orthodontics wires 1
TRANSCRIPT
1
Orthodontic wires-I
Orthodontic wires-I
Dr.Meenakshi Vishwanath
2
Contents Introduction Evolution of materials Basic properties of materials Mechanical & Elastic properties Physical properties Requirements of an ideal arch wire Properties of wires Orthodontic arch wire materials
3
Introduction “All you can do is push, pull or turn a tooth. I have given you an appliance and now for God’s sake use
it” Edward.H.Angle
The main components of an orthodontic appliance -brackets and wires.
Active and reactive elements (Burstone)
Wires Brackets Bonding
4
Introduction
Orthodontics involves correction of the position of teeth –requiring moving teeth.
Forces and Moments
Optimum orthodontic tooth movement- light continuous force.
5
Introduction The challenge – Appliance which produces forces that are
neither too great nor variable.
Different materials and type of wires introduced to provide forces.
6
Evolution of Materials 1. Material Scarcity, Abundance of Ideas (1750-1930) Before Angle’s search; Noble metals and their alloys.
- Gold (at least 75%), platinum, iridium and silver alloys
Good corrosion resistance Acceptable esthetics
Lacked flexibility and tensile strength Inappropriate for complex machining and joining.
7
Evolution of Materials Angle listed few materials appropriate for work:
Strips of wire of precious metals. Wood Rubber Vulcanite Piano wire Silk thread
8
Evolution of Materials Angle (1887) German silver (a type of brass)
“according to the use for which it was intended”-varying the proportion of Cu, Ni & Zn and various degrees of cold work.
Neusilber brass (Cu 65%, Ni 14%, Zn 21%) jack screws (rigid) expansion arches (elastic) Bands (malleable)
Opposition by Farrar – discolored
9
Evolution of Materials Stainless steel (entered dentistry -1919). Dumas ,Guillet and Portevin-(France), qualities
reported in Germany –Monnartz (1900-1910). Discovered by chance before W W I. 1919 – Dr. F Hauptmeyer –Wipla (wie platin). Simon, Schwarz, Korkhous, De Coster-
orthodontic material. Angle used steel as ligature wire (1930).
10
Evolution of Materials Opposition Emil Herbst
-Gold wire was stronger than stainless steel (1934).
“The Edgewater" tradition- -1950-2 papers presented back to back-
competition between SS & gold. - B/w Dr.Brusse (The management of stainless
steel) and Drs.Crozat & Gore (Precious metal removable appliances).
Begg (1940s) with Wilcock-ultimately resilient arch wires-Australian SS.
11
Evolution of Materials2. Abundance of materials, Refinement of
Procedures (1930 – 1975). Kusy-after 1960s-proliferation abounds.
Improvement in metallurgy and organic chemistry – mass production(1960).
Farrar’s dream(1878)-mass production of orthodontic devices.
12
Evolution of Materials Cobalt chrome (1950s)-Elgin watch company
developed a complex alloy-Cobalt(40%),Chromium(20%),iron(16%)&nickel(15%).
Rocky Mountain Orthodontics- ElgiloyTM
1958-1961 various tempers
Red – hard & resilientgreen – semi-resilientYellow – slightly less formable but
ductileBlue – soft & formable
13
Evolution of Materials
Variable cross-section orthodontics-
Burstone To produce changes in load-deflection rate- wires
of various cross sections were used.
Load deflection rate varies with 4th power of the wire diameter.
14
Evolution of Materials
1962 - Buehler discovers nickel-titanium dubbed NITINOL (Nickel Titanium Naval Ordnance Laboratory)
1970-Dr.George Andreason (Unitek) introduced NiTi to orthodontics.
50:50 composition –excellent springback, no superelasticity or shape memory (M-NiTi).
Late 1980s –NiTi with active austenitic grain structure.
15
Evolution of Materials Exhibited Superelasticity (pseudoelasticity in
engineering). New NiTi by Dr.Tien Hua Cheng and associates
at the General Research Institute for non Ferrous Metals, in Beijing, China.
Burstone et al–Chinese NiTi (1985).
In 1978 Furukawa electric co.ltd of Japan produced a new type of alloy
1. High spring back.
2. Shape memory.
3. Super elasticity.
Miura et al – Japanese NiTi (1986)
16
Evolution of MaterialsVariable – modulus orthodontics-Burstone
(1981) Wire size was kept constant and material of the wire
is selected on the basis of clinical requirements.
Fewer wire changes.
Different materials-maintaining same cross-section.
17
Evolution of Materials Cu NiTi – (thermoelasticity) - Rohit Sachdeva.
•Quaternary metal – Nickel, Titanium, Copper, Chromium.•Copper enhances thermal reactive properties and creates a consistent unloading force.
Variable transformation temperature orthodontics
18
Evolution of Materials3. The beginning of Selectivity (1975 to the
present) Orthodontic manufacturers CAD/CAM – larger production runs Composites and Ceramics Iatrogenic damage
Nickel and en-masse detachments
New products- control of government agencies, private organizations
19
Evolution of Materialsβ titanium –Burstone and Goldberg-1980
β phase –stabilized at room temperature. Early 1980s Composition
Ti – 80% Molybdenum – 11.5% Zirconium – 6% Tin – 4.5%
Burstone’s objective deactivation characteristics 1/3rd of SS or twice of conventional NiTi
TMA – Titanium Molybdenum alloy - ORMCO
20
Evolution of Materials Titanium-Niobium- M. Dalstra et al.
Nickel free Titanium alloy.
Finishing wire.
Ti-74%,Nb-13%,Zr-13%.
TiMolium wires (TP Lab)-Deva Devanathan (late 90s)
Ti - 82% ,Mo - 15% , Nb-3%
21
Evolution of Materials β III- Ravindra Nanda (2000-2001)
• Bendable,inc. force-low deflection
• Ni free
• Versatility of steel with memory of NiTi.
22
Evolution of MaterialsFiber reinforced polymeric composites:
Next generation of esthetic archwires
Many orthodontic materials adapted-Aerospace industry
Pultrusion – round + rectangular
ADV – tooth colored enhanced esthetics - reduced friction
DISADV – difficult to change its shape once manufactured
23
Basic Properties of Materials
To gain understanding of orthodontic wires – basic knowledge of their atomic or
molecular structure and their behavior during handling and use in the oral
environment .
24
Basic Properties of Materials
Atom - smallest piece of an element that keeps its chemical properties.
Element - substance that cannot be broken down by chemical reactions.
25
Basic Properties of Materials
Electrons – orbit around nucleus.
Floating in shells of diff energy levels
Electrons form the basis of bonds
26
Basic Properties of Materials
Pure substances are rare-eg. Iron always contains carbon, gold though occurs as a pure metal can be used only as an alloy.
An ore contains the compound of the metal and an unwanted earthly material.
Compound - substance that can be broken into elements by chemical reactions.
Molecule - smallest piece of a compound that keeps its chemical properties (made of two or more atoms).
27
Basic Properties of Materials Cohesive forces-atoms held together.
Interatomic bonds
Primary Secondary Ionic Hydrogen Covalent Van der Waals Metallic
forces
28
Basic Properties of Materials Ionic-mutual attraction between positive and
negative ions-gypsum, phosphate based cements.
Covalent-2 valence electrons are shared by adjacent atoms-dental resins.
29
Basic Properties of Materials Metallic –increased spatial extension of valence-
electron wave functions. The energy levels are very closely spaced and
the electrons tend to belong to the entire assembly rather than a single atom.
