Section 14: Mechanics of Materials Material Properties 14-1 - - PowerPoint PPT Presentation

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Section 14: Mechanics of Materials Material Properties 14-1 - - PowerPoint PPT Presentation

Section 14: Mechanics of Materials Material Properties 14-1 Stress &Strain Stress &Strain Stress-strain ratio: stiffness or compliance of the material A E = / / E = Linear material Hooke law:


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SLIDE 1

Section 14: Mechanics of Materials – Material Properties

14-1

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SLIDE 2

Stress &Strain Stress &Strain

  • Stress-strain ratio:

stiffness or compliance of the material

E = / ε

A

– E = σ/ ε

  • Linear material

– Hooke’ law: σ = E· ε

σ

  • Biological material non-

linear due to its tissue fluid component B fluid component (viscoelastic properties) ε

14-2 From: Noffal

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SLIDE 3
  • 1. General mechanics principle
  • The underlying mechanics principle for metal forming is

the stress-strain relationship; see Figure 1.

14-3 From: Zhang

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SLIDE 4

Stress vs Strain Stress vs. Strain

Strain: Stress:

δ ε =

F = σ

S S

l ε =

A = σ

Hooke’s law:

ε σ E =

Where: E = Modulus of Elasticity

σ = stress

ε = strain

F th bik f k t i l E 29 0 106 i

14-4 From: Gateway Engineering Education Coalition

For the bike fork material E = 29.0 x 106 psi.

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SLIDE 5

Strain Strain

  • Change in shape or

Change in shape or deformation (ε)

  • Absolute strain
  • Relative strain

– ΔL/Lo

14-5 From: Noffal

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SLIDE 6

Poisson's ratio :

For a homogeneous isotropic material

d d Δ + d

F F

l

x

  • normal strain :

l x = ε

l

x

normal strain : l t l t i

d Δ

l

  • lateral strain :
  • Poisson's ratio :

d

L =

ε

ε ε ν /

L

− ≡

14-6 From: Ong

  • value of ν :

0.2 - 0.5

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SLIDE 7

Definition of Strain and Poisson’s R i Ratio:

l l l Δ − ) (

  • i

l l l l l Δ = = ) ( ε

  • This is the definition of

engineering strain.

  • In this definition, l0 is

the initial length of the specimen; l is the ν=εx/εz specimen; li is the instantaneous length of the specimen; Δl is the difference between the

14-7 From: Wei

two.

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SLIDE 8

Viscoelasticity Viscoelasticity

  • Pure elastic material

– strain energy returned – no energy loss

Vi l ti ti

  • Viscoelastic tissues

– lose energy due to heat – energy is not returned

σ Elastic

immediately – Resilient – Dampened

σ Non

p

  • Hysteresis: area

representing energy lost

14-8 From: Noffal

ε

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SLIDE 9

Viscoelasticity Viscoelasticity

  • Creep response

Creep response

  • Stress-relaxation

response

ε

creep

p

  • Effects of strain-rate
  • n stress relaxation

σ

14-9 From: Noffal

Time