on the load-deflection rate required.
2. Secondarily on the magnitude of the forces and
moments needed.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Many orthodontists select a cross section of wire based on two other factors, which,
although valid, are not as significant:
1) Eliminate the play between wire and bracket:
Some clinicians believe that increasingly heavier wires are needed in a replacement
technique to eliminate the play between wire and bracket.
2) Smaller the wire, the greater the maximum elastic deflection:
The smaller the wire, the more it can be deflected without permanent deformation. This
is true, but maximal elastic deflection varies inversely with the diameter of the wire.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Small differences in cross section produce big changes in load-deflection rates
because in round wires the load deflection rate varies as the fourth power of the
diameter. (Table 11-1).
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
In bending, the stiffness, or load-deflection rate, is determined by the
moment of inertia of the cross section of the wire with respect to the
neutral axis.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Clinicians are interested in the relative stiffness of the wire they use,
but they have neither the time nor the inclination to use engineering
formulas to determine these degrees of stiffness.
Therefore, a simple numbering system has been developed, based on engineering theory,
that gives the relative stiffness of wires of different cross sections if the material
composition of the wire is the same.
The cross-sectional stiffness number (Cs) uses 0.1-mm (0.004-inch) round wire as a base of 1.
A 0.006-inch wire has a Cs of 5.0, which means that for the same activation, 5 times as much
force is delivered.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Tables 11-2 and 11-3 list, under the Cs column, stiffness numbers based on nominal cross
sections. Manufacturing variation or mislabeling of wires obviously can change the actual
Cs significantly. Two Cs numbers are given for rectangular wires—one for the first-order
direction and one for the second-order direction.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Any two sections of wire can be compared for
stiffness simply by dividing the Cs number of one
into the other.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
The overall stiffness of an appliance (S) is determined by two factors:
1. Wire itself (Ws)
2. Design of the appliance (As)
S = Ws × As
where S is the appliance load-deflection rate (Stiffness);
Ws, the wire stiffness; and
As, the design stiffness factor.
In general terms
Appliance stiffness = wire stiffness × design stiffness
Wire stiffness =material stiffness × cross-sectional stiffness
Wire stiffness is determined by a cross-sectional property (e.g., moment of inertia) and a
materials property (the E).
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
A full range of forces can be obtained by varying the material of the wire while keeping the
cross section the same.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
1. Variable cross-section Principle:
The amount of play between the attachments and the wire can be varied, depending on
the stiffness required.
With small, low-stiffness wires, excessive play may lead to lack of control over tooth
movement.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
2. Variable-Modulus Principle:
Clinician determines the amount of play required before selecting the wire.
In some instances more play is needed to allow the brackets freedom of movement
along the arch wire.
In other situations minimal play is allowed to ensure good orientation and effective
third-order movement.
After the desired amount of play has been established, the correct wire stiffness
can be produced by using a material with a proper Ms.
In this way the play between the wire and the attachment is not dictated by the stiffness
required but rather is under the full control of the operator.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Selection of the Proper Wire
(Alloy and Cross Section)
2. Variable-Modulus Principle:
The variable-modulus principle allows the orthodontist to use oriented rectangular
wires or square wires in light force and heavy force applications and stabilization.
A rectangular wire orients in the bracket and thus offers greater control in delivering the
desired force system; it is easier to bend because the orientation of the wire can be
checked carefully.
More important, when placed in the brackets, the wire does not turn or twist,
allowing the forces to be dissipated in improper directions.
TYPES OF
ORTHODONTIC WIRES
Reference:
• Orthodontics, the art and science, 4th Edition, S.I.Bhalaji
• Up until the 193Os, the only orthodontic wires available were made of gold.
• Austenitic stainless steel, with its greater strength, higher modulus of elasticity, good
resistance to corrosion, and moderate costs, was introduced as an orthodontic wire in
1929, and shortly afterward gained popularity over gold.
History
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Stainless Steel (SS) Wires
Types of orthodontic wires
• Most commonly used: austenitic 18-8 stainless steel (contains chromium and nickel content of approximately 18% and 8%, respectively)
Characteristics:
• High resistance to Corrosion (by the formation of a passivated oxide layer, which blocks the further oxygen
diffusion to the underlying mass)
• Produce higher forces applied during shorter time periods (since they have
lower spring back ability).
• Store less energy compared to those of beta-titanium or nickel-
titanium.
• Can be soldered with different biomechanical attachments.
• The corrosion resistance of stainless steel is good in general (but releases nickel
and chromium in fewer amounts and may induce hypersensitivity reactions)
Kolokitha et al., concluded that orthodontic treatment is not related to an increased likelihood of
hypersensitivity reactions to nickel unless there is a history of skin piercing.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Stainless Steel (SS) Wires
Types of orthodontic wires
• Stainless steel wires have a lower bracket-wire friction than other
types of wires (this friction can be further reduced by using nanotechnology applications)
• Australian wires are a kind of stainless steel wires available in
different grades with gradually increasing stored energy values
(resiliency).
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Stainless Steel (SS) Wires
Types of orthodontic wires
• Properties of Stainless steel wires can be controlled by varying the
amount of cold working and annealing during manufacture.
• Steel is softened by annealing and hardened by cold working.
• Fully annealed stainless steel wires are soft and highly formable.
• Steel ligatures are made from such “dead soft” wire.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Stainless Steel (SS) Wires
Types of orthodontic wires
• “Super Grades” Steel wires:
possess impressive yield strength, are brittle and break if bend
sharply.
• “Regular Grades” Steel wires:
can be bent to almost any desired shape without breaking.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Cobalt-chromiumWires
Types of orthodontic wires
• Cobalt-chromium-nickel alloy known as elgiloy.
• These alloys were originally developed for use as watch spring by ELGIU national company.
• Available in different tempers depending on amount of cold work and are usually color-
coded.
Color codes
High spring tempers Red
Semispring temper Green
Soft or ductile tempers Yellow
High formability combined with increased elasticity and yield strength following heat
treatment by 10% and 20- 30%, respectively, have made Blue Elgiloy, a cobalt chromium
wire type, popular in clinical practice.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Cobalt-chromiumWires
Types of orthodontic wires
Characteristics:
• Easy to bend.
• Can be heat hardened at 482° C for about 7 minutes after
manipulation to increase hardness (strength) approximately equal
to that of stainless steel.
• Non-heat treated cobalt-chromium wires have a smaller spring-
back than stainless steel wires
• Excellent resistance to tarnish and corrosion.
• Inexpensive and can be soldered (fluoride fluxes are used) and
welded.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Cobalt-chromiumWires
Types of orthodontic wires
COMPARISON WITH STAINLESS STEEL:
• Elgiloy, the cobalt–chromium alloy, has the advantage that it can be supplied in a
softer and therefore more formable state, and the wires can be hardened by
heat treatment after being shaped.
The heat treatment increases strength significantly.
• After heat treatment, the softest Elgiloy becomes equivalent to regular stainless
steel, while harder initial grades are equivalent to the “super” steels.
• This material, however, had almost disappeared by the end of the twentieth
century because of its additional cost relative to stainless steel and the extra step
of heat treatment to obtain optimal properties.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Types of orthodontic wires
Shape Memory Alloys:
1. Nickel titanium (nitinol) - William F. Buehler
2. Superelastic NiTi wires
3. TMA
4. Titanium niobium
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Beta TitaniumWires
Types of orthodontic wires
• Introduced in 1979
• Also known as titanium-molybdenium alloy (TMA) or Titanium Niobium.
Characteristics:
• Modulus of elasticity of these wires is lower than half of stainless
steel wires and almost twice that of Nitinol.
• Demonstrate good formability, (but should not be strongly bent for there is a risk of breaking).
• Electrical welding of biomechanical attachments is possible, (but overheating
should not be done as it makes the wire more brittle).
• According to a recent study, beta-titanium wires are better in terms
of joinability than stainless steel wires (since they demonstrate higher resilience and better surface and
structural characteristics, which indicates only a minor change in wire properties after welding).
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Beta TitaniumWires
Types of orthodontic wires
Characteristics:
• Resistance to corrosion is similar to that of cobalt chromium and
stainless steel wires.
• Good biocompatible material (due to the absence of nickel).
• Resistance to corrosion is due to the formation of a surface
passivation oxide layer (but exposure to fluoride agents leads to the degradation, subsequent corrosion, and qualitative alteration
of the wire’s surface).
• Highly expensive
• More bracket-wire friction than any other alloy
Alpha-beta titanium alloy is also called as TiMolium, it has stiffness and other characteristics (such as
elasticity and yield strength) are between the values set for stainless steel and beta-titanium wires
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Beta TitaniumWires
Types of orthodontic wires
Characteristics:
• TMA has a modulus of elasticity between that of steel and nitinol
(approximately 0.4 times that of stainless steel).
• TMA can be deflected up to 2 times as much as steel without
permanent deformation.