Array of positive ions in a “sea of electrons”
30
Basic Properties of Materials Electrons free to move
Electrical and thermal conductivity
Ductility and malleability -electrons adjust to deformation
31
Basic Properties of Materials
IONIC BOND METALLIC BOND
Ionic bond Metallic bond
32
Basic Properties of Materials Materials broadly subdivided into 2 categories - Atomic arrangement
Crystalline structure Non-crystalline structureRegularly spaced Possess short range
config-space lattice. atomic order. Anisotropic –diff in Isotropic-prop of materialmechanical prop due remains same in all directional arrangement directions. of atoms. Amorphous
33
Characteristic properties of metals
An opaque lustrous chemical substance that is a good conductor of heat and electricity & when polished is a good reflector of light – Handbook of metals.
Metals are-• Hard• Lustrous• Dense (lattice structure)• Good conductors of heat & electricity• Opaque (free e- absorb electromagnetic energy of
light)• Ductile & Malleable
34
Basic Properties of Materials Crystals and Lattices
1665-Robert Hooke simulated crystal shapes –musket ball.
250 years later-exact model of a crystal with each ball=atom.
Atoms combine-minimal internal energy.
Space lattice- Any arrangement of atoms in space in which every atom is situated similarly to every other atom. May be the result of primary or secondary bonds.
35
Basic Properties of Materials
Crystal combination of unit cells, in which each shell shares faces, edges or corners with the neighboring cells
There are 8 crystal systems: Cubic system –Important as many metals belong
to it.
36
Basic Properties of MaterialsThere are 14 possible lattice forms.( Bravais
lattices) The unit cells of 3 kinds of space lattices of
practical importance –1.Face-centered cubic: Fe above 910°C & Ni.
37
Basic Properties of Materials2.Body centered cubic:
Fe-below 910°C &above 1400°C. Cr &Ti above 880°C.
38
Basic Properties of Materials3.Hexagonal close packed:
Co & Ti below 880°C
39
Basic Properties of Materials Perfect crystals - rare - atoms occupy well-
defined positions. Cation-anion-cation-anion- Distortion strongly opposed -similarly charged
atoms come together. Single crystals- strong Used as reinforcements –whiskers (single
crystals- 10 times longer, than wide)
40
Basic Properties of Materials Crystal growth-atoms attach themselves in
certain directions. Perfect crystals-atoms-correct direction. In common metals the crystals penetrate each
other such that the crystal shapes get deformed. Microscopic analysis of alloys-grains (microns to
centimeters).
41
Basic Properties of Materials
42
Basic Properties of Materials Grain boundaries-area-crystals meet. Atoms-irregular
Decrease mechanical strength Increase corrosion
imperfections beneficial-interfere with movement along slip planes
Dislocations cannot cross boundary- deformation requires greater stress.
43
Basic Properties of Materials Usually crystals have imperfections- Lattice
defects.1.Point defects: a. Impurities •Interstitials – Smaller atoms that penetrate the lattice
Eg – Carbon, Hydrogen, Oxygen, Boron.
•Substitutial Element – Another metal atom of approx same size can substitute . E.g. - Nickel or Chromium substituting iron in stainless steel.
44
Basic Properties of Materialsb.Vacancies:
2.Line defects: Dislocations along a line. Plastic deformations of metals occurs –motion of dislocations.
These are empty atom sites.
45
Basic Properties of Materials Edge dislocation
Sufficiently large force- bonds broken and new bonds formed.
Slip plane + Slip direction = Slip system
46
Basic Properties of Materials Significance of slip planes-
Shear stress atoms of the crystal can glide.
More the slip planes easier is it to deform.
Slip planes intercepted at grain boundaries.
47
Basic Properties of Materials
Elastic deformation
Plastic deformation
Greater stress - fracture
48
Basic Properties of Materials Twinning – alt. mode of permanent deformation. Seen in metals-few slip planes (NiTi & α-
titanium) Small atomic movements on either side of a
twinning plane results in atoms with mirror relationship
49
Basic Properties of Materials Also the mechanism for reversible
transformation-austenite to martensite.• A movement that divides the lattice into 2 planes at a certain angle.•NiTi – multiple twinning•Subjected to a higher temperature, stress
de - twinning occurs (shape memory)
50
Basic Properties of Materials Cold working ( strain hardening or work
hardening)
• Dislocations pile up along the grain boundaries.
• Hardness & strength ductility
• Plastic deformation-difficult.
• During deformation - atomic bonds within the crystal get stressed
resistance to more deformation
51
Basic Properties of Materials An interesting effect of cold work-crystallographic
orientation in the distorted grain structure.
Anisotropic (direction dependant) mechanical properties.
Slip planes align with shear planes.
Wires – mechanical properties different when measured parallel and perpendicular to wire axis.
52
Basic Properties of Materials Implications: Fine grained metals with large no. of grains
- stronger
•Enhancing crystal nucleation by adding fine particles with a higher melting point, around which the atoms gather.
•Preventing enlargement of existing grains. Abrupt cooling (quenching) of the metal.
•Dissolve specific elements at elevated temperatures. Metal is cooled
Solute element precipitates barriers to the slip planes.
53
Basic Properties of Materials The effects of cold working can be reversed-
heating the metal to appropriate temperature- Annealing
• Relative process-heat below the melting temperature •More the cold work, more rapid the annealing
•Higher melting point – higher annealing temp
•Rule of thumb-½ the melting temperature (°K)
54
Basic Properties of Materials Recovery-cold work disappears.
• Ortho appliances heat treated (recovery temperature)-
• stabilizes the configuration of the appliance and
• reduces-fracture.
Recrystallization –severely cold worked-after recovery-radical change in microstructure.
• New stress free grains• Consume original cold worked structure. • Inc. ductility ,dec. resiliency
55
Basic Properties of Materials
Grain growth - minimizes the grain boundary area.
•Coarse grains
56
Basic Properties of Materials Before Annealing
Recovery – Relief of stresses
Recrystallization – New grains from severely cold worked areas
Grain Growth – large crystal “eat up” small ones
57
Basic Properties of MaterialsPolymorphism Metals and alloys exist as more than one type of
structure
Transition from one to the other-reversible- Allotropy
Steel and NiTi
58
Basic Properties of Materials
Steel -alloy of iron and carbon Iron – 2 forms-
• FCC-above 910°c• BCC-below-Carbon practically insoluble.
(0.02%) •Iron FCC form (austenite)
•Lattice spaces greater
•Carbon atom can easily be incorporated into the unit cell
59
Basic Properties of Materials On Cooling
FCC BCC
Carbon diffuses out as Fe3C
Cementite adds strength to ferrite and austenite
Rapidly cooled (quenched)
Carbon cannot escape
Distorted body centered tetragonal lattice called martensite
Too brittle-tempered-heat b/w 200-450°C –held at a given temp for known length of time-cooled rapidly.
60
Basic Properties of Materials
61
Basic Properties of Materials Austenite (FCC)
slow cooling rapid cooling
Mixture of: Tempering Martensite (BCT) Ferrite(BCC) distorted lattice-
& Pearlite hard & brittle
Cementite(Fe3C)
62
Basic Properties of Materials NiTi-
• Transformations –temperature & stress.• Austenite (BCC)• Martensitic (Distorted monoclinic, triclinic,
hexagonal structure.
Austenite- high temperature & low stress.Martensite –low temperature & high stress. Twinning-Reversible below elastic limit
Transformations and reverse-not same temperature-hysteresis
63
Basic Properties of Materials Bain distortion
• Transformations occur without chemical change or diffusion
• Result-crystallographic reln b/w parent and new phase
• Rearrangement of atoms-minor movements
64
Evolution of Materials Gold 1887-Neusilber brass (Cu,Ni,Zn) 1919-Stainless steel 1950s-Cobalt chromium 1962-NiTiNOL-1970-Orthodontia Early 1980s-β-titanium 1985,86-superelastic NiTi 1989-α-Titanium 1990s- Cu NiTi, Ti Nb and Timolium 2000-β-III
65
Basic Properties of Materials Metallic bond-properties
Crystals & lattices
Imperfections
Edge dislocations, Twinning
Cold working
Annealing
Polymorphism
Bain distortion
66
Making an orthodontic wire Sources Stainless steel- based on standard formulas of AISI.
