4.1 me 340: materials & design chapter 4 frac ture

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4.1ME 340: Materials & Design

 

Chapter 4

FRACTURE

4.2ME 340: Materials & Design

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FAST FRACTURE

If more energy released than is absorbed crack advances

The FundamentalsFracture = separation of body into two or more pieces due to application of static stress

Tensile,CompressiveShear or torsional

Fails by fast fracture even though below yield stress

In a balloon energy is stored:1. Compressed gas

2. Elastic energy of Rubber membrane

Explosion of boilers, collapse of bridges

4.3ME 340: Materials & Design

Transgranular vs. intergranular fracture

Modes of fracture

DUCTILE

BRITTLE

4.4ME 340: Materials & Design

y

x

Stress trajectories

Professor Inglis (1913)

The birth of the term ‘’stress concentration’’

Large structures

4.5ME 340: Materials & Design

Griffith and his Energy criterion

Crack propagates when favorable, i.e. system reduces its total energy

Relaxed material behind crack =Elastic strain energy released

Crack having surface energy (s) a

a = edge crack or 1/2 central crack

4.6ME 340: Materials & Design

What about ductile materials

But for v. ductile materials p >>> s

Define the strain energy release rate Gc

(IRWIN 1950)

HenceToughness or Strain energy release rate(Energy absorbed per unit area of crack)

4.7ME 340: Materials & Design

cEGa Condition for fast fracture (for crack through center of a wide plate)

Comes up a lotHence give it symbol, K,Stress intensity factor

Fast fracture occurs when K=Kc

Modes of fracture

4.8ME 340: Materials & Design

Stress intensity factor

AND =

4.9ME 340: Materials & Design

Plastic zone

What about ductile materials consider y (i.e. y means direction not yield)

4.10ME 340: Materials & Design

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4.12ME 340: Materials & Design

4.13ME 340: Materials & Design

From: H.L.Ewalds, and R.J.H. Wanhill, Fracture Mechanics, 1991

4.14ME 340: Materials & Design

From: H.L.Ewalds, and R.J.H. Wanhill, Fracture Mechanics, 1991

4.15ME 340: Materials & Design

To be plane strain Plane strain fracture toughness

4.16ME 340: Materials & Design

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Design using fracture mechanics

Example: Compare the critical flaw sizes in the following metals subjected to tensile stress 1500MPa and K = 1.12 a. KIc (MPa.m1/2) Al 250Steel 50 Zirconia(ZrO2) 2 Toughened Zirconia 12

Critical flaw size (microns)70002800.4516

Where Y = 1.12. Substitute values

SOLUTION

4.18ME 340: Materials & Design

COMPRESSED AIR TANKS FOR A SUPERSONIC WIND TUNNELSupersonic wind tunnels in an Aerodynamic Lab, are powdered by a bank of large cylindrical pressure vessels. How can we design and check pressure vessels to make sure that they are safe?

t

pr

Hoop stress in the wall of a cylindrical pressure vessel containing gas at pressure p:Provided that the wall is thin (t<<r)

For general yielding y For Fast Fracture cKa

From, M. Ashby, Engineering Materials 1, 2nd edition, 1996

Vessels must be safe from plastic collapse or fail by fast fractureAlso must not fail by fatigue

4.19ME 340: Materials & Design

)1

(a

Kc

Yield before fracture

Fracture before Yield

Fatigue or stress corrosionIncreases crack size to critical value

4.20ME 340: Materials & Design

Easy to detect 10mm critical crack but not 1mm as for Al

4.21ME 340: Materials & Design

For critical crack size 2a

If critical flaw size is less than thickness fast fracture NO WARNING

4.22ME 340: Materials & Design

R-curve behavior

From: Brian Lawn, Fracture of brittle solids, 2nd edition, Cambridge university press) p.210, 1993

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