SGD Orthodontic: Material

SGD Orthodontic: Material

Hamzi, Zulkhairi, Azizul, Haziq, Aishah, Anis, Asmat, Masyitah

Lecture outline: material

Wire fracture

Mechanics of spring

Bauchinger effect

How does the material affect stability and the stiffness of the component?

Wire fracture

Small loads → the stress is below the elastic limit of the material, reversible elastic strain occurs that disappears completely when specimen is unloaded.

High stress A ductile material begins to undergo irreversible

plastic or permanent deformation A brittle material will fracture without any

significant permanent deformation

Stainless steel wire Orthodontic wire are generally

shaped by bending and the wire should possess sufficient ductility to resist fracture during this bending procedure.

The amount of residual ductility remaining in a wire depends in part on the ductility used up in its manufacture.

Mechanics of spring

Mechanics of springForce= (deflection)(radius4) @ F=dr4/l3

length3

• Force:– Single rooted: 25-40g– Excess force: delay movement, overload

anchorage & discomfort.

• Deflection:– Common spring activation: 3mm– Greater activation -> pt insert it incorrectly ->

unwanted movement– Smaller activation -> force applied decrease -

> wanted tooth movement (1-2mm/month)

BAUSCHINGER EFFECT

Named after German Engineer, Johann Bauschinger.

Applies to very small deformations.

May be stated as follows

“By applying a tensile or compressive load beyond the

elastic limit, the elastic limit for compression or for tension,

respectively, is reduced considerably, and the more the

load exceeds the elastic limit, the greater the reduction”

Tensi

le

stre

ss

Com

pre

ssi

ve s

tress

Tensile strainCompressive strain

In this graph, lets treat tensile stress and strain

as POSITIVE and compressive stress and

strain as NEGATIVE

0

If an annealed specimen is loaded from 0 to B beyond its elastic limit,

Tensi

le

stre

ss

Com

pre

ssi

ve s

tress

Tensile strainCompressive strain 0

B

designated by point A,

A

and unloaded,

Its condition is represent by C.

C

Note that the elastic limit of the material in tensile is given by SeT

SeT

Tensi

le

stre

ss

Com

pre

ssi

ve s

tress

Tensile strainCompressive strain 0

BA

C

SeT

If the same specimen is next loaded in compression, it follows the path CDE,

E

where D is the elastic limit point on the compression curve,so that the elastic limit in compression is now S’eC

D

S’eC

According to Bauschinger effect, S’eC < SeT

Tensi

le

stre

ss

Com

pre

ssi

ve s

tress

Tensile strainCompressive strain 0

BA

C

SeT

E

D

S’eC

If an annealed specimen instead of being loaded in tension and then in compression, as stated above, was directly loaded in compression,The elastic limit in compression of the annealed material should be SeC ,

SeC

F

And would be equal to magnitude to SeT .

Hence, SeC = SeT ,and S’eC < SeT and S’eC < SeC

Similar reasoning will happen if the annealed specimen was initially loaded in compression past the elastic limit, unloaded and loaded next in tension.

The resulting elastic limit in tension would be smaller than the elastic limit of annealed material in compression

Whereas Bauschinger effect was originally stated in terms of the elastic limit, the discussion of this effect in the literature has involve the use of terms elastic limit and yield strength interchangeably.

The reason for this anomaly lies in the elastic limit and the yield point being located very close to each other on the stress-strain curve.

The important thing is that one should not lose

sight of the fact that Bauschinger effect

applies to VERY small strains only.

How does the material affect stability and the stiffness of the component?

How does the material affect stability and the stiffness of the component?

The stability ratio of a spring in mechanical terms :

Stiffness in the direction of unwanted displacementStiffness in the intended direction of tooth movement

The spring must be guided so that its action is exerted only in the appropriate direction by: Place the spring in an undercut of the tooth so

that it does not slip occlusally during activation Use a guide to hold the spring in its position

during activation Bond an attachment to the tooth surface to

engage the spring

In Practice High stability spring eg. Finger spring

Straightforward to adjust/movement

Low stability spring eg. Buccal canine retractor Difficult to position precisely on the tooth

to be moved

The spring should be adjusted so that the point of application will give the desired direction of tooth movement.

Self supported spring These springs are made up of thicker

wire to avoid distortion by the patient

Supported spring These springs are made up of thinner

wire , a guidewire maybe provided. Alternatively, they maybe supported by an additional sleeve or ‘boxed’ of acrylic – to ensure adequate stability