After manufacture –further selection to surpass the basic commercial standard
Orthodontists –small yet demanding customers
Chrome – cobalt and titanium alloys- fixed formulas
Gold –supplier’s own specification.
67
Making an orthodontic wire 4 steps in wire production 1. Melting
2.The Ingot
3.Rolling
4.Drawimg
68
Making an orthodontic wire Melting -Selection and melting of alloy materials-
important -Physical properties influenced -Fixes the general properties of the metal
The Ingot -Critical step- pouring the molten alloy into mold - Non –uniform chunk of metal - Varying degrees of porosities and inclusions of
slag.
69
Making an orthodontic wire -Microscopy –grains –influence mechanical
properties. -Size and distribution of grains –rate of cooling
and the size of ingot. -Porosity -2 sources
o Gases dissolved or producedo Cooling and shrinking –interior cools
late -Ingot – trimmed
Important to control microstructure at this Important to control microstructure at this
stage – basis of its physical properties and stage – basis of its physical properties and
mechanical performancemechanical performance
70
Making an orthodontic wire Rolling
- 1st mechanical step-rolling ingot –long bars
-Series of rollers – reduced to small diameter
-Different parts of ingot never completely lose identity
-Metal on outside of ingot-outside the finest wire, likewise ends
- Different pieces of wire same ingot differ depending on the part they came from
-Individual grains also retain identity
71
Making an orthodontic wire -Each grain elongated in the same proportion as the
ingot
-Mechanical rolling-forces crystals into long finger-like shapes –meshed into one another
-Work hardening-increases the hardness and brittleness
-if excess rolling-small cracks
-Annealing –atoms become mobile-internal stresses relieved
-More uniform than original casting
-Grain size controlled
72
Making an orthodontic wire Drawing -Further reduced to final
size
-Precise process –wire pulled through a small hole in a die
- Hole slightly smaller than the starting diameter of the wire – uniformly squeezed
-Wire reduced to the size of die
73
Making an orthodontic wire - Many series of dies
- Annealed several times at regular intervals
- Exact number of drafts and annealing cycles depends on the alloy (gold <carbon steel<stainless steel)
74
Making an orthodontic wire Rectangular wires -Draw through rectangular die or roll round
wires to rectangular shape
-Little difference in the wires formed by the 2 processes
-Drawing –produces sharper corners –advantageous in application of torque
75
Making an orthodontic wire Hardness and spring properties depend–entirely
on the effects of work hardening during manufacture
Drawing –Annealing schedule –planned carefully with final properties & size in mind
Metal almost in need of annealing at final size-maximum spring prop.
Drawing carried too far-brittle, not enough-residual softness.
76
77
Mechanical properties
Strength-ability to resist stress without fracture or strain (permanent deformation).
Stress & strain-internal state of the material.
Stress-internal distribution of load – force/ unit area (Internal force intensity resisting the applied load)
Strain- internal distortion produced by the load- deflection/unit
length (change in length/original length)
78
Mechanical properties Material can be stressed in 4 ways-
• Compression
• Tensile
• Shear
• Complex force systems
79
Mechanical properties Evaluation of mechanical properties –
• Bending tests• Tension tests• Torsional tests
Bending tests : 3 types• A cantilever bending test-Oslen stiffness tester
(ADA-32)• 3 point• 4 point
80
Mechanical properties
Universal testing machine
81
Mechanical properties
82
Mechanical properties
The modulus of elasticity calculated from the force-deflection plot, using equations from solid mechanics.
Cantilever bending test-incompatible with flexible wires-(NiTi and multistranded).
Disadvantage of 3 point-bending moment-maximum at loading point to zero at the 2 supports.
4 point –uniform bending moment-specimen fails at the weakest point.
83
Mechanical properties Nikolai et al proposed a 5 point bending test: -2 loading points at each end-simulate a
couple. -simulates engagement of arch wire in bracket.
Tensile testing-strain - rate mechanical testing machine is used.
84
Elastic properties Stress-Strain relationship (ductile material)
85
Elastic properties
STRAIN
STR
ES
S
Elastic portion
Wire returns back to original dimension when stress is removed
(Hooke’s law)(Hooke’s law)
86
Elastic properties
0.1%
stre
ss
strain
Elastic limit
Proportional limit Yield point
87
Elastic properties Elastic /Proportional limit-used interchangeably
Proportional limit –determined by placing a straight edge on the stress-strain plot.
Elastic limit -determined with aid of precise strain measurement apparatus in the lab.
Yield strength (Proof stress) -PL-subjective ,YS used to for designating onset of permanent deformation.0.1% is reported.
Determined by intersection of curved portion with 0.1% strain on horizontal axis.
88
Elastic properties
Ultimate tensile strength Fracture point
stre
ss
strain
Plastic deformation
89
Elastic properties Ultimate tensile strength -the maximum load the
wire can sustain (or) maximum force that the wire can deliver.
Permanent (plastic) deformation -before fracture-removal of load-stress-zero, strain = zero.
Fracture -Ultimate tensile strength higher than the stress at the point of fracture reduction in the diameter of the wire
(necking)
90
Elastic properties
Slope α Stiffness Stiffness α 1
Springiness
stre
ss
strain
91
Elastic properties Slope of initial linear region- modulus of
elasticity (E). (Young’s modulus)
• Corresponds to the elastic stiffness or rigidity of the material
• Amount of stress required for unit strain
• E = σ/ε where σ does not exceed PL (Hookean elasticity)
• The more horizontal the slope-springier the wire; vertical-stiffer
92
Elastic properties
93
Elastic properties
Springback deflection
forc
e
Range
YP
Point of arbitrary clinical loading
94
Elastic properties of metals Range-
• Proffit-Distance that the wire bends elastically, before permanent deformation occurs
• Kusy – Distance to which an archwire can be activated-
• Thurow – A linear measure of how far a wire or material can be deformed without exceeding the limits of the material.
95
Springback-• Proffit- Portion of the loading curve b/w elastic
limit and ultimate tensile strength.
•Kusy - The extent to which the range recovers upon deactivation
•Ingram et al – a measure of how far a wire can be deflected without causing permanent deformation.
•Kapila & Sachdeva- YS/E
96
Elastic properties
resi
lien
cy
form
ab
ilit
y
YP
PL
stre
ss
strain
97
Elastic properties Resiliency-Area under stress-strain curve till
proportional limit. -Maximum amount of energy a material
can absorb without undergoing permanent deformation.
When a wire is stretched, the space between the atoms increases. Within the elastic limit, there is an attractive force between the atoms.
Energy stored within the wire.
Strength + springiness
98
Elastic properties Work = f x d
• When work is done on a body-energy imparted to it.
• If the stress not greater than the PL elastic energy is stored in the structure.
• Unloading occurs-energy stored is given out
99
Elastic properties It depends on –
Stiffness and Working Range
Independent of – Nature of the material Size (or) Form
100
Elastic properties Formability –
• Amount of permanent deformation that the wire can withstand before failing.
• Indication of the ability of the wire to take the shape
• Also an indication of the amount of cold work that it can withstand
101
Elastic properties Flexibility –• Amount a wire can be strained without
undergoing plastic deformation.
• Large deformation (or large strain) with minimal force, within its elastic limit.
• Maximal flexibility is the strain that occurs when a wire is stressed to its elastic limit.
Max. flexibility = Proportional limit Modulus of elasticity.
102
Elastic properties st
ress
strain
Toughness
103
Elastic properties Toughness –Amount of elastic & plastic
deformation required to fracture a material. Total area under the stress – strain graph.
Brittleness –Inability to sustain plastic deformation before fracture occurs.
Fatigue – Repeated cyclic stress of a magnitude below the fracture point of a wire can result in fracture. Fatigue behavior determined by the number of cycles required to produce fracture.