• Unlike Nitinol, TMA is not significantly altered by the placement of
bends and twists and has good ductility, equivalent to or slightly
better than that of stainless steel, and can be welded without
significant reduction in yield strength.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Nickel Titanium Wires
Types of orthodontic wires
• Exceptional ability to apply light force over a large range of activations.
This phase transition allows certain NiTi alloys to exhibit two remarkable
properties found in no other dental materials—shape memory and
superelasticity.
Martensitic form
Lower temperatures
Higher stress
Austenitic form
Higher temperatures
Lower stress
The uniqueness of NiTi is that the transition between the two structures is fully reversible
and occurs at a remarkably low temperature.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Nickel Titanium Wires
Types of orthodontic wires
 The original Nitinol wires marketed under that name in the late 1970s by Unitek were M-
NiTi wires, with no application of phase transition effects.
 M-NiTi remains useful, primarily in the later stages of treatment when flexible but larger
and somewhat stiffer wires are needed.
M-NiTi: NiTi wires stabilized in the martensitic form are referred to as M-NiTi.
A-NiTi: NiTi wires displaying martensite–austenite transitions are referred to as A-NiTi.
 In the late 1980s, new nickel–titanium wires with an austenitic grain structure (A-NiTi)
appeared.
 These wires exhibit superelasticity and/or shape memory in various degrees.
 The properties of A-NiTi have quickly made it the preferred material for orthodontic
applications in which a long range of activation with relatively constant force is needed
(i.e., for initial archwires and coil springs).
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Nickel Titanium Wires
Types of orthodontic wires
Shape memory: refers to the ability of the material to “remember” its original
shape after being plastically deformed while in the martensitic form.
Superelasticity: refers to the very large reversible strains that certain NiTi wires can
withstand due to the martensite-austenite phase transition.
• Materials displaying superelasticity are austenitic alloys that undergo a transition to martensite in
response to stress—a mechanical analogue to the thermally induced shape memory effect.
• Superelastic materials must exhibit a reversible phase change at a close transition temperature,
which must be lower than room temperature for the austenite phase to exist clinically.
Shape memory is a thermal reaction and superelasticity is a mechanical one, they are inherently linked.
Reference:
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Nickel Titanium Wires
Types of orthodontic wires
Thermoelasticity:
• In a typical application, a certain shape is set while the alloy is maintained at an elevated
temperature, above the martensite–austenite transition temperature.
• When the alloy is cooled below the transition temperature, it can be plastically
deformed, but the original shape is restored when it is heated enough to regain an
austenitic structure.
• This temperature-induced change in crystal structure (called thermoelasticity) was
important to the original nitinol use in the space program but proved difficult to exploit
in orthodontic applications.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Nickel Titanium Wires
Types of orthodontic wires
• A wrought Ni-Ti alloy known as Nitinol (Nickel-Titanium naval ordinance laboratory) was
introduced in 1972.
Characteristics:
• High resiliency.
• Higher energy storage capacity
• Shape memory or thermal memory.
• Pseudoelastic or superelasticity.
• Limited formability.
• Cannot be welded or fused.
The friction develops at bracket-wire interface is more with Nitinol wires followed by beta-titanium,
stainless steel and chromium-cobalt wires
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Nickel Titanium Wires
Types of orthodontic wires
Two major phases
One intermediate phase
Austenitic Phase
Martensitic phase
• At higher temperature
• Body centered cubic
structure (BCC)
• At lower temperature
• hexagonal close packed
structure (HCP)
Delays the transition from austenite to martensite
upon cooling until lower temperatures are achieved.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Nickel Titanium Wires
Types of orthodontic wires
Shape memory achieved by first establishing a shape
at temperatures near 482° C.
If the appliance wire is then cooled and formed into a
second shape and heated through a lower transition
temperature range (TTR), the wire will return to its original
shape.
The cobalt content is used to control the transition
temperature range, which can be near mouth temperature.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Nickel Titanium Wires
Types of orthodontic wires
Phase transformation (from BCC austenitic to HCP
martensitic) can be seen by decreasing the temperature
from an elevated temperature
and can also be induced by the application of stress and a
volumetric change is associated during this transition.
This transformation results in two unique features such as
shape memory and pseudoelasticity or superelasticity.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Nickel Titanium Wires
Types of orthodontic wires
Pseudoelasticity or Superelasticity Inducing the austenitic
to martensitic transformation by stress can produce
superelasticity, a phenomena that is employed with Ni –
Ti wires.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Nickel Titanium Wires
Types of orthodontic wires
The shape memory principle is not used clinically. Instead, nitinol is
used for its low force and high springback.
The most dramatic characteristic of nitinol, however, is its resistance
to permanent deformation.
NiTi wires can be activated over twice the distance of stainless steel,
with minimal permanent deformation.
Nitinol is more brittle than stainless steel and cannot be joined by
soldering or welding.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Superelastic Ni-Ti Wires
Types of orthodontic wires
 Unlike nitinol, these alloys have a much lower transition
temperature—either slightly below or slightly higher than mouth
temperature.
 Generally speaking, the austenitic form of these alloys has a slightly
higher springback than nitinol and may be less brittle.
 The superelastic NiTi wires are available in different degrees of
stiffness.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Superelastic Ni-Ti Wires
Types of orthodontic wires
 Although the final transition temperature of some superelastic NiTi
wires is below mouth temperature, others are not activated fully
until they reach 37°C or higher.
 These wires have both superelastic and shape memory properties.
 Generally, the heat treatment process performed during
manufacture to raise the transition temperature allows for wires
that deliver lower forces at mouth temperature;
 hence the orthodontist may be able to achieve full bracket
engagement with larger wires earlier in treatment.
Reference:
• Orthodontics current principles and techniques; Grabber, 5th edition
Titanium Niobium Wires
Types of orthodontic wires
Characteristics:
• Low springback (equivalent to stainless steel)
• Much less stiff than TMA
• Useful when a highly formable wire with low forces in small
activations is required.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Chinese Ni-Ti Wires
Types of orthodontic wires
The Chinese NiTi wires were recommended by Burstone et
al in 1985.
They exhibited 4.4 times the spring-back of stainless steel
wires and 1.6 times the spring-back of the original Nitinol
wires if a constant force in the middle of its deactivation
range.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Japanese Ni-Ti Wires
Types of orthodontic wires
The Japanese NiTi wires was introduced by Miura et al. in
1986
Their properties were almost similar to Chinese NiTi wires.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Multistranded Wires
Types of orthodontic wires
• Made of a varying number of stainless steel wire strands coaxially placed or coiled around
each other in different configurations.
Characteristics:
• Deliver low forces
• Low stiffness
• Low resilience
• Inexpensive than titanium alloys
• Higher friction at bracket-wire interface compared to NiTi wires and
single-stranded stainless steel wires
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Esthetic Wires
Fiber-reinforced composite arch wires
Types of orthodontic wires
Characteristics:
• Highly esthetic
• Biocompatible
• Hydrolytic stability
• Less water sorption
• Stiffness is same as metallic wires
• Post processing formability
• Sliding mechanics are good
• Wearing of these arch wires at the interface chances of leaching of
glass fibers within the oral cavity.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Esthetic Wires
Teflon coated stainless steel arch wires
Types of orthodontic wires
• Teflon is coated on stainless steel wire by an atomic process that
forms a layer of about 20-25ìm thickness on the wire that imparts
to the wire a hue which is similar to that of natural teeth.
• Teflon coating protects the underlying wire from the corrosion
process.
• However, corrosion of the underlying wire is likely to take place if it
is used for longer period in the oral cavity since this coating is
subject to flaws that may occur during clinical use.
Reference:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014)
Types of orthodontic wires
Other Esthetic wires:
 Optiflex
 Bioforce wires
 Marsenol
 Lee White wire
REFERENCES:
Articles:
• Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif.
Organs, 28(1), 32-36 (2014)
Books:
• Orthodontics current principles and techniques; Grabber, 5th edition
• Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.
Dr Abbas Naseem
abbas_naseem@yahoo.com
Dated: November 26th , 2014

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Wire selection in orthodontics / Orthodontics wires

  • 2. Learning Outcomes …….. 1. Basic Terminology 2. Mechanical properties of orthodontic wire 3. Elastic properties of orthodontic wire 4. Properties of ideal orthodontic wire 5. What are the ideal orthodontic alloys 6. Characteristics/factors that influence selection of desirable orthodontic wire • Wire cross-section • Wire length • Amount of wire • Selection of proper wire (Alloy and Cross Section) 7. History/Evolution of archwires 8. Types of archwires
  • 3. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Basic Terms Stress: Force per unit area. Stress is the internal distribution of the load. Strain: Deflection per unit length. Internal distortion produced by the load.
