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What is slip?
Slip is lose one's footing and slide unintentionally for a
short distance… or to fall down.
SLIP SYSTEM
CONCEPT
Describes slips plane and slips direction
Explain the types of dislocation.
Understand the metallic crystal structure, FCC, BCC and HCP
Understand the crystallographic direction and planes, and able
to find the linear and planar density
Explain about slip systems, the way to determine it and its effect
on the metal characteritcs.
SLIP PLANES
β€’ A plane surface through a
crystal along which slip can
take place under some
conditions without apparently
disrupting the crystal.
β€’ Slip planes are the plane with
the highest density of atoms.
SLIP DIRECTION
Defintion:
β€’ The direction in which the dislocation moves, which is the direction of
the Burgers vector for edge dislocations.
Burgers vector:
β€’ the magnitude and direction of the lattice distortion resulting from a
dislocation in a crystal lattice.
β€’ Uni-directional.
Types of
Dislocations
Edge dislocation
Screw dislocation
EDGE DISLOCATIONS
β€’ One of the most common crystal
structure defects is edge
dislocations.
β€’ This type of dislocation occurs
when there are extra atoms
inserted into a plane in the crystal
lattice.
SCREW DISLOCATION
β€’ Defined as a dislocation in the lattice structure of a crystal in which the
atoms are arranged in a helical pattern that is normal to the direction of
the stress.
β€’ The motion of screw dislocation is also a result of shear stress.
β€’ Motion is perpendicular to the direction of stress.
CLOSE-PACKING OF EQUAL SPHERES
β€’ In geometry, close-packing of equal spheres is a dense arrangement of
congruent spheres in an infinite, regular arrangement or lattice.
β€’ We will discuss at the 3 most common metallic crystal structure.
Face-centred cubic crystal structure
(FCC)
Body-centred cubic crystal structure (BCC)
Hexagonal close-packed
crystal structure (HCP)
FCC
β€’ Face-Centred Cubic (FCC) is a crystal structure found for many metals
that has a unit cell of cubic geometry with atoms located at each of the
corners and the centres of all the cube faces.
above
in front
side
FCC
1. 1. Unit cell of cubic geometry, with atoms
located at each of the corners and centres of
all cube faces.
2. 2. The unit cell length a and atomic radius R is
related through
3. π‘Ž = 2𝑅 2
4. 3. Coordination number: 12
5. 4. examples: copper, aluminium, silver
6. Definition
7. Coordination number:
8. the number of attachments to the central atom
in a coordination complex
9. Unit cell:
10. Small repeated entities that is subdivided from
the structure of atomic arrangement.
(a) A hard sphere-unit cell
representation
(b) A reduced-sphere unit cell
representation
(c) An aggregate of many atoms
BCC
1. 1. Consist of a single atom at the centre of unit
cell, surrounded by 8 one quarter of atoms,
each shared among 8 unit cells.
2. 2. The unit cell length a and atomic radius R is
related through
3. π‘Ž =
4𝑅
3
4. 3. Coordination number: 8
5. 4. examples: Chromium, iron, tungsten
(a) A hard sphere-unit cell
representation
(b) A reduced-sphere unit cell
representation
(c) An aggregate of many atoms
HCP
1. 1. Consist of 6 atoms that form hexagons and
surround a single atoms at the centre of top
and bottom face. In between top and bottom
faces, there is a plane consist of 3 additional
atoms
2. 2. The short unit cell length, a and long unit
cell length, c is related through
3.
𝑐
π‘Ž
= 1.633 (ideal value)
4. 3. Coordination number: 12
5. 4. examples: cadmium, magnesium, titanium.
(a) A reduced-sphere unit cell
representation
(b) An aggregate of many atoms
CRYSTALLOGRAPHIC
DIRECTION
Defined as a line between two
points, or a vector.
Denoted as [uvw], u,v,w are
reduce projections along xyz axis.
Equivalent direction can be
grouped into family in < >
Example: [100],[010],[001] can be
grouped as <100>
CRYSTALLOGRAPHIC
DIRECTION FOR HCP
β€’ The 3 π‘Ž1, π‘Ž2 π‘Žπ‘›π‘‘ π‘Ž3 axes are
all contained in single plane
(basal plane), and 120 degree
to each other.
β€’ z-axis is perpendicular to
basal plane
CRYSTALLOGRAPHIC
PLANES
Specified by Miller
indices (hkl)
CRYSTALLOGRAPHIC PLANE
FOR HCP
Accomplished by Miller-Bravais system
The convention use (β„Žπ‘˜π‘–π‘™)
i is determined through
𝑖 = βˆ’ β„Ž + π‘˜
β„Ž = 1
π‘˜ = βˆ’1
𝑙 = 1
𝑖 = βˆ’ β„Ž + π‘˜
𝑖 = 0
β„Žπ‘˜π‘–π‘™ 𝑖𝑛𝑑𝑖𝑐𝑒𝑠 π‘Žπ‘Ÿπ‘’ (1101)
LINEAR AND PLANAR DENSITIES
β€’ Linear density (LD) is defined as
β€’ 𝐿𝐷 =
π‘›π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘Žπ‘‘π‘œπ‘šπ‘  π‘π‘’π‘›π‘‘π‘Ÿπ‘’π‘‘ π‘œπ‘› π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘› π‘£π‘’π‘π‘‘π‘œπ‘Ÿ
π‘™π‘’π‘›π‘”π‘‘β„Ž π‘œπ‘“ π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘› π‘£π‘’π‘π‘‘π‘œπ‘Ÿ
β€’ 𝐿𝐷110 =
2 π‘Žπ‘‘π‘œπ‘šπ‘ 
4𝑅
=
1
2𝑅
β€’ Planar density (PD) is defined as
β€’ 𝑃𝐷 =
π‘›π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘Žπ‘‘π‘œπ‘šπ‘  π‘π‘’π‘›π‘‘π‘Ÿπ‘’π‘‘ π‘œπ‘› π‘π‘™π‘Žπ‘›π‘