104
Elastic properties Poisson’s ratio (ν) ν = - εx/ εy = -εy / εz
Axial tensile stress (z axis) produces elastic tensile strain and accompanying elastic contractions in x in y axis.
The ratio of x,y or x,z gives the Poissons ratio of the material
It is the ratio of the strain along the length and along the diameter of the wire.
105
Elastic properties Ductility –ability to sustain large permanent
deformation under tensile load before fracturing. Wires can be drawn
Malleability –sustain deformation under compression-hammered into sheets.
106
Requirements of an ideal arch wire Robert P.Kusy- 1997 (AO) 1. Esthetics2. Stiffness3. Strength4. Range5. Springbac
k6. Formabilit
y
7.Resiliency8.Coefficient of
friction9.Biohostability10.Biocompatibility11.Weldability
107
Requirements of an ideal arch wire Esthetic •Desirable
•Manufacturers tried-coating -White coloured
wires
• Deformed by masticatory loads
•Destroyed by oral enzymes
•Uncoated-transparent wires-poor mechanical
properties
•Function>Esthetics
•Except the composite wires
108
Requirements of an ideal arch wire Stiffness / Load –Deflection Rate
•Proffit: - Slope of stress-strain curve
•Thurow - Force:Distance ratio, measure of
resistance to deformation.
•Burstone – Stiffness is related to – wire property
& appliance design
Wire property is related to – Material & cross
section.
•Wilcock – Stiffness α Load
Deflection
109
Requirements of an ideal arch wire
Magnitude of the force delivered by the appliance
for a particular amount of deflection.
Low stiffness or Low LDR implies that:-
1) Low forces will be applied
2) The force will be more constant as the appliance
deactivates
3) Greater ease and accuracy in applying a given
force.
110
Requirements of an ideal arch wire
Strength
• Yield strength, proportional limit and ultimate
tensile & compressive strength
• Kusy - Force required to activate an archwire to
a specific distance.
• Proffit - Strength = stiffness x range.
• Range limits the amount the wire can be bent,
stiffness is the indication of the force required to
reach that limit.
111
Requirements of an ideal arch wire Range
•Distance to which an archwire can be activated
• Distance wire bends elastically before permanent deformation.
•Measured in millimeters.
112
Requirements of an ideal arch wire Springback • The extent to which the range recovers upon
deactivation
•Clinically useful-many wires deformed -wire performance-EL & Ultimate strength
113
Requirements of an ideal arch wire
Formability
• Kusy – The ease in which a material may be
permanently deformed.
• Clinically- Ease of forming a spring or
archwire
114
Requirements of an ideal arch wire
Resiliency
• Store/absorb more strain energy /unit volume
before they get permanently deformed
• Greater resistance to permanent deformation
• Release of greater amount of energy on
deactivation
High work availability to move the teeth
115
Requirements of an ideal arch wire Coefficient of Friction
• Brackets (and teeth) must be able to slide along
the wire
• Independent of saliva-hydrodynamic boundary
layer
• High amounts of friction anchor loss.
• Titanium wires inferior to SS
116
Requirements of an ideal arch wire Biohostability- •Site for accumulation of bacteria, spores or viruses.
• An ideal archwire must have poor biohostability.
•Should not-actively nurture nor passively act as a substrate for micro-organisms/spores/viruses
•Foul smell, discolouration, build up of material-compromise mechanical properties.
117
Requirements of an ideal arch wire Biocompatability
• Ability of a material to elicit an appropriate biological response in a given application in the body
• Wires-resist corrosion –products – harmful
• Allergies
• Tissue tolerance
118
Requirements of an ideal arch wire Weldability –
• Process of fusing 2 or more metal parts though application of heat, pressure or both with/out a filler metal to produce a localized union across an interface.
• Wires –should be easily weldable with other metals
119
Elastic properties Thurow - 3 characteristics of utmost importance
- Important for the orthodontist –selection of the material and design-any change in 1 will require compensatory change in others.
Strength = Stiffness x Range
120
Elastic properties Clinical implications:• The properties can be expressed in absolute
terms -in orthodontics-simple comparison.
• Main concern-change in response – if there is change in material, wire size or bracket arrangement.
• Knowledge- force and movement can be increased or decreased in certain circumstances
Comparing the 3 properties
121
Elastic properties Stiffness indicates- rate of force delivery how much force how much distance can be covered
Strength –measures the load or force that carried at its maximum capacity
Range-amount of displacement under maximum load
122
Elastic properties Factors effecting the 3 components
- Mechanical arrangement-includes bracket
width, length of arch wire.
-Form of wire-size, shape & cross-section
- Alloy formula, hardness, state of heat
treatment
123
Optimal Forces & Wire Stiffness
Varying force levels produced during deactivation of a wire: excessive, optimal, suboptimal, & subthreshold.
During treatment by a wire with high load deflection rate the optimal zone is present only over a small range
124
Optimal Forces & Wire Stiffness
Overbent wire with low load-deflection rate (Burstone) Tooth will reach desired position before subthreshold force zone is reached. Replacement of wires is not required
125
Effects of wire cross-section Variable-cross section orthodontics How does change in size and shape of wire
effect stiffness, strength & springiness? Considering a cantilever beam;
126
Effects of wire cross-section Doubling diameter makes beam 8 times stronger But only 1/16 times springy ½ the range.
Strength changes as a cubic fn of the ratio of the 2 cross sections.
Springiness-4th power Range-direct proportion
127
Effects of wire cross-section Rectangular wire
The principle is same In torsion more shear stress rather than bending
stress in encounteredHowever the principle is same
Increase in diameter – increase in stiffness & strength
rapidly– too stiff for orthodontic use & vice-versa
Ideally wire should be in b/w these two extremes
128
Effects of wire cross-section Wire selection-based on load -deflection rate requirement -magnitude of forces and moments
required
Is play a factor? Wire ligature minimizes the play in I order
direction as wires can seat fully. Narrow edgewise brackets-ligature tie tends to
minimize No point-0.018” over 0.016-diffrence in play.
129
Effects of wire cross-section Should a smaller wire be chosen to obtain
greater elastic deflection? Elastic deflection varies inversely with
diameter of wire but differences are negligible- 0.016 has 1.15 times maximum elastic deflection
as 0.018 wire. Major reason- load deflection rate Small changes in the wire produce large changes
in L-D rate Determined by moment of inertia.
130
Effects of wire cross-sectionShape Moment of
InertiaRatio to stiffness of round wire
Пd4
641
s4
121.7
b3h12
1.7 b3hd4
131
Effects of wire cross-section The clinician needs a simplified system to
determine the stiffness of the wire he uses. Cross-sectional stiffness number (CS)-relative
stiffness 0.1mm(0.004in) round wire-base of 1.
132
Effects of wire cross-section
133
Effects of wire cross-section
0
500
1000
1500
2000
2500
3000
3500
Sti
ffn
es
s n
um
be
r (B
urs
ton
e)
14 16 18 20 22 16x16 18x18 21x21 16x22 22x16 18x25 25x18 21x25 25x21 215x28 28x215
Wire dimension
Relative stiffness
134
Effects of wire cross-section Rectangular wires • Bending perpendicular to the larger dimension
(ribbon mode) • Easier than bending perpendicular to the
smaller dimension (edgewise).
•The larger dimension correction is needed.
•The smaller dimension the plane in which more stiffness is needed.
135
> first order, < second order – RIBBON
> Second order, < first order - EDGEWISE
Effects of wire cross-section
•> 1st order correction in anterior segment
•> 2nd order in the posterior segment, wire can be twisted 90°•Ribbon mode in anterior region and edgewise in posterior region.
136
Effects of wire cross-section Both, 1st & 2nd order corrections are required to
the same extent, then square or round wires.
The square wires - advantage -simultaneously control torque
better orientation into a rectangular slot. (do not turn and no unwanted forces are
created).