  • 4. Reference: 1. Orthodontics, the art and science, 4th Edition, S.I.Bhalaji 2. Textbook of orthodontics, 2nd Edition, Gurkeerat singh Basic Terms Stiffness: The presence of low stiffness provides the ability to apply lower forces and a more constant force over time. ¹ Stiffness / Load defection rate: This is the force magnitude delivered by an appliance and is proportional to modulus of elasticity (E). ² Low stiffness leads to an ability to apply lower forces, a more constant force to be delivered overtime and greater ease and accuracy in applying a given force. Spring back: It is the measure of how far a wire can be deflected without causing permanent deformation. It is also called elastic deflection. The archwire should ideally possess high springback, which results in an increase in its range of action. ¹ Spring back / maximum elastic deflection / working range: ratio of yield strength(YS) to modulus of elasticity(E) of the material. ² Higher springback provides ability to apply large activations with a resultant increase in working time of appliance, thus decreasing number of archwire changes.
  • 5. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. The range is the distance along the X-axis to the point at which permanent deformation occurs (usually taken as the yield point, at which 0.1%permanent deformation has occurred). Basic Terms Stress and strain are internal characteristics that can be calculated from measurements of force and deflection, so the general shapes of force–deflection and stress–strain curves are similar. The stiffness of the material is given by the slope of the linear portion of the curve. Clinically useful springback occurs if the wire is deflected beyond the yield point (as to the point indicated here as “arbitrary clinical loading”), but it no longer returns to its original shape.
  • 6. Reference: 1. Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. 2. Orthodontics, the art and science, 4th Edition, S.I.Bhalaji Basic Terms Resilience: Area under the stress-strain curve out to the proportional limit. Represents the energy storage capacity of wire, which is a combination of strength and springiness. ¹ Resilience is the amount of force the wire can withstand before permanent deformation. Archwires should exhibit high resilience so as to increase working range of appliance.² Formability: Amount of permanent deformation that a wire can withstand before failing. Represents the amount of permanent bending the wire will tolerate before it breaks. ¹ The archwire material should exhibit high formability so as to bend the arch wire into desired configuration such as coils, loops without fracturing the wire. ²
  • 7. Reference: • Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:8-9) Resilience: The energy absorbed by a material in undergoing elastic deformation up to the elastic limit. Toughness: The total amount of energy which a material can absorb upto point of fracture. Basic Terms
  • 8. Reference: • Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:11) Stress & Strain Relationship (Cause and effect Relationship)• Use to characterise the mechanical properties of materials. • The application of an external force, producing a stress within a material, results in a change in dimension or strain within the body. P: Propotional Limit: Linear relationship between stress and strain upto point P. • Further increases in stress cause proportionally greater increases in strain until the material fractures at point T. E: Yield Stress • Corresponds to the stress beyond which strains are not fully recovered. • Maximum stress which a material can withstand without undergoing some permanent deformation. T: fracture stress (Tensile/Compressive strength)
  • 9. Reference: 1. Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:11) 2. Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Yield stress is difficult to characterise experimentally… ¹ It requires a series of experiments in which stress is gradually increased then released and observations on elastic recovery made. As a consequence of these experimental difficulties, the proportional limit is often used to give an approximation to the value of the yield stress. Hence, High value of proportional limit indicates a sample of material is more likely to withstand applied stress without permanent deformation. Proportional limit VS. Yield stress Precisely determining proportional point can be difficult, so a more practical indicator is the yield strength. ² True elastic limit ?
  • 10. Reference: • Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:11) • Rigid • Strong • Tough • Ductile • Rigid • Strong • Brittle • Flexible • Weak • Brittle • Flexible • Tough • Rigid • Weak • Brittle • Flexible • Resilient
  • 11. “Stress and strain relationship used to characterise the mechanical properties of materials.” - Applied Dental Materials, 9th Edition, John F. Mcable (Chapter:2. page:8) The Basic Properties of Elastic Materials – “The elastic behavior of any material is defined in terms of its stress–strain response to an external load.” - Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. (Chapter:9. page:312) MECJANICAL PROPERTIES VS. ELASTIC PROPERTIES
  • 14. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition The mechanical properties of an alloy to be used in an orthodontic wire can be described on at least three levels. 1. Observational level 2. Stress-strain level 3. Atomic and molecular level Mechanical Properties of the Orthodontic wires
  • 15. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • Basic Behavior of Alloys • Elastic Limit • Modulus of Elasticity Mechanical Properties of the Orthodontic wires
  • 16. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Active and Reactive Members The active member is the part involved in tooth movement. The reactive member serves as anchorage and involves the teeth that will not be displaced. Specifically of interest are three important characteristics involving active and reactive members: 1. Moment-to-Force Ratio 2. Load-deflection Rate / Torque Twist Rate 3. Maximum elastic load / moment Mechanical Properties of the Orthodontic wires
  • 17. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition All three of the important characteristics of an orthodontic appliance 1. Moment-to-Force Ratio 2. Load-deflection Rate / Torque Twist Rate 3. Maximum elastic load / moment are found within the elastic range of an orthodontic wire and therefore may be called spring characteristics. Mechanical Properties of the Orthodontic wires
  • 18. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition On the subclinical level the three primary objectives: 1. Control the center of rotation of the tooth. 2. Produce desirable stress levels in the PDL. 3. Maintain a relatively constant level of stress. At the clinical level of observation: the focus becomes the forces and moments produced by an orthodontic appliance. Mechanical Properties of the Orthodontic wires
  • 19. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 1. Moment-to-Force Ratio Mechanical Properties of the Orthodontic wires
  • 20. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Force—a load applied to an object that will tend to move it to a different position in space. Moment—a measure of the tendency to rotate an object around some point. A moment is generated by a force acting at a distance. Mechanical Properties of the Orthodontic wires
  • 21. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Couple—two forces equal in magnitude and opposite in direction. The result of applying two forces in this way is a pure moment, since the translatory effect of the forces cancels out. A couple will produce pure rotation, spinning the object around its center of resistance. Mechanical Properties of the Orthodontic wires
  • 22. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Center of resistance—The center of resistance (CR) for any tooth is at the approximate midpoint of the embedded portion of the root. Center of rotation—The point around which rotation actually occurs when an object is being moved. Mechanical Properties of the Orthodontic wires
  • 23. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 1. Moment-to-Force Ratio Mechanical Properties of the Orthodontic wires • To produce different types of tooth movement, the ratio between the applied moment and the force on the crown must be changed. • As the M/F ratio is altered, the center of rotation changes. • Crown tipping, translation, and root movement are examples of different types of tooth movement that can be produced with the proper M/F ratio. • The M/F ratio determines the control the orthodontic appliance has over the active and reactive units. • Specifically, it controls the center of rotation of the tooth or a group of teeth.
  • 24. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 2. Load-deflection Rate / Torque Twist Rate Mechanical Properties of the Orthodontic wires • Force produced per unit activation. OR The force required per unit deflection. • is a factor in the delivery of a relatively constant force. • As the load deflection rate declines for a tooth that is moving under a continuous force, the change in force value is reduced. For active members a low load-deflection rate is desirable for two important reasons: 1. Maintains a more desirable stress level in the PDL because the force on a tooth does not radically change magnitude every time the tooth has been displaced. 2. Offers greater accuracy in controlling force magnitude.
  • 25. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 2. Load-deflection Rate / Torque Twist Rate Mechanical Properties of the Orthodontic wires The reactive member it should have a high load-deflection rate. (should be relatively rigid)
  • 26. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 3. Maximum elastic load / moment Mechanical Properties of the Orthodontic wires Greatest force or moment that can be applied to a member without causing permanent deformation.
  • 27. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • Basic Behavior of Alloys Mechanical Properties of the Orthodontic wiresPmax: • A point where load and deflection are no longer proportionate. • Near Pmax, permanent deformation is being produced in the spring, which will not return to its original shape. • Pmax represents the highest load that can be placed on the spring without permanent deformation; that is, the maximal elastic load. Hooke’s Law
  • 28. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Mechanical Properties of the Orthodontic wiresElastic Limit (EL) The EL is the greatest stress that can be applied to the alloy without permanent deformation. Modulus of elasticity (E) this mechanical property determines the load-deflection rate of a spring. Stress in a wire is force per unit area applied to a cross section. Strain is deflection per unit length of the wire. Modulus of elasticity (E) is the ratio of stress to strain.
  • 29. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Mechanical Properties of the Orthodontic wires The EL is analogous to the maximal elastic load (Pmax) and therefore is the mechanical property that determines the ability of a member to withstand permanent deformation.
  • 30. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Mechanical Properties of the Orthodontic wires A number of other terms describe this general part of the curve (O- EL), such as yield point, yield strength, and proportional limit; these points are close to the EL, although they differ by definition.
