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5/6/2002, Monday Summary: What we learned from this course?

5/6/2002, Monday Summary: What we learned from this course?

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Page 1: 5/6/2002, Monday Summary: What we learned from this course?

5/6/2002, Monday

Summary: What we learned from this course?

Page 2: 5/6/2002, Monday Summary: What we learned from this course?

Multi-scales Material Behaviors

nanoscale

microscale

millimeter scale

macroscale

Page 3: 5/6/2002, Monday Summary: What we learned from this course?

Nanometer Scales

Page 4: 5/6/2002, Monday Summary: What we learned from this course?

Burgers Vector

Magnitude of Burgers vector ~0.5nm

Bond breakage occurs consecutively rather than simultaneously.

Page 5: 5/6/2002, Monday Summary: What we learned from this course?

Hydrogen EmbrittlementHydrogen can diffuse rapidly through the lattice because of its small size.

Hydrogen tends to accumulate at the tension part of the dislocation, thus hinders the movement of dislocation.

Page 6: 5/6/2002, Monday Summary: What we learned from this course?

Environment Assisted Cracking

Page 7: 5/6/2002, Monday Summary: What we learned from this course?

Dislocation Emissions

Dislocation free zone size is about several nanometers

Page 8: 5/6/2002, Monday Summary: What we learned from this course?

Slip Systems

Resolved shear stress acting on the slip system

For FCC crystals, slip occurs most often on {111} planes and in <110> directions.

Page 9: 5/6/2002, Monday Summary: What we learned from this course?

Slip Plane

Monotonic loading gives rise to staircase morphology slip offsets.

Cyclic loading produces sharp peaks (extrusions) and troughs (intrusions).

Page 10: 5/6/2002, Monday Summary: What we learned from this course?

Micrometer Scales

Page 11: 5/6/2002, Monday Summary: What we learned from this course?

Strength of metal crystals as a function of dislocation density

The strength of a metal approaches extremely high levels when there are either no dislocations present or when the number of dislocations is extremely high.

Page 12: 5/6/2002, Monday Summary: What we learned from this course?

Dislocation DensityOn the surface of a thin metal film:

1011−1012 dislocations/cm2

0.03μm−0.01μmAverage inter-dislocation distance

Cold-worked metal:

104 −105 dislocations/cm2

100μm−32μmAverage inter-dislocation distance

Annealed metal:

Page 13: 5/6/2002, Monday Summary: What we learned from this course?

Inter- or Intra-granular Fracture

Intergranular-fracture Intragranular-fracture

For regular material, crack prefers to follow grain boundaries.

Page 14: 5/6/2002, Monday Summary: What we learned from this course?

Grain Boundary Strengthening

Grain boundaries serve as effective barriers to the movement of glide dislocations.

Page 15: 5/6/2002, Monday Summary: What we learned from this course?

Fatigue Striation

Page 16: 5/6/2002, Monday Summary: What we learned from this course?

Dislocation Creep

Dislocation creep involves the climbing of edge dislocations away from dislocation barriers.

Page 17: 5/6/2002, Monday Summary: What we learned from this course?

Millimeter Scales

Page 18: 5/6/2002, Monday Summary: What we learned from this course?

Crack Tip Plastic Zone

12π

K IC

σ ys

⎝ ⎜

⎠ ⎟

2

=1

2π72.5MPa m1340MPa

⎝ ⎜ ⎞

⎠ ⎟

2

~0.5mm

A typical steel

Page 19: 5/6/2002, Monday Summary: What we learned from this course?

Ductile Tensile Test

Page 20: 5/6/2002, Monday Summary: What we learned from this course?

Macro Scales

Page 21: 5/6/2002, Monday Summary: What we learned from this course?

Specimen Size for Fracture Test

Valid plane-strain fracture toughness conditions.

t and a≥2.5K IC

σys

⎝ ⎜

⎠ ⎟

2

t and a≥2.533MPa m490MPa

⎝ ⎜ ⎞

⎠ ⎟

2

=0.011m

Typical metal alloy:

Page 22: 5/6/2002, Monday Summary: What we learned from this course?

Simple Torsion Failure

The maximum normal stress failure theory is generally suitable for brittle materials.

The Tresca theory describes failure as taking place when the maximum shear stress exceeds the shear strength.

Page 23: 5/6/2002, Monday Summary: What we learned from this course?

Necking

With increasing load, a point is reached where the strain-hardening capacity of the material is exhausted and the further plastic deformation is localized in the necked region.