137
Mechanical & Elastic properties Ideal requirements of an arch wires Strength, stiffness & range Optimal forces and wire stiffness
Effects of cross-section Strength changes as a cubic fn of the ratio of the
2 cross sections. Springiness-4th power Range-direct proportion
Orthodontic wires
138
Effects of length Changing the length-dramatically affects
properties Considering a cantilever ;
139
Effects of length If length is doubled-• Strength – cut by half-(decreases
proportionately)• Springiness – inc. 8 times ( as a cubic function)• Range – inc 4 times (increases as a square.)In the case of torsion, the picture is slightly different. Increase in length –
•Stiffness decreases proportionately•Range increases proportionately•Strength remains unchanged.
140
Effects of length Way the beam is attached also affects the values Cantilever, the stiffness of a wire is obviously
less Wire is supported from both sides (as an
archwire in brackets), again, the stiffness is affected
• Method of ligation of the wire into the brackets.
•Loosely ligated, so that it can slide through the brackets, it has ¼th the stiffness of a wire that is tightly ligated.
141
Effects of material Modulus of elasticity varied by changing the
material Material stiffness number-relative stiffness of the
material Steel -1.0(Ms)
142
Effects of material
143
Nomograms Developed by Kusy
Graphic representation-comparing wire materials
and sizes
Fixed charts that display mathematical
relationships-scales
Nomograms of each set drawn to same base, any
wire on 1 of 3 can be compared to any other.
144
A reference wire is chosen (0.012”SS) and given a value of 1 . The strength , stiffness and range of other wires are calculated to this reference
Nomograms
145
Nomograms
146
Nomograms
147
Clinical implications Balance between stiffness, strength &
range
Vary - material ,cross-section or length as the situation demands.
148
Clinical implications Variation in Cross-Section
Wires with less cross-section-low stiffness (changes by 4th power)
Used initial part of treatment Thicker-stiffer wires used later
149
Clinical implications Multi-stranded wires 2 or more wires of smaller diameter are twisted
together/coiled around a core wire
Twisting of the two wires causes the strength to increase, so that the wire can withstand masticatory forces.
The properties of multistranded wires depend on the individual wires that are coiled, and on how tightly they are coiled together.
150
Clinical implications
Variation in length
•Removable appliance -cantilever spring
•The material of choice is usually steel. (Stiff material)
•Good strength to resist masticatory and other oral forces.
151
Clinical implications Increase the length of the wire-
Proportionate decrease in strength, but the stiffness will decrease as a cubic function
Length is increase by either bending the wire over itself, or by winding helices or loops into the spring
152
Clinical implications Fixed appliance
The length of wire between brackets can be
increased
Loops, or Smaller brackets,
or Special bracket designs –Mini-unitwin
bracket,Delta
153
Clinical implications Variation in the material
Relatively constant dimension important for the third order control
Titanium wires-low stiffness-used initial part of treatment
Steel-when rigidity-control and torque expression required
154
Clinical implications
155
Clinical implicationsStage Wires Reason
Aligning Multistranded SS,NiTi
Great range and light forces are reqd
Space closure Β-Ti (frictionless), SS – if sliding mechanics is needed
Increased formability, springback , range and modest forces per unit activation are needed
Finishing SS , preferably rectangular
More stability & less tooth movement reqd
156
Clinical implicationsStage Wires Reason
Aligning Multistranded SS,Low LDR-SS
Great range and light forces are reqd
Space closure SS(high resilience aust.wire) – sliding mechanics
Increased formability, springback , range and modest forces per unit activation are needed
Finishing SS , α-titanium More stability & less tooth movement reqd
157
Clinical implicationsA rough idea can be obtained clinically
Forming an arch wire with the thumb gives an indication of the stiffness of the wire.
Flexing the wires between the fingers, without deforming it, is a measure of flexibility
Deflecting the ends of an archwire between the thumb and finger gives a measure of resiliency.
158
Physical properties Corrosion Chemical or electrochemical
process in which a solid, usually a metal, is attacked by an environmental agent, resulting in partial or complete dissolution.
Not merely a surface deposit –deterioration of metal
Localized corrosion-mechanical failure Biological effects-corrosion products
159
Physical propertiesNickel -1. Carcinogenic, 2. Mutagenic, 3. Cytotoxic and 4. Allergenic.
Stainless steels, Co-Cr-Ni alloys and NiTi are all rich in Ni
Co & Cr can also cause allergies.
160
Physical properties Studies-Ni alloy implanted in the tissue
Although-more invasive –reactivity of the implanted material is decreased –connective tissue capsule
Intraoral placement-continuous reaction with environment
Corrosion resistance of steel- SS- passivating layer-Cr-also contains Fe, Ni, Mo
161
Physical properties Passivating film-inner oxide layer-mainly-Cr
oxide outer- hydroxide layer Elgiloy-similar mechanism of corrosion
resistance
Titanium oxides-more stable
Corrosion resistance of SS inferior to Ti alloys
162
Physical properties -Forms of corrosion1. Uniform attack – Commonest type The entire wire reacts with the environment Hydroxides or organometallic compounds Detectable after a large amount of metal is
dissolved.
2. Pitting Corrosion – Manufacturing defects Sites of easy attack
163
Physical properties Excessive porous surface-as received wires
Steel NiTi
164
Physical properties
3.Crevice corrosion or gasket corrosion -
Parts of the wire exposed to corrosive environment
Non-metallic parts to metal (sites of tying)
Difference in metal ion or oxygen concentration
Plaque build up disturbs the regeneration of the
passivating layer
Depth of crevice-reach upto 2-5 mm
High amount of metals can be dissolved in the mouth.
165
Physical properties
166
Physical properties4.Galvanic /Electrochemical Corrosion
Two metals are joined Or even the same metal after different type of
treatment are joined
Difference in the reactivity
Galvanic cell.
Less Reactive More Reactive
(Cathodic) (Anodic) less noble metal
167
Physical properties Less noble metal-oxidizes-anodic-soluble
Nobler metal-cathodic-corrosion resistant
“Galvanic series”
SS-can be passive or active depending on the nobility of the brazing material
168
Physical properties5.Intergranular corrosion Sensitization - Precipitation of CrC-grain
boundaries
-Solubility of chromium carbide
6.Fretting corrosion6.Fretting corrosion
Material under load
Wire and brackets contact –slot – archwire interface
Friction surface destruction
Cold welding -pressure rupture at contact points-wear oxidation pattern
169
Physical properties7.Microbiologically influenced corrosion (MIC)
Sulfate reducing-Bacteroides corrodens
Matasa – Ist to show attack on adhesives in
orthodontics
Craters in the bracket
Certain bacteria dissolve metals directly form the
wires.
Or by products alter the microenvironment-
accelerating corrosion
170
Physical properties
171
Physical properties8.Stress corrosion Similar to galvanic corrosion-electrochemical
potential difference-specific sites
Bending of wires - different degrees of tension and compression develops locally
Sites-act as anodes and cathodes.
172
Physical properties 9.Corrosion9.Corrosion Fatigue:Fatigue: Cyclic stressing of a wire-aging
Resistance to fracture decreases
Accelerated in a corrosive medium such as saliva
Wires left intraorally-extended periods of time under load
173
Physical properties Corrosion – Studies
In vitro Vs In vivo
Never simulate the oral environment
Retrieval studies
Biofilm-masks alloy topography
Organic and inorganic components
Mineralized –protective esp. low pH
174
Physical properties Ni hypersensitivity-case reports-very scarce
Insertion of NiTi wires – rashes swelling Erythymatous lesions
Ni and Cr impair phagocytosis of neutrophils and impair chemotaxis of WBCs.
175
Physical properties Ni at conc. released from dental alloys
Activating monocytes and endothelial cells, Promote intercellular adhesion(molecule 1) Promotes inflammatory response in soft
tissues.
