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Lecture 9/2: Dislocations

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Lecture 9/2: Dislocations PHYS 430/603 material Laszlo Takacs UMBC Department of Physics Edge dislocation The crystal is partially cut, a new half-plane of atoms ... – PowerPoint PPT presentation

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Title: Lecture 9/2: Dislocations


1
Lecture 9/2 Dislocations
  • PHYS 430/603 material
  • Laszlo Takacs
  • UMBC Department of Physics

2
Edge dislocation
  • The crystal is partially cut, a new half-plane of
    atoms inserted coherently with the rest of the
    structure and the bonds between layers
    re-established.
  • The Burgers vector is perpendicular to the
    dislocation line.

3
Screw dislocation
  • The crystal is partially cut, one side shifted by
    a lattice parameter, then the bonds are
    re-established between the two sides.
  • The Burgers vector is parallel to the line of
    the dislocation.

4
  • Deformation can take place by both edge and screw
    dislocations

5
  • A mixed dislocation. The dislocation line can be
    bent, the Burgers vector remains the same along
    the dislocation.

6
Dislocation in a compound. There are both an
extra Mg and and extra O plane ending at the edge
of the dislocation.
7
Dislocation loop
  • Dislocations can begin and end at the surface of
    the crystal or at lattice defects. They can also
    form closed loops.
  • Notice that the Burgers vector is the same along
    the loop and its nature is edge or screw
    depending on the direction of the dislocation
    line.

8
Prismatic loop
  • The Burgers vector is perpendicular to the plane
    of the loop, thus it is edge dislocation all
    around. Equivalent to a partial extra lattice
    plane or a finite area of a lattice plane missing.

9
Twinning The crystal continues as its own mirror
image beginning with a lattice plane as the
mirror.After a few layers of atoms the
crystal is may return to the original orientation
via another twin boundary, but shifted. Twinning
can result in plastic deformation, just like
dislocation movement does.
10
Plastic deformation produced by twinning and by
slip
11
Twinning in an fcc latticeThe rectangles
represent 1 1 0 planes.
12
The (-1 1 0) plane in the cubic fcc unit cell and
a view of this plane showing the edge of the
close-packed planes.
13
Twinning in brass (optical micrograph)
14
Twinning in La aluminate(oblique illumination
optical image)
15
Stacking faults and twinning in Si (HRTEM)
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