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CHE 333 Class 18

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CHE 333 Class 18. Fracture of Materials. Ductile or Brittle Failure. Following elastic deformation, two different processes can occur – plastic deformation leading to ductile failure or movement to brittle fracture with little or no plasticity. The stress strain curve is shown for ductile - PowerPoint PPT Presentation
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CHE 333 Class 18 Fracture of Materials
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Page 1: CHE 333 Class 18

CHE 333 Class 18

Fracture of Materials

Page 2: CHE 333 Class 18

Ductile or Brittle FailureFollowing elastic deformation, two different processes can occur – plastic deformationleading to ductile failure or movement tobrittle fracture with little or no plasticity.The stress strain curve is shown for ductilefailure. After the UTS the ductility is shownby the necking of the material. This wouldonly be for round bar.The stress strain curve for brittle materialsis indicated, which would be for glass andceramics.

Brittle FailureSvS stops here

Page 3: CHE 333 Class 18

Fracture ProcessesFor ductile materials which have plasticityonce the neck starts, a sequence of structural changes occurs as the metal proceeds to failure. Internally voids areinitiated . Both the true stress and strainare both still increasing. With furtherincrease in strain the voids becomelarger, as they become circular orellipsoidal in shape. The small ligamentsof metal between the voids eventuallytears and an internal crack is initiated.With further true stress and strain increasethe last areas to fail are those connecting the internal crack to the surface. A “shear lip”at 45o to the surface characterizes this regionleading to “cup and cone” fracture in rod.

Ligament of material Stretches between voids

Page 4: CHE 333 Class 18

Micro Failure Processes.In single phase materials, small voids appearat the cell walls as each dislocation effectivelycarries a vacancy with it. These voids then grow with further stressing

Page 5: CHE 333 Class 18

Micro Failure Processes

s

45o

Second Phase

In two phase material, several differentmicro processes can lead to void initiationgrowth and failure. If the second phase is either large or continuous,then a dislocation pile up in one phase will leadto a void formation. This will then grow in phase. The second phase will have strengthenedthe material but will also have eventuallyinitiated the failure process.Examples include pearlitic steels and other platelet structures such as those in titanium alloys Void from dislocation

pile up on slip plane

Page 6: CHE 333 Class 18

Micro Failure Example

Example of toughened material?

Page 7: CHE 333 Class 18

Micro Failure ProcessesWhen the second phase is small and non discontinuous, other processes inaddition to dislocation pile up and a void on the slip plane are possible. The controllingfactors are the strength of the second phaseparticle and interface between the secondphase and the matrix material.If the second phase is weaker or morebrittle than the matrix, then the second phaseparticle may crack.Age hardened aluminum alloys behave inthis manner

Page 8: CHE 333 Class 18

Micro Failure Example

Al 7079 Age Hardened alloy showing particle failure.

Page 9: CHE 333 Class 18

Micro Failure Examples

Page 10: CHE 333 Class 18

Macro View of Failure

Page 11: CHE 333 Class 18

Fracture Surface Features

Ductile failure in a titanium alloy which is two phase showing dimples from void formation

Page 12: CHE 333 Class 18

Final Failure in Shear Lip

Shear dimples in area of shear lip.

Page 13: CHE 333 Class 18

Brittle Failure Fracture Surface

A faceted type of fracture surface is often seen with a brittle failure as cracks are on a singlecrystal plane, no shear lip would be found..

Page 14: CHE 333 Class 18

Fracture Mechanics.Originally to explain why glass has low toughness where toughness is the ability to resist crack growth in a material. Simple energy balance used – energy applied is the stress and it is used up by creating fresh surface. Works well for brittle materials where no plastic deformation. For ductile materials energy absorbed is complicated by plastic deformation. Fracture mechanics relates the sizeof a defect in the material to the stress is can withstand before failure.

Kc = Ysc (pa)0.5

I II IIIMode

Page 15: CHE 333 Class 18

Plane Strain Fracture Toughness

Page 16: CHE 333 Class 18

Ductile to Brittle TransitionIn some materials, mainly steels, ductility can decrease very sharply with temperature, so a ductilematerials becomes brittle – know as the ductile brittle transition. The standard test is to use an impacttester – a pendulum type hammer and the energy absorbed in failure is measured by how far thehammer swings through after impact – the further the less energy.

Carbon content effect on DBTT for SteelsShear ratio to impact energy

Page 17: CHE 333 Class 18

Homework1. For a material with a single crystal yield strength of 300 MPa,

calculate the yield strength for a grain size of 50 micron and for a grain size of 2.5 microns. Assume k =1

2. Decide the crack initiation process in a tensile test for the following conditions:-

Matrix shear strength Matrix Normal Strength Interface Strength Particle Strengtha 25 60 35 55b 55 50 60 60c 55 60 35 45d 45 55 45 35Data units MPa.


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