  • 31. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Fundamentally, elastic behavior involves interatomic bonding. Because atoms are pulled apart, a fairly definite relationship exists between stress and strain. However, plastic behavior involves displacement along slip planes, which are molecular, not atomic. Plastic behavior therefore is not as linear as elastic behavior. Mechanical Properties of the Orthodontic wires
  • 32. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Elastic Limit (EL): • The EL is the greatest stress that can be applied to the alloy without permanent deformation. • The EL determines the maximal elastic load (Pmax) of a configuration. • With respect only to the mechanical properties of the wire, the maximal elastic load varies directly and linearly with the EL. Mechanical Properties of the Orthodontic wires In a given alloy (e.g., 18-8 stainless steel), a number of factors determine the elastic limit. 1. Cold working
  • 33. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Mechanical Properties of the Orthodontic wiresCold working The amount of work hardening produced during cold drawing of the wire sharply influences the EL. • Wires that have been considerably cold worked have a hard temper and therefore a high EL. • Small, round wires may have particularly high ELs because the percentage of reduction by cold working is high. • Also, the cold worked outer core becomes proportionately greater in a wire of smaller cross section.
  • 34. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Mechanical Properties of the Orthodontic wiresCold working Too much work hardening, however, produces a structurally undesirable wire that becomes highly brittle and may fracture during normal use in the mouth. Far better is to have a slightly lower EL so that an orthodontic member can deform permanently rather than break under accidental loading.
  • 35. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Mechanical Properties of the Orthodontic wiresWork hardening VS. Anodic reduction Because the work hardening required to reduce the diameter of a wire increases the EL, Anodic reduction is a poor method for reducing the size of the wire. Anodic reduction does not cold work a metal; therefore, the wire produced by that method has a lower EL than a work-hardened one, a circumstance that could lead to permanent deformation.
  • 36. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Raising EL Many orthodontic alloys, such as Elgiloy and gold, can be heat treated to raise the EL, but the most commonly used alloy, 18-8 stainless steel, cannot. Stress relief process at 8508°F for 3 minutes or longer raises the apparent elastic limit of 18-8 stainless steel. Stress relief removes undesirable residual stress introduced during manufacturing and during fabrication by the orthodontist. Mechanical Properties of the Orthodontic wires
  • 37. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Modulus of Elasticity(E): • Modulus of elasticity (E) is the ratio of stress to strain. • The mechanical property that determines the load-deflection rate of an orthodontic member is the modulus of elasticity (E). Mechanical Properties of the Orthodontic wires Load-deflection varies directly and linearly with Modulus of elasticity (E). (in torsion, linearly and directly as the modulus of rigidity).
  • 38. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Modulus of Elasticity(E): • Steel has an Modulus of elasticity (E) approximately 1.8 times greater than that of gold. • Unlike the Elastic limit (EL), the Modulus of elasticity (E) is constant for a given alloy and is not influenced by work hardening or heat treatment. Mechanical Properties of the Orthodontic wires
  • 40. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. The Basic Properties of Elastic Materials The elastic behavior of any material is defined in terms of its stress–strain response to an external load. For orthodontic purposes, three major properties of beam materials are critical in defining their clinical usefulness: strength, stiffness (or its inverse, springiness), and range. Elastic Properties of the Orthodontic wires
  • 41. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. 1.Strength 2.Stiffness/Springiness 3. Range 4.Resilience 5.Formability The Basic Properties of Elastic Materials First three major properties have an important relationship: Strength = Stiffness X Range Elastic Properties of the Orthodontic wires
  • 42. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. The Basic Properties of Elastic Materials 1. Strength: Three different points on a stress–strain diagram can be taken as representative of the strength of a material. 1. Proportional limit 2. Yield strength 3. Ultimate tensile strength
  • 43. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. 2. Stiffness: Stiffness and springiness are reciprocal properties: Each is proportional to the slope of the elastic portion of the force–deflection curve. The more vertical the slope, the stiffer the wire; The more horizontal the slope, the springier the wire. The Basic Properties of Elastic Materials
  • 44. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. 3. Range: Range is defined as the distance that the wire will bend elastically before permanent deformation occurs. (distance is measured in millimeters) The Basic Properties of Elastic Materials • If the wire is deflected beyond this point, it will not return to its original shape, but clinically useful springback will occur unless the failure point is reached.
  • 45. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. The relative strength, stiffness, and range for stainless steel, TMA, and M-NiTi wires (which would be the same for any wire size). The Basic Properties of Elastic Materials • Note that both TMA and M-NiTi have half the strength of steel; • M-NiTi has slightly less stiffness but much more range than TMA.
  • 46. Reference: 1. Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. 2. Orthodontics, the art and science, 4th Edition, S.I.Bhalaji 4. Resilience: Area under the stress-strain curve out to the proportional limit. Represents the energy storage capacity of wire, which is a combination of strength and springiness. ¹ Resilience is the amount of force the wire can withstand before permanent deformation. Archwires should exhibit high resilience so as to increase working range of appliance.² 5. Formability: Amount of permanent deformation that a wire can withstand before failing. Represents the amount of permanent bending the wire will tolerate before it breaks. ¹ The archwire material should exhibit high formability so as to bend the arch wire into desired configuration such as coils, loops without fracturing the wire. ² The Basic Properties of Elastic Materials
  • 47. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Each of the major elastic properties—strength, stiffness, and range—is substantially affected by the geometry of a beam. Both the cross-section (whether the beam is circular, rectangular, or square) and the length of a beam are of great significance in determining its properties. Geometry: • Size and Shape (changes are independent of the material) • Length and attachment Effects on Elastic Properties of Beams
  • 48. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Changing the diameter (d) of a beam, no matter how it is supported, greatly affects its properties. Doubling the diameter of a cantilever beam makes it 8 times as strong, but it is then only 1/16 as springy and has half the range. Effects on Elastic Properties of Beams
  • 49. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Changing either the length of a beam (whatever its size or the material from which it is made ) OR the way in which it is attached dramatically affects its properties. Doubling the length of a cantilever beam cuts its strength in half (?) but makes it 8 times as springy and gives it 4 times the range. Effects on Elastic Properties of Beams
  • 50. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Changing either the length of a beam OR the way in which it is attached dramatically affects its properties. If a beam is rigidly attached on both ends, it is twice as strong but only one-fourth as springy as a beam of the same material and length that can slide over the abutments. For this reason, the elastic properties of an orthodontic archwire are affected by whether it is tied tightly or held loosely in a bracket. Effects on Elastic Properties of Beams
  • 51. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. The best balance of strength, springiness, and range must be sought among the almost innumerable possible combinations of beam materials, diameters, and lengths.
  • 53. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Properties of Ideal Orthod It should possess: 1) High Strength 2) Low Stiffness (in most applications) 3) High Range 4) High Formabililty 5) Material should be weldable or solderable 6) Reasonable in cost
  • 54. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Properties of Ideal Orthod
  • 55. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Ideal orthodontic wire for an active member: gives a high maximal elastic load and a low load- deflection rate. What are Ideal Orthodontic Alloys? The orthodontist should look for alloys that have a high EL and a low E. In the reactive member of an appliance: however, not only is a sufficiently high EL required, but also a high E is desirable. The ratio between the EL and E determines the desirability of the alloy: the higher the ratio, the better the spring properties (M/F ratio, Load deflection rate/Torque twist rate, Maximum elastic load/ moment) of the wire.
  • 56. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Four other properties of wire should be considered when evaluating an orthodontic wire: 1. resistant to corrosion 2. sufficiently ductile 3. fabricated in a soft state and later heat treated to hard temper. 4. easy soldering of attachments What are Ideal Orthodontic Alloys?
  • 57. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Factors / Characteristics that influence Selection of desirable orthodontic wire ? 1. Wire Cross Section 2. Wire Length 3. Amount of Wire 4. Selection of the Proper Wire (Alloy and Cross Section)
  • 58. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 1. Wire Cross Section Small changes in cross section can influence the maximal elastic load and the load-deflection rate greatly. The maximal elastic load varies directly as the third power of the diameter of round wire, and the load deflection rate varies directly as the fourth power of the diameter.