Arsenides and sulfides of Ni - carcinogens and
mutagens.
Ni at non toxic levels - DNA damage.
176
177
Stainless steel Gold
1960s-Abandoned in favour of stainless steel
Crozat appliance –original design
1919 – Dr. F Hauptmeyer –Wipla (wie platin).
•Extremely chemically stable•Better strength and springiness• High resistance to corrosion-
Chromium content.
178
Stainless steel Properties of SS controlled-varying the degree of
cold work and annealing during manufacture
Steel wires-offered in a range of partially annealed states –yield strength progressively enhanced at the cost of formability compromised
Fully annealed stainless steel extremely soft, and highly formable
Ligature wire-“Dead soft”
179
Stainless steel
Steel wires with high yield strength- “Super” grade wires-brittle-used when sharp bends are not needed
High formability- “regular” wires-bent into desired shapes
180
Stainless steel Structure and composition
Iron –always contains carbon-(2.1%)
When aprrox 12%-30% Cr added- stainless
Cr2O3-thin transparent, adherent layer when
exposed to oxidizing atm.
Passivating layer-ruptured by
chemical/mechanical means-protective layer
reforms
Favours the stability of ferrite (BCC)
181
Stainless steel
Nickel(0-22%) – Austenitic stabilizer (FCC)
Loosly bound
Copper, manganese and nitrogen – similar
function
Mn-dec corrosion resistance
Carbon (0.08-1.2%)– provides strength Reduces the corrosion resistance
182
Stainless steel Sensitization.
400-900oC-looses corrosion resistance During soldering or welding
Chromium diffuses towards the carbon rich areas (usually the grain boundaries)-chromium carbide-most rapid 650°C
Chromium carbide is soluble- intergranular corrosion.
183
Stainless steel 3 methods to prevent sensitization-
1. Reduce carbon content-precipitation cannot occur-not economically feasible
2. Severely cold work the alloy-Cr carbide ppts at dislocations-more uniform
Stabilization Addition of an element which precipitates
carbide more easily than Chromium. Niobium, tantalum & titanium
184
Stainless steel Usually- Titanium.
Ti 6x> Carbon
No sensitization during soldering.
Most steels used in orthodontics are not stabilized-additional cost
185
Stainless steel Other additions and impurities-
Silicon – (low concentrations) improves the resistance to oxidation and carburization at high temperatures and corrosion resistance
Sulfur (0.015%) increases ease of machining
Phosphorous – allows sintering at lower
temperatures.
But both sulfur and phosphorous reduce the
corrosion resistance.
186
Stainless steel Classification
American Iron and Steel Institute (AISI)
Unified Number System (UNS)
German Standards (DIN).
187
Stainless steel
The AISI numbers used for stainless steel range
from 300 to 502
Numbers beginning with 3 are all austenitic
Higher the number
Less the non-ferrous content
More expensive the alloy
Numbers having a letter L signify a low
carbon content
188
Basic Properties of Materials Austenite (FCC)
slow cooling rapid cooling
Mixture of: Tempering Martensite (BCT) Ferrite(BCC) distorted lattice-
& Pearlite hard & brittle
Cementite(Fe3C)
189
Stainless steel
190
Stainless steel
Austenitic steels (the 300 series)
Most corrosion resistance
FCC structure, non ferromagnetic
Not stable at room temperature,
Austenite stabilizers Ni, Mn and N
191
Stainless steel Type 302-basic alloy -17-
19% Cr,8-10% Ni,0.15%-C
304- 18-20%-Cr, 8-12%-Ni,0.08%-C
Known as the 18-8 stainless steels- most common in orthodontics
316L-10-14%-Ni,2-3%-Mo,16-18%-Cr,O.03%-C-implants
192
Stainless steel The following properties-
Greater ductility and malleability More cold work-strengthened Ease –welding Dec. sensitization Less critical grain growth Ease in forming
X-ray diffraction-not always single phase-Bcc martensitic phase present
193
Stainless steel Khier,Brantly,Fournelle(AJO-1998)
Austenitic structure-metastable
Decomposes to martensite-cold work & heat treatment
Manufacturing process
194
Stainless steel
Martensitic steel (400)
FCC BCC
BCC structure is highly stressed. (BCT) More grain boundaries,
Stronger Dec. ductulity-2% Less corrosion resistant
Making instrument edges which need to be sharp and wear resistant.
195
Stainless steel
196
Stainless steel
Ferritic steels – (the 400 series)
Name derived from the fact-microstr (BCC) same as
iron
Difference-Cr
“super ferritics”-19-30% Cr-used Ni free brackets
Good corrosion resistance, low strength.
Not hardenable by heat treatment-no phase change
Not readily cold worked.
197
Stainless steel
Duplex steels
Both austenite and ferrite grains
Fe,Mo,Cr, lower nickel content
Increased toughness and ductility than ferritic
steels
Twice the yield strength of austenitic steels
High corrosion resistant-heat treated –sigma-dec
corrosion resistance
Manufacturing low nickel attachments-one piece
brackets
198
Stainless steel
Precipitation hardened steels
Certain elements added to them precipitate and increase the hardness on heat treatment.
The strength is very high
Resistance to corrosion is low.
Used to make mini-brackets.
199
Stainless steel -General properties
1. Relatively stiff material
Yield strength and stiffness can be varied
Altering diameter/cross section
Altering the carbon content and
Cold working and
Annealing
High forces - dissipate over a very short amount
of deactivation (high load deflection rate).
200
Stainless steel In clinical terms-
•Loop - activated to a very small extent so as to achieve optimal force but
•Deactivated by only a small amount (0.1 mm) force level will drop tremendously
•Type of force-Not physiologic
•More activations
201
Stainless steel Force required to engage a steel wire into a
severely mal-aligned tooth.
Either cause the bracket to pop out,
Or the patient to experience pain.
Overcome by using thinner wires, which have a
lower stiffness.
Not much control.
202
Stainless steel
High stiffness can be advantageous
Maintain the positions of teeth & hold the
corrections achieved
Begg treatment, stiff archwire, to dissipate the
adverse effects of third stage auxiliaries
203
Stainless steel
2. Lowest frictional resistance
Ideal choice of wire during space closure with
sliding mechanics
Teeth will be held in their corrected relation
Minimum resistance to sliding
204
Stainless steel3.High corrosion resistance Ni is used as an austenite stabilizer.
Not strongly bonded to produce a chemical
compound.
Likelihood of slow release of Ni
Symptoms in sensitized patients
205
Stainless steel
Passivating layer dissolved in areas of plaque
accumulation – Crevice corrosion.
Different degrees of cold work – Galvanic
corrosion
Different stages of regeneration of passivating
layer – Galvanic corrosion
Sensitization – Inter-granular corrosion
206
Stainless steel
1919-SS introduced
Structure and composition-stainless
Classifications
FCC-BCC
General properties
207
208
High Tensile Australian Wires Claude Arthur J. Wilcock started association with
dental profession-1936-37
Around 1946-asssociation with Dr.Begg
Flux, silver solder, lock pins, brackets, bands, ligature wires, pliers & high tensile wire
Needed-wires that were active for long
Dr Begg-progressively harder wires
209
High Tensile Australian Wires Beginners found it difficult to use the highest
tensile wires Grading system Late 1950s, the grades available were –
Regular Regular plus Special Special plus
210
High Tensile Australian Wires Demand-very high-1970s
Raw materials overseas
Higher grades-Premium
Preformed appliances, torquing auxiliaries, springs
Problems-impossibility in straightening for appliances
-work softening-straightening
-breaking
211
High Tensile Australian Wires
•Higher working range-
E (same) But inc. YS
Range=YS/E
•Higher resiliency
ResilαYS2/E
•Zero stress relaxation
•Reduced formability
212
High Tensile Australian WiresZero Stress Relaxation If a wire is deformed and held in a fixed position,
the stress in the wire may diminish with time, but the strain remains constant.
Property of a wire to deliver a constant light elastic force, when subjected to external forces (like occlusal forces).
Only wires with high yield strength-possess this desirable property
213
High Tensile Australian Wires Relaxation in material- Slip dislocation
Materials with high YS-resist such dislocations-internal frictional force.
New wires-maintain their configuration-forces generated are unaffected
214
High Tensile Australian Wires Zero stress relaxation in springs.
To avoid relaxation in the wire’s working stress
Diameter of coil : Diameter of wire = 4 (spring index)
smaller diameter of wires smaller diameter springs
(like the mini springs)
Higher grade wires (high YS), ratio can be =2, much
lighter force
Bite opening anchor bends- zero stress relaxation –infrequent
reactivation
215
High Tensile Australian Wires Spinner straightening
It is mechanical process of straightening resistant materials in the cold-hard drawn condition
The wire is pulled through rotating bronze rollers that torsionally twist it into straight condition
Wire subjected to tension-reverse straining. Disadv:
Decreases yield strength (strain softened) Creates rougher surface
216
High Tensile Australian Wires
Straightening a wire - pulling through a series of
rollers
Prestrain in a particular direction.
Yield strength for bending in the opposite
direction will decrease.
217
High Tensile Australian Wires
Bauschinger effect
Described by Dr. Bauschinger in 1886.
Material strained beyond its yield point in one
direction,
then strained in the reverse direction,
its yield strength in the reverse direction is
reduced.
218
High Tensile Australian Wires
roundning
219
High Tensile Australian Wires
Plastic prestrain increases the elastic limit of
deformation in the same direction as the prestrain.
Plastic prestrain decreases the elastic limit of
deformation in the direction opposite to the prestrain.
If the magnitude of the prestrain is increased, the
elastic limit in the reverse direction can reduce to zero.
220
High Tensile Australian Wires JCO,1991 Jun(364 - 369): Clinical Considerations
in the Use of Retraction Mechanics - Julie Ann Staggers, Nicholas Germane
The range of action will be greatest in the direction of the last bend
With open loop, activation unbends loop; but with closed loop, activation is in the direction of the last bend -increases range of activation.
Premium wire special plus or special wire
221
222
High Tensile Australian Wires Pulse straightening Placed in special machines that permits
high tensile wires to be straightened.
This method :Permits the straightening of high tensile wires1. Does not reduce the yield strength of the wire2. Results in a smoother wire, hence less wire –
bracket friction.
223
High Tensile Australian Wires Dr.Mollenhauer requested –ultra high tensile
SS round wire.
Supreme grade wire –lingual orthodontics-initial
faster and gentler alignment of teeth-brackets
close
Labial Begg brackets-reduces tenderness
Intrusion simultaneously with the base wires
Gingival health seemed better
224
High Tensile Australian Wires Higher yield strength
more flexible Supreme grade
flexibility = β-titanium.
Higher resiliency
nearly three times.
NiTi higher flexibility but it lacks formability
225
High Tensile Australian Wires
Methods of increasing yield strength of Australian wires.
1. Work hardening
2. Dislocation locking
3. Solid solution strengthening
4. Grain refinement and orientation
226
High Tensile Australian WiresTwelftree, Cocks and Sims (AJO 1977) Wires-0.016-7 wires Premium plus, Premium and Special plus wires
showed minimal stress relaxation-no relaxation -3 days
Special, Remanit, Yellow Elgiloy, Unisil. Special plus maintained original coil size, Unisil-
inc. curvature
227
High Tensile Australian Wires Hazel, Rohan & West (1984)
Stress relaxation of Special plus wires after 28 days was less than Dentaurum SS and Elgiloy wires.
Barrowes (82) Sp.plus greater working range than stnd. SS but
NiTi,TMA & multistranded-greater
Jyothindra Kumar (89) -evluated working range Australian wires-better recovery than Remanuim
228
High Tensile Australian Wires Pulse straightened wires – Spinner
straightened
(Skaria 1991)
Strength, stiffness and Range higher than spinner staightened wires
Coeff. of friction higher-almost double
Similar- surface topography, stress relaxation and Elemental makeup.
229
High Tensile Australian Wires Anuradha Acharya (2000)
Super Plus (Ortho Organizers) – between
Special plus and Premium
Premier (TP) – Comparable to Special
Premier Plus (TP)– Special Plus
Bowflex (TP) – Premium
230
High Tensile Australian Wires
Highest yield strength and ultimate tensile
strength as compared to the corresponding wires.
Higher range
Lesser coefficient of friction
Surface area seems to be rougher than that of
the other manufacturers’ wires.
Lowest stress relaxation.
231
High Tensile Australian Wires High and sharp yield points-freeing of
dislocations and effective shear stress to move these dislocations.
Flow stress dependent on- Temperature Density of dislocations in the material
Resulting structure-hard-high flow stress Plastic deformation absence of dislocation
locking-low YS Internal stress=applied stress x density of
dislocations
232
High Tensile Australian Wires
Fracture of wires and crack propagationDislocation locking
High tensile wires have high density of dislocations
and crystal defects
Pile up, and form a minute crack
Stress concentration
233
High Tensile Australian Wires
Small stress applied with the plier beaks
Crack propagation
Elastic energy is released
Propagation accelerates to the nearest grain boundary
234
High Tensile Australian WiresWays of preventing fracture
1.Bending the wire around the flat beak of the pliers.
-Introduces a moment about the thumb and wire gripping
point, which reduces the applied stress on the wire.
235
High Tensile Australian Wires
236
High Tensile Australian Wires
2. The wire should not be held tightly in the beaks
of the pliers.
Area of permanent deformation to be slightly
enlarged, Nicking and scarring avoided
3.Wilcock-Begg light wire pliers, preferably not
tungsten carbide tipped
237
High Tensile Australian Wires
238
High Tensile Australian Wires4. The edges rounded reduce the stress
concentration in the wire. –sandpaper & polish if sharp.
5.Ductile – brittle transition temperature slightly above room temperature. Wire should be warmed – pull though fingersSpools kept in oven at about 40o, so that the wire remains slightly warm.
239
Multistranded wires They are composed of specified numbers of thin
wire sections coiled around each other to provide round or rectangular cross section
The wires-twisted or braided
When twisted around a core wire-coaxial wire
240
Multistranded wires
Co-axial
Twisted wire
Multi braided
241
Multistranded wires
Individual diameter - 0.0165 or 0.0178
final diameter – 0.016" – 0.025“
On bending - individual strands slip over each
other , making bending easy.
Strands of .007 inch twisted into .017 inch-(3 wires)
stiffness comparable to a solid wire of .010 inch
242
Multistranded wires Stiffness – decreases as a function of the 4th
power Range – increases proportionately Strength – decreases as a function of the 3rd
power
Result - high elastic modulus wire behaving like a low stiffness wire
243
Multistranded wiresElastic properties of multistranded archwires depend on
–1.Material parameters – Modulus of elasticity
2.Geometric factors – moment of inertia & wire dimension
3.Twisting or braiding or coaxial
4.Dimensionless constants Number of strands coiled Helical spring shape factor Bending plane shape factor
244
Multistranded wiresHelical spring shape factor Coils resemble the shape of a helical spring. The helical spring shape factor is given as –
2sin α
2+ v cos α
α - helix angle and
v - Poisson’s ratio (lateral strain/axial strain)
Angle α can be seen in the following diagram :-
245
Multistranded wires
246
Multistranded wires
Schematic definition of the helix angle (a). If one revolution of a wire strand is unfurled and its base length [p(D-d)] and corresponding distance traversed along the original wire axis (S*) are determined, then a ratio of these two distances equals tan a. Everything else being equal, the greater p(D-d) or the less S* is, the more compliant a wire will be.
247
Multistranded wires Bending shape factor Complex property
number of strands orientation of the strands diameter of the strands and the entire wire helix angle etc.
Different for different types of multistranded wires
248
Multistranded wires Deflection of multi stranded wire
= KPL3
knEIK – load/support constantP – applied forceL – length of the beamK – helical spring shape factorn- no of strandsE – modulus of elasticityI – moment of inertia
249
Multistranded wiresKusy (AJO 1984) Triple stranded 0.0175” (3x0.008”) SS
GAC’s Wildcat
Compared the results to other wires commonly used by orthodontists- SS,NiTi & β-Ti
250
Multistranded wires The multistranded wire did not resemble the
0.018 wire in any way except for the size and & slot engagement Stiffness was comparable to 0.010 SS wire but
strength was 20% higher
0.016 NiTi-equal in stiffness, considerably stronger and 50% more activation
0.016 β-Ti –twice as stiff, comparable to 0.012 SS
251
Multistranded wires
252
Multistranded wires
253
Multistranded wiresIngram, Gipe and Smith
(AJO 86) Range independent of
wire size Range seems to increase
with increase in diameter
It varies only from 11.2-10.0-largest size having slightly greater range than smallest wire.
254
Multistranded wires Oltjen,Duncanson,Nanda,Currier (AO-1997) Wire stiffness can be altered by not only
changing the size or alloy composition but by varying the number of strands.
Increase in No. of strands stiffness
Unlike single stranded wires
stiffness varied as deflection varied.
Increase in No. of strands stiffnessUnlike single stranded wires
stiffness varied as deflection varied.
255
Multistranded wires
Rucker & Kusy (AO 2002)
Interaction between individual strands was
negligible.
Range and strength Triple stranded = Co-axial
(six stranded)
Stiffness Coaxial < Triple stranded
Range of small dimension single stranded SS
wire was similar.
256
Multistranded wires
257
Cobalt chromium
1950s the Elgin Watch
“The heart that never breaks”
Rocky Mountain Orthodontics - Elgiloy
CoCr alloys –belong to stellite alloys
superior resistance to corrosion (Cr oxide),
comparable to that of gold alloys exceeding
SS.
258
Cobalt chromium
Composition
Co-40%
Cr-20%
Ni-15% - strength & ductility
Fe-16%,traces of Molybdenum, Tungsten, Titanium-stable carbides –enhance hardenability and set resistance.
259
Cobalt chromium
Advantages over SS
1. Delivered in different degrees of hardening or tempers
2. High formability
3.Further hardened by heat treatment
4.Greater resistance to fatigue and distortion
5.Longer function as a resilient spring
260
Cobalt chromium
The alloy as received is highly formable, and can be easily shaped.
Heat treated-Considerable strength and resiliency Strength Formability
261
Cobalt chromium Ideal temperature- 482oC for 7 to 12 mins
Precipitation hardening
ultimate tensile strength of the alloy, without hampering the resilience.
After heat treatment, Elgiloy had elastic properties similar to steel
. Heating above 650oC
partial annealing, and softening of the wire
Optimum heat treatment dark straw color of the
wire or temperature indicating paste
262
Cobalt chromium1958-1961-4 tempers
Red – hard & resilient
Green – semi-resilient
Yellow – slightly less formable but ductile
Blue – soft & formable
263
Cobalt chromium Blue-bent easily -fingers or pliers Recommended –considerable bending, soldering
or welding required Yellow -bent with ease-more resilient -inc. in resiliency and spring
performance-heat Green –more resilient than yellow,can be shaped
to some extent-pliers Red- most resilient –high spring
qualities,minimal workingHeat treatment-inc. resilient but fractures easily.
264
Cobalt chromium
After heat treatment
Blue and yellow =normal steel wire
Green and red tempers =higher grade steel
E very similar –SS & blue elgiloy (10% inc in E)
Similar force delivery and joining characters
265
266
Cobalt chromium Comparable amount of Ni
Coefficient of friction higher than steel -recent
study-comparable to steel-zero torque brackets
are used.
The high modulus of elasticity of Co-Cr and SS-
Deliver twice the force of β-Ti and 4times NiTi
for equal amounts of activation.
267
Cobalt chromium Stannard et al (AJO 1986)
Co-Cr highest frictional resistance in wet and dry conditions.
Ingram Gipe and Smith (AJO 86) •Non heat treated
•Range < stainless steel of comparable sizes
•But after heat treatment, the range was considerably increased.
268
Cobalt chromium Kusy et al (AJO 2001) 16 mil (0.4mm or .016 inch) evaluated E values –identical -red –highest- YS & UTS -blue-most ductile
269
Cobalt chromium The elastic modulus did not vary appreciably
edgewise or ribbon-wise configurations. Round wires -
higher ductility than square or rectangular wires
270
Cobalt chromium
The averages of E,YS,UTS and ductility plotted
against specific cross-sec area.
Elastic properties (yield strength and ultimate
tensile strength and ductility) were quite similar
for different cross sectional areas and tempers.
This does not seem to agree with what is
expected of the wires.
271
Cobalt chromium
272
Cobalt chromium Conclusion- based on force-deactivation
characteristics- interchangeably – SS
Can choose different tempers and amounts of
formability
Inc the YS by heat treating
Fine in principle-but-lack of control of the
processing variables in the as received state.
273
To strive, to seek to find ,and not to yield - Lord Tennyson ( Ulyssess)
274
References Proffit – Contemporary orthodontics-3rd ed
Graber vanarsdall – orthodontics – current
principles and techniques-3rd ed
Phillips’ science of dental materials-Anusavice -
11th ed
Orthodontic materials-scientific and clinical
aspects-Brantly and Eliades
Edgewise orthodontics-R.C. Thurow-4th ed
Notes on dental materials-E.C.Combe-6th ed
275
References Frank and Nikolai. A comparative study of frictional
resistance between orthodontic brackets and archwires. AJO 80;78:593-609
Burstone. Variable modulus orthodontics. AJO 81; 80:1-16
Kusy and Dilley. Elastic property ratios of a triple stranded stainless steel archwire. AJO 84;86:177-188
Stannard, Gau, Hanna. Comparative friction of orthodontic wires under dry and wet conditions. AJO 86;89:485-491Ingram, Gipe, Smith. Comparative range of orthodontic wires AJO 1986;90:296-307
276
References Ingram, Gipe, Smith. Comparative range of
orthodontic wires AJO 1986;90:296-30
Arthur J Wilcock. JCO interviews. JCO 1988;22:484-489
Khier, Brantley, Fournelle,Structure and mechanical properties of as received and heat treated stainless steel orthodontic wires. AJO March 1988, 93, 3, 206-212
Twelftree, Cocks, Sims. Tensile properties of Orthodontic wires. AJO 89;72:682-687
Kapila & Sachdeva. Mechanical properties and clinical applications of orthodontic wires. AJO 89;96:100-109.
277
References Arthur Wilcock. Applied materials engineering for
orthodontic wires. Aust. Orthod J. 1989;11:22-29.
Julie Ann Staggers, Nicolas ,Clinical considerations in the use of retraction mechanics.. JCO June 1991
Klump, Duncanson, Nanda, Currier ,Elastic energy/ Stiffness ratios for selected orthodontic wires.. AJO 1994, 106, 6, 588-596
A study of the metallurgical properties of newly introduced high tensile wires in comparison to the high tensile Australian wires for various applications in orthodontic treatment. – Anuradha Acharya, MDS Dissertation September 2000.
278
References Kusy, Mims, whitley ,Mechanical characteristics
of various tempers of as received Co-Cr archwires.. AJO March 2001, 119, 3, 274-289
Eliades, Athanasios- In vivo aging of orthodontic alloys: implications for corrosion potential, nickel release, & biocompatibility –AO, 72,3,2002
Kusy.Orthodontic biomaterials: From the past to the present-AJO May 2002