  • 59. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition The fact that the load-deflection rate varies as the fourth power of the diameter in round wires suggests the crucial importance of selecting a proper cross section. In selecting a proper cross section for the rigid reactive members of an appliance, the load-deflection rate, rather than the maximal elastic load, is the prime consideration. Drawbacks to round wire: 1. Round wire must be properly oriented or activations may not operate in the intended plane. 2. Round wire may rotate in the bracket and if certain loops are incorporated into the configuration, these can roll into the gingiva or the cheek. 1. Wire Cross Section
  • 60. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition What is the optimal cross section for a flexible member? Generally, for multidirectional activations in which the structural axis is bent in more than one plane, a circular cross section is the structure of choice. 1. Wire Cross Section
  • 61. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • Many orthodontic wire configurations undergo unidirectional bending. For example, an edgewise vertical loop used for anterior retraction has a structural axis that bends in only one plane. • For unidirectional bending, flat wire is the cross section of choice. • More energy can be absorbed into a spring made of a flat wire than with any other cross section. 1. Wire Cross Section
  • 62. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Advantages of Flat wires: • Problem of orientation is much easier to solve than with a round cross section. • Can be anchored definitely into a tube or bracket so that it will not spin during deactivation of a given spring. • Can also be used in certain situations when considerable tooth movement is required in one plane but limited tooth movement is needed in the other. 1. Wire Cross Section
  • 63. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition For the reactive member, square or rectangular wire is superior to round wire because of the ease of orientation and greater multidirectional rigidity of the former, which leads to more definite control of the anchorage units. In the edgewise mechanism the assumption may be made that greater rigidity is needed buccolingually or labiolingually than occlusogingivally because an edgewise wire is used. This may or may not be true, depending on the intended use of the edgewise mechanism. 1. Wire Cross Section
  • 64. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition The length of a member may influence the maximal elastic load and the load- deflection in a number of ways, depending on the configuration and loading of the spring. 1. Loading the cantilever with a vertical force applied at the free end. 2. Loading the cantilever with a couple applied at the free end. 2. Wire Length
  • 65. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Figure 11-26 shows a cantilever attached at B with a vertical force applied at A. The distance L represents the length of the cantilever measured parallel to its structural axis. Load deflection rate ∝ 1/L³ Maximum elastic load ∝ 1/L 1.) Loading the cantilever with a vertical force applied at the free end: 2. Wire Length
  • 66. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Increasing the length of the cantilever is a better way to reduce the load-deflection rate than is reducing the cross section. Increasing the length of the cantilever greatly reduces the load-deflection rate, yet the maximal elastic load is not changed radically because it varies linearly with the length. 2. Wire Length
  • 67. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition 2.) Loading the cantilever by means of a couple or moment applied to the free end: Load deflection rate ∝ 1/L² Maximum elastic load – no effect The length may be doubled or tripled, but the maximal elastic moment remains the same. This is a most desirable type of loading because additional length can reduce the moment- deflection rate, but the maximal elastic moment is not reduced. However, the principle can be applied only if moments alone are required for a given tooth movement. 2. Wire Length
  • 68. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • Additional length of wire may be incorporated in the form of loops or helices or some other configuration. This tends to lower the load- deflection rate and increase the range of action of the flexible member. The maximal elastic load may or may not be affected. • When a member is to incorporate additional wire, the parts of the configuration where additional wire should be placed must be located properly, and the form the additional wire should take must be determined. • If location and formation are done properly, lowering the load- deflection rate without changing the maximal elastic load should be possible merely by adding the least amount of wire that will achieve these ends. 3. Amount of wire
  • 69. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Consider the problem of the cantilever in relation to the placement of the additional wire. The bending moment represents an internal moment resisting the 100-g force applied to the free end of the cantilever. 3. Amount of wire
  • 70. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Significance of the bendingmoment: Amount of bending at each cross section of the wire is directly proportionate to the magnitude of the bending moment. in other words, The greater the bending moment at any particular cross section, the more the wire is going to bend at that point. 3. Amount of wire
  • 71. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition The optimal place for additional wire is at cross sections where the bending moment is greatest. In the case of the cantilever, the position for additional wire is at the point of support because the bending moment is greatest there: 1000 g-mm. • Helical coils can be used to reduce the load-deflection rate. Figure 11-30 illustrates the proper positioning of a helical coil for this purpose. 3. Amount of wire
  • 72. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • The load-deflection rate is maximally lowered for the amount of wire used if the helix is placed at the point of support. • Placement of additional coils at the point of support in a cantilever does not change the maximal elastic load. 3. Amount of wire
  • 73. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • A straight wire of a given length and a wire with numerous coils at the point of support have identical maximal elastic loads, provided they have the same length measured from the force to the point of support. • This should not be surprising because the maximal elastic load is a function of this length of the configuration rather than of the amount of wire incorporated into it. This is true of many other configurations as well: the load-deflection rate can be lowered without changing the maximal elastic load if additional wire is incorporated properly. 3. Amount of wire
  • 74. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition How to Determine where the bending moment is greatest? A practical way of deciding where these parts of a wire might be is to activate a configuration and see where most of the bending or torsion occurs. The sections where the bending or torsional moments are greatest are the cross sections with the greatest stress. The configuration of the additional wire should be such that maximal advantage can be taken of the bending and torsional properties of the wire. 3. Amount of wire
  • 75. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition • In short, the amount of wire used is not what is important in achieving a desirably flexible member, but rather the placement of the additional wire and its form. • Additional wire should not be used in reactive or rigid members. Loops and other types of configurations diminish the rigidity of the wire and thus may be responsible for some loss of control over the anchor units. 3. Amount of wire
  • 76. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) Selection of the proper size wire should be based: 1. Primarily on the load-deflection rate required. 2. Secondarily on the magnitude of the forces and moments needed.
  • 77. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) Many orthodontists select a cross section of wire based on two other factors, which, although valid, are not as significant: 1) Eliminate the play between wire and bracket: Some clinicians believe that increasingly heavier wires are needed in a replacement technique to eliminate the play between wire and bracket. 2) Smaller the wire, the greater the maximum elastic deflection: The smaller the wire, the more it can be deflected without permanent deformation. This is true, but maximal elastic deflection varies inversely with the diameter of the wire.
  • 78. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) Small differences in cross section produce big changes in load-deflection rates because in round wires the load deflection rate varies as the fourth power of the diameter. (Table 11-1).
  • 79. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) In bending, the stiffness, or load-deflection rate, is determined by the moment of inertia of the cross section of the wire with respect to the neutral axis.
  • 80. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) Clinicians are interested in the relative stiffness of the wire they use, but they have neither the time nor the inclination to use engineering formulas to determine these degrees of stiffness. Therefore, a simple numbering system has been developed, based on engineering theory, that gives the relative stiffness of wires of different cross sections if the material composition of the wire is the same. The cross-sectional stiffness number (Cs) uses 0.1-mm (0.004-inch) round wire as a base of 1. A 0.006-inch wire has a Cs of 5.0, which means that for the same activation, 5 times as much force is delivered.
  • 81. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) Tables 11-2 and 11-3 list, under the Cs column, stiffness numbers based on nominal cross sections. Manufacturing variation or mislabeling of wires obviously can change the actual Cs significantly. Two Cs numbers are given for rectangular wires—one for the first-order direction and one for the second-order direction.
  • 82. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section)
  • 83. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) Any two sections of wire can be compared for stiffness simply by dividing the Cs number of one into the other.
  • 84. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) The overall stiffness of an appliance (S) is determined by two factors: 1. Wire itself (Ws) 2. Design of the appliance (As) S = Ws × As where S is the appliance load-deflection rate (Stiffness); Ws, the wire stiffness; and As, the design stiffness factor. In general terms Appliance stiffness = wire stiffness × design stiffness Wire stiffness =material stiffness × cross-sectional stiffness Wire stiffness is determined by a cross-sectional property (e.g., moment of inertia) and a materials property (the E).
  • 85. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) A full range of forces can be obtained by varying the material of the wire while keeping the cross section the same.
  • 86. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section)
  • 87. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section)
  • 88. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) 1. Variable cross-section Principle: The amount of play between the attachments and the wire can be varied, depending on the stiffness required. With small, low-stiffness wires, excessive play may lead to lack of control over tooth movement.
  • 89. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) 2. Variable-Modulus Principle: Clinician determines the amount of play required before selecting the wire. In some instances more play is needed to allow the brackets freedom of movement along the arch wire. In other situations minimal play is allowed to ensure good orientation and effective third-order movement. After the desired amount of play has been established, the correct wire stiffness can be produced by using a material with a proper Ms. In this way the play between the wire and the attachment is not dictated by the stiffness required but rather is under the full control of the operator.
  • 90. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Selection of the Proper Wire (Alloy and Cross Section) 2. Variable-Modulus Principle: The variable-modulus principle allows the orthodontist to use oriented rectangular wires or square wires in light force and heavy force applications and stabilization. A rectangular wire orients in the bracket and thus offers greater control in delivering the desired force system; it is easier to bend because the orientation of the wire can be checked carefully. More important, when placed in the brackets, the wire does not turn or twist, allowing the forces to be dissipated in improper directions.
  • 92. Reference: • Orthodontics, the art and science, 4th Edition, S.I.Bhalaji • Up until the 193Os, the only orthodontic wires available were made of gold. • Austenitic stainless steel, with its greater strength, higher modulus of elasticity, good resistance to corrosion, and moderate costs, was introduced as an orthodontic wire in 1929, and shortly afterward gained popularity over gold. History
  • 93. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Stainless Steel (SS) Wires Types of orthodontic wires • Most commonly used: austenitic 18-8 stainless steel (contains chromium and nickel content of approximately 18% and 8%, respectively) Characteristics: • High resistance to Corrosion (by the formation of a passivated oxide layer, which blocks the further oxygen diffusion to the underlying mass) • Produce higher forces applied during shorter time periods (since they have lower spring back ability). • Store less energy compared to those of beta-titanium or nickel- titanium. • Can be soldered with different biomechanical attachments. • The corrosion resistance of stainless steel is good in general (but releases nickel and chromium in fewer amounts and may induce hypersensitivity reactions) Kolokitha et al., concluded that orthodontic treatment is not related to an increased likelihood of hypersensitivity reactions to nickel unless there is a history of skin piercing.
  • 94. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Stainless Steel (SS) Wires Types of orthodontic wires • Stainless steel wires have a lower bracket-wire friction than other types of wires (this friction can be further reduced by using nanotechnology applications) • Australian wires are a kind of stainless steel wires available in different grades with gradually increasing stored energy values (resiliency).
  • 95. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Stainless Steel (SS) Wires Types of orthodontic wires • Properties of Stainless steel wires can be controlled by varying the amount of cold working and annealing during manufacture. • Steel is softened by annealing and hardened by cold working. • Fully annealed stainless steel wires are soft and highly formable. • Steel ligatures are made from such “dead soft” wire.
  • 96. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Stainless Steel (SS) Wires Types of orthodontic wires • “Super Grades” Steel wires: possess impressive yield strength, are brittle and break if bend sharply. • “Regular Grades” Steel wires: can be bent to almost any desired shape without breaking.
  • 97. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Cobalt-chromiumWires Types of orthodontic wires • Cobalt-chromium-nickel alloy known as elgiloy. • These alloys were originally developed for use as watch spring by ELGIU national company. • Available in different tempers depending on amount of cold work and are usually color- coded. Color codes High spring tempers Red Semispring temper Green Soft or ductile tempers Yellow High formability combined with increased elasticity and yield strength following heat treatment by 10% and 20- 30%, respectively, have made Blue Elgiloy, a cobalt chromium wire type, popular in clinical practice.
  • 98. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Cobalt-chromiumWires Types of orthodontic wires Characteristics: • Easy to bend. • Can be heat hardened at 482° C for about 7 minutes after manipulation to increase hardness (strength) approximately equal to that of stainless steel. • Non-heat treated cobalt-chromium wires have a smaller spring- back than stainless steel wires • Excellent resistance to tarnish and corrosion. • Inexpensive and can be soldered (fluoride fluxes are used) and welded.
  • 99. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Cobalt-chromiumWires Types of orthodontic wires COMPARISON WITH STAINLESS STEEL: • Elgiloy, the cobalt–chromium alloy, has the advantage that it can be supplied in a softer and therefore more formable state, and the wires can be hardened by heat treatment after being shaped. The heat treatment increases strength significantly. • After heat treatment, the softest Elgiloy becomes equivalent to regular stainless steel, while harder initial grades are equivalent to the “super” steels. • This material, however, had almost disappeared by the end of the twentieth century because of its additional cost relative to stainless steel and the extra step of heat treatment to obtain optimal properties.
  • 100. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Types of orthodontic wires Shape Memory Alloys: 1. Nickel titanium (nitinol) - William F. Buehler 2. Superelastic NiTi wires 3. TMA 4. Titanium niobium
  • 101. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Beta TitaniumWires Types of orthodontic wires • Introduced in 1979 • Also known as titanium-molybdenium alloy (TMA) or Titanium Niobium. Characteristics: • Modulus of elasticity of these wires is lower than half of stainless steel wires and almost twice that of Nitinol. • Demonstrate good formability, (but should not be strongly bent for there is a risk of breaking). • Electrical welding of biomechanical attachments is possible, (but overheating should not be done as it makes the wire more brittle). • According to a recent study, beta-titanium wires are better in terms of joinability than stainless steel wires (since they demonstrate higher resilience and better surface and structural characteristics, which indicates only a minor change in wire properties after welding).
  • 102. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Beta TitaniumWires Types of orthodontic wires Characteristics: • Resistance to corrosion is similar to that of cobalt chromium and stainless steel wires. • Good biocompatible material (due to the absence of nickel). • Resistance to corrosion is due to the formation of a surface passivation oxide layer (but exposure to fluoride agents leads to the degradation, subsequent corrosion, and qualitative alteration of the wire’s surface). • Highly expensive • More bracket-wire friction than any other alloy Alpha-beta titanium alloy is also called as TiMolium, it has stiffness and other characteristics (such as elasticity and yield strength) are between the values set for stainless steel and beta-titanium wires
  • 103. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Beta TitaniumWires Types of orthodontic wires Characteristics: • TMA has a modulus of elasticity between that of steel and nitinol (approximately 0.4 times that of stainless steel). • TMA can be deflected up to 2 times as much as steel without permanent deformation. • Unlike Nitinol, TMA is not significantly altered by the placement of bends and twists and has good ductility, equivalent to or slightly better than that of stainless steel, and can be welded without significant reduction in yield strength.
  • 104. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Nickel Titanium Wires Types of orthodontic wires • Exceptional ability to apply light force over a large range of activations. This phase transition allows certain NiTi alloys to exhibit two remarkable properties found in no other dental materials—shape memory and superelasticity. Martensitic form Lower temperatures Higher stress Austenitic form Higher temperatures Lower stress The uniqueness of NiTi is that the transition between the two structures is fully reversible and occurs at a remarkably low temperature.
  • 105. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Nickel Titanium Wires Types of orthodontic wires  The original Nitinol wires marketed under that name in the late 1970s by Unitek were M- NiTi wires, with no application of phase transition effects.  M-NiTi remains useful, primarily in the later stages of treatment when flexible but larger and somewhat stiffer wires are needed. M-NiTi: NiTi wires stabilized in the martensitic form are referred to as M-NiTi. A-NiTi: NiTi wires displaying martensite–austenite transitions are referred to as A-NiTi.  In the late 1980s, new nickel–titanium wires with an austenitic grain structure (A-NiTi) appeared.  These wires exhibit superelasticity and/or shape memory in various degrees.  The properties of A-NiTi have quickly made it the preferred material for orthodontic applications in which a long range of activation with relatively constant force is needed (i.e., for initial archwires and coil springs).
  • 106. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Nickel Titanium Wires Types of orthodontic wires Shape memory: refers to the ability of the material to “remember” its original shape after being plastically deformed while in the martensitic form. Superelasticity: refers to the very large reversible strains that certain NiTi wires can withstand due to the martensite-austenite phase transition. • Materials displaying superelasticity are austenitic alloys that undergo a transition to martensite in response to stress—a mechanical analogue to the thermally induced shape memory effect. • Superelastic materials must exhibit a reversible phase change at a close transition temperature, which must be lower than room temperature for the austenite phase to exist clinically. Shape memory is a thermal reaction and superelasticity is a mechanical one, they are inherently linked.
  • 107. Reference: • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver. Nickel Titanium Wires Types of orthodontic wires Thermoelasticity: • In a typical application, a certain shape is set while the alloy is maintained at an elevated temperature, above the martensite–austenite transition temperature. • When the alloy is cooled below the transition temperature, it can be plastically deformed, but the original shape is restored when it is heated enough to regain an austenitic structure. • This temperature-induced change in crystal structure (called thermoelasticity) was important to the original nitinol use in the space program but proved difficult to exploit in orthodontic applications.
  • 108. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Nickel Titanium Wires Types of orthodontic wires • A wrought Ni-Ti alloy known as Nitinol (Nickel-Titanium naval ordinance laboratory) was introduced in 1972. Characteristics: • High resiliency. • Higher energy storage capacity • Shape memory or thermal memory. • Pseudoelastic or superelasticity. • Limited formability. • Cannot be welded or fused. The friction develops at bracket-wire interface is more with Nitinol wires followed by beta-titanium, stainless steel and chromium-cobalt wires
  • 109. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Nickel Titanium Wires Types of orthodontic wires Two major phases One intermediate phase Austenitic Phase Martensitic phase • At higher temperature • Body centered cubic structure (BCC) • At lower temperature • hexagonal close packed structure (HCP) Delays the transition from austenite to martensite upon cooling until lower temperatures are achieved.
  • 110. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Nickel Titanium Wires Types of orthodontic wires Shape memory achieved by first establishing a shape at temperatures near 482° C. If the appliance wire is then cooled and formed into a second shape and heated through a lower transition temperature range (TTR), the wire will return to its original shape. The cobalt content is used to control the transition temperature range, which can be near mouth temperature.
  • 111. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Nickel Titanium Wires Types of orthodontic wires Phase transformation (from BCC austenitic to HCP martensitic) can be seen by decreasing the temperature from an elevated temperature and can also be induced by the application of stress and a volumetric change is associated during this transition. This transformation results in two unique features such as shape memory and pseudoelasticity or superelasticity.
  • 112. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Nickel Titanium Wires Types of orthodontic wires Pseudoelasticity or Superelasticity Inducing the austenitic to martensitic transformation by stress can produce superelasticity, a phenomena that is employed with Ni – Ti wires.
  • 113. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Nickel Titanium Wires Types of orthodontic wires The shape memory principle is not used clinically. Instead, nitinol is used for its low force and high springback. The most dramatic characteristic of nitinol, however, is its resistance to permanent deformation. NiTi wires can be activated over twice the distance of stainless steel, with minimal permanent deformation. Nitinol is more brittle than stainless steel and cannot be joined by soldering or welding.
  • 114. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Superelastic Ni-Ti Wires Types of orthodontic wires  Unlike nitinol, these alloys have a much lower transition temperature—either slightly below or slightly higher than mouth temperature.  Generally speaking, the austenitic form of these alloys has a slightly higher springback than nitinol and may be less brittle.  The superelastic NiTi wires are available in different degrees of stiffness.
  • 115. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Superelastic Ni-Ti Wires Types of orthodontic wires  Although the final transition temperature of some superelastic NiTi wires is below mouth temperature, others are not activated fully until they reach 37°C or higher.  These wires have both superelastic and shape memory properties.  Generally, the heat treatment process performed during manufacture to raise the transition temperature allows for wires that deliver lower forces at mouth temperature;  hence the orthodontist may be able to achieve full bracket engagement with larger wires earlier in treatment.
  • 116. Reference: • Orthodontics current principles and techniques; Grabber, 5th edition Titanium Niobium Wires Types of orthodontic wires Characteristics: • Low springback (equivalent to stainless steel) • Much less stiff than TMA • Useful when a highly formable wire with low forces in small activations is required.
  • 117. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Chinese Ni-Ti Wires Types of orthodontic wires The Chinese NiTi wires were recommended by Burstone et al in 1985. They exhibited 4.4 times the spring-back of stainless steel wires and 1.6 times the spring-back of the original Nitinol wires if a constant force in the middle of its deactivation range.
  • 118. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Japanese Ni-Ti Wires Types of orthodontic wires The Japanese NiTi wires was introduced by Miura et al. in 1986 Their properties were almost similar to Chinese NiTi wires.
  • 119. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Multistranded Wires Types of orthodontic wires • Made of a varying number of stainless steel wire strands coaxially placed or coiled around each other in different configurations. Characteristics: • Deliver low forces • Low stiffness • Low resilience • Inexpensive than titanium alloys • Higher friction at bracket-wire interface compared to NiTi wires and single-stranded stainless steel wires
  • 120. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Esthetic Wires Fiber-reinforced composite arch wires Types of orthodontic wires Characteristics: • Highly esthetic • Biocompatible • Hydrolytic stability • Less water sorption • Stiffness is same as metallic wires • Post processing formability • Sliding mechanics are good • Wearing of these arch wires at the interface chances of leaching of glass fibers within the oral cavity.
  • 121. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Esthetic Wires Teflon coated stainless steel arch wires Types of orthodontic wires • Teflon is coated on stainless steel wire by an atomic process that forms a layer of about 20-25ìm thickness on the wire that imparts to the wire a hue which is similar to that of natural teeth. • Teflon coating protects the underlying wire from the corrosion process. • However, corrosion of the underlying wire is likely to take place if it is used for longer period in the oral cavity since this coating is subject to flaws that may occur during clinical use.
  • 122. Reference: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Types of orthodontic wires Other Esthetic wires:  Optiflex  Bioforce wires  Marsenol  Lee White wire
  • 123. REFERENCES: Articles: • Ravichandra Sekhar Kotha et. Al, An Overview of Orthodontic Wires, Trends Biomater. Artif. Organs, 28(1), 32-36 (2014) Books: • Orthodontics current principles and techniques; Grabber, 5th edition • Contemporary Orthodontics, 5th Edition, Proffit & Fields & Sarver.

Editor's Notes

  1. In this presentation we will learn…
  2. Range is defined as the distance that the wire will bend elastically before permanent deformation occurs.
  3. Yield stress, Yeild strength, Yeild point = ????
  4. Precisely determining this proportional point can be difficult, so a more practical indicator is the yield strength—the intersection of the stress–strain curve with a parallel line offset at 0.1%strain. Typically, the true elastic limit lies between these two points, but both serve as good estimates of how much force or deflection a wire can withstand clinically before permanent deformation occurs.
  5. On observational level, forces and deflection can be noted and measured. In other words, a certain amount of force in grams can be applied, and the wire will deflect by a certain number of millimeters. On Stress-strain level the orthodontist is dealing with pounds per square inch and deflection per unit length. These values cannot be measured directly, but they can be calculated from measurements made on the observational level. Atomic and molecular level: An understanding of events at the atomic and molecular level enhances the ability to predict responses and design new structures.
  6. All three of the important characteristics of an orthodontic appliance—the M/F ratio, the load-deflection rate, and the maximal elastic load or moment—are found within the elastic range of an orthodontic wire and therefore may be called spring characteristics.
  7. Moment: Quantitatively, it is the product of the force times the perpendicular distance from the point of force application to the center of resistance and thus is measured in units of gram-millimeter (or equivalent). If the line of action of an applied force does not pass through the center of resistance, a moment is necessarily created. Not only will the force tend to translate the object, moving it to a different position, it also will tend to rotate the object around the center of resistance. This, of course, is precisely the situation when a force is applied to the crown of a tooth. Not only is the tooth displaced in the direction of the force, it also rotates around the center of resistance—thus the tooth tips as it moves. --------Notes------- Moment will 1.translate & 2. rotate the tooth around the COR.
  8. Couple: A couple will produce pure rotation, spinning the object around its center of resistance, while the combination of a force and a couple can change the way an object rotates while it is being moved.
  9. Center of resistance: If a single force is applied to the crown of a tooth, the tooth will not only translate but also rotate around CR (i.e., the center of rotation and center of resistance are identical) because a moment is created by applying a force at a distance from CR. Center of rotation: When two forces are applied simultaneously to an object, the center of rotation can be controlled and made to have any desired location. The application of a force and a couple to the crown of a tooth, in fact, is the mechanism by which bodily movement of a tooth, or even greater movement of the root than the crown, can be produced. -----------------------------------------------------
  10. The load-deflection rate is an indicator of the force required per unit deflection. The load-deflection rate gives the force produced per unit activation.
  11. The anchorage potential of a group of teeth can be enhanced if the teeth displace as a unit. If individual teeth in the reactive unit tend to rotate around separate centers of rotation, higher stress distributions are produced in the PDL and the teeth can be more easily displaced. Another factor to consider is that the equal and opposite forces produced by the active members usually are distributed to localized areas, with just one or a few teeth involved. Localized tooth changes in these areas can be minimized if the reactive members of the appliance are sufficiently rigid.
  12. Active and reactive members must be designed so they do not deform if activations are made that allow optimal force levels to be reached. In designing an appliance, a good idea is to go beyond required force needs and create a safety factor. Thus permanent deformation or breakage will not occur from accidental overloading, which can be caused by abnormal activation of an appliance or by abnormal forces during mastication.
  13. In range of Hooks Law..Load divided by deflection is a constant through this range. (Load-deflection rate)
  14. A reactive member made of stainless steel is 1.8 times as resistant to deflection as one made of gold.
  15. Typically, the true elastic limit lies between these two points, but both serve as good estimates of how much force or deflection a wire can withstand clinically before permanent deformation occurs. Proportional limit: Hook’s Law Yield Strength: at which 0.1%permanent deformation has occurred. Ultimate tensile strength - The maximum load the wire can sustain, is reached after some permanent deformation and is greater than the yield strength. Since this ultimate strength determines the maximum force the wire can deliver if used as a spring, it also is important clinically, especially since yield strength and ultimate strength differ much more for the newer titanium alloys than for steel wires. Strength is measured in units of stress—the SI (standard international) unit is the pascal (Pa), but English units such as gm/cm2 are still frequently encountered. Data in megaPa (MPa) now appear frequently in orthodontic journals, and MPa will be used in the rest of this text. The conversion factor: 100 gm/cm2 = ~10 MPa (actually 9.81 MPa, but that small difference is not significant in clinical evaluation of orthodontic materials).
  16. Orthodontic wires often are deformed beyond their elastic limit, so springback properties are important in determining clinical performance.
  17. The range is the distance along the X-axis to the point at which permanent deformation occurs (usually taken as the yield point, at which 0.1%permanent deformation has occurred).
  18. The principle with any supported beam, however, is the same as with a cantilever beam: as the beam size increases, strength increases as a cubic function, while springiness decreases as a fourth power function and range decreases proportionately, not exponentially. More generally, when beams of any type made from two sizes of wire are compared, strength changes as a cubic function of the ratio of the two cross-sections; springiness changes as the fourth power of the ratios; range changes as a direct proportion (but the precise ratios are different from those for cantilever beams). When a round wire is used as a fingerspring, doubling the diameter of the wire increases its strength eight times (i.e., the larger wire can resist eight times as much force before permanently deforming or can deliver eight times as much force).
  19. More generally, strength varies inversely with length, whereas springiness varies as a cubic function of the length ratios and range as a second power function.
  20. More generally, strength varies inversely with length, whereas springiness varies as a cubic function of the length ratios and range as a second power function.
  21. Elastic Limit (EL) The EL is the greatest stress that can be applied to the alloy without permanent deformation. Maximal elastic load: The EL is analogous to the maximal elastic load (Pmax) and therefore is the mechanical property that determines the ability of a member to withstand permanent deformation. Load-deflection rate: force produced per unit activation OR force required per unit deflection. Modulus of elasticity (E) this mechanical property determines the load-deflection rate of a spring. Load-deflection varies directly and linearly with Modulus of elasticity (E).
  22. The alloy should be reasonably resistant to corrosion caused by the fluids of the mouth. The wire should be sufficiently ductile so that it does not fracture under accidental loading in the mouth or during fabrication of an appliance. The wire should be able to be fabricated in a soft state and later heat treated to hard temper. The alloy should allow easy soldering of attachments.
  23. The most obvious means of reducing the load deflection rate of an active member may seem to be to reduce the size of the wire. However, the fallacy in reducing the size of the cross section is that the maximal elastic load also is reduced at an alarmingly high rate (as d3). When designing active members, a good policy is to use as small a cross section as is consistent with a safety factor so that undue permanent deformation does not occur.
  24. Normal circumstances require a large enough wire cross section to give sufficient rigidity so that a sufficiently high load-deflection rate is ensured.
  25. For unidirectional bending, flat wire is the cross section of choice; more energy can be absorbed into a spring made of a flat wire than with any other cross section. This principle has been used for years in watch springs and other commercial designs. Hence flat (ribbon) wire can deliver lower load deflection rates without permanent deformation more successfully than any other type of cross section.
  26. For instance, if continuous ribbon wires are used (long-axis oriented occlusogingivally), positive leveling can be achieved occlusogingivally over a limited range, and buccolingual and labiolingual tooth alignment can be effected over a long range of action. A configuration of this type is useful when most of the problems are in the horizontal rather than the vertical plane.
  27. The cantilever has been chosen to demonstrate the effect of length because the cantilever principle is widely used in orthodontic mechanisms. A finger spring may be visualized for the following discussion.
  28. In this type of loading the load-deflection rate varies inversely as the third power of the length; in other words, the longer the cantilever, the lower is the load-deflection rate. The maximal elastic load varies inversely as the length of the cantilever. Again, the longer the cantilever, the lower is the maximal elastic load.
  29. Adding length within the practical confines of the oral cavity is an excellent way to improve spring properties.
  30. With a couple applied at the free end, the moment-deflection rate varies inversely as the second power of the length. Interestingly, the maximal elastic moment is not affected at all by changes in length. The length may be doubled or tripled, but the maximal elastic moment remains the same. This is a most desirable type of loading because additional length can reduce the moment-deflection rate, but the maximal elastic moment is not reduced. However, the principle can be applied only if moments alone are required for a given tooth movement. Increasing the length of a wire with vertical loops is one of the more effective means of reducing load deflection rates for flexible members and at the same time only minimally altering their maximal elastic loads. However, limitations exist on how much the length can be increased. The distance between brackets in a continuous arch is predetermined by tooth and bracket width.
  31. In Figure 11-29 a cantilever is shown with the vertical force of 100 g at the free end. Imaginary vertical sections can be cut along the length of the wire, and at each of these sections a bending can be calculated. The bending moment is found by multiplying the load at the end of the cantilever by the perpendicular distance to the section in question; therefore the bending moment at the point of force application at the free end of the wire is zero. Approximately 1 mm closer to the point of support, it is 100 g-mm. At 2 mm closer, it is 200 g-mm. Finally, at the point of support, the bending moment is 1000 g-mm.
  32. This is important from a design standpoint because it provides a method of lowering the load-deflection rate without subsequently reducing the maximal elastic load.
  33. Although additional wire is helpful in the design of flexible members, it should not be used in reactive or rigid members. Loops and other types of configurations diminish the rigidity of the wire and thus may be responsible for some loss of control over the anchor units.
  34. 1. The primary reason for selecting a particular wire size is the stiffness of the wire (i.e., its load-deflection rate). In a replacement technique, for example, the orthodontist might begin with a 0.014-inch wire that, deflected over 2 mm, gives the desired force. After the tooth had moved 1 mm, the wire can be replaced with a 0.018-inch wire, which gives almost the same force with 1 mm of activation. 2. A wire also may be selected because it is believed that the smaller the wire, the greater the maximum elastic deflection possible; in other words, the smaller the wire, the more it can be deflected without permanent deformation. This is true, but maximal elastic deflection varies inversely with the diameter of the wire. A 0.016-inch wire has only 1.15 times as much maximal elastic deflection as a 0.018-inch wire; therefore the difference is negligible from a clinical standpoint. If the difference is 2 : 1 (as in 0.010-inch versus 0.020-inch wire), this factor becomes clinically significant.
  35. In the past, the cross section of wires has been varied to produce different degrees of stiffness. As the appliance design is changed by increasing wire between the brackets or by adding loops, the stiffness can be reduced as the design stiffness factor changes; however, the orthodontist is not concerned only with ways in which wire stiffness can be altered. Wire stiffness is determined by the cross section and the material of the wires: Ws =Ms ×Cs where Ws is the wire stiffness number, Ms, the material stiffness number; and Cs, the cross-sectional stiffness number. In the past, because most orthodontists used only stainless steel with almost identical Es, only the size of the wire was varied and no concern was expended on the material property, which determines wire stiffness. With the availability of new materials, one can use the same cross section of wire but with different materials with differing degrees of stiffness to produce the wide range of forces and load-deflection rates required for comprehensive orthodontics.
  36. These wires contain more amount of carbon content that is up to 10 times higher than that in a standard stainless steel orthodontic wire (up to 0.20%) and this results in increased surface roughness, hardness, porosity, and susceptibility for breakage during clinical bending, particularly for higher grades. So their use is restricted to biomechanical attachments. Recently, super stainless steels have been developed with a lower nickel content, higher corrosion resistance, and improved mechanical properties.
  37. These wires contain more amount of carbon content that is up to 10 times higher than that in a standard stainless steel orthodontic wire (up to 0.20%) and this results in increased surface roughness, hardness, porosity, and susceptibility for breakage during clinical bending, particularly for higher grades. So their use is restricted to biomechanical attachments. Recently, super stainless steels have been developed with a lower nickel content, higher corrosion resistance, and improved mechanical properties.
  38. These wires contain more amount of carbon content that is up to 10 times higher than that in a standard stainless steel orthodontic wire (up to 0.20%) and this results in increased surface roughness, hardness, porosity, and susceptibility for breakage during clinical bending, particularly for higher grades. So their use is restricted to biomechanical attachments. Recently, super stainless steels have been developed with a lower nickel content, higher corrosion resistance, and improved mechanical properties.
  39. In the early 1980s, after Nitinol but before A-NiTi, a quite different titanium alloy, beta-titanium (beta-Ti), was introduced into orthodontics. This beta-Ti material was developed primarily for orthodontic use. It offers a highly desirable combination of strength and springiness (i.e., excellent resilience), as well as reasonably good formability. This makes it an excellent choice for auxiliary springs and for intermediate and finishing archwires, especially rectangular wires for the late stages of edgewise treatment.
  40. A-NiTi: Shape memory alloys only have exceptional range clinically if stress-induced transformation also occurs. Otherwise, in order to keep the force light, the temperature would have to be slowly increased as the teeth come closer to alignment—which obviously does not occur clinically. Due to the close interaction of these properties, wires displaying martensite–austenite transitions are subsequently referred to as A-NiTi. M-NiTi: All other NiTi wires are stabilized in the martensitic form and are subsequently referred to as M-NiTi.
  41. Superelasticity, In engineering applications, it also is frequently described as pseudoelasticity, due to the nonlinear stress–strain curve, which is not typical of elastic behavior. Superelasticity possible because the transition temperature is very close to room temperature. Most archwire materials can be reversibly deformed only by stretching interatomic bonds (which creates the linear region of the stress–strain curve superelastic materials can undergo a reversible change in internal structure after a certain amount of deformation. This stress-induced martensitic transformation manifests itself in the almost flat section of the load-deflection curve. Superelastic materials can undergo a reversible change in internal structure after a certain amount of deformation. This stress-induced martensitic transformation manifests itself in the almost flat section of the load-deflection curve.
  42. Superelasticity, In engineering applications, it also is frequently described as pseudoelasticity, due to the nonlinear stress–strain curve, which is not typical of elastic behavior. Superelasticity possible because the transition temperature is very close to room temperature. Most archwire materials can be reversibly deformed only by stretching interatomic bonds (which creates the linear region of the stress–strain curve superelastic materials can undergo a reversible change in internal structure after a certain amount of deformation. This stress-induced martensitic transformation manifests itself in the almost flat section of the load-deflection curve. Superelastic materials can undergo a reversible change in internal structure after a certain amount of deformation. This stress-induced martensitic transformation manifests itself in the almost flat section of the load-deflection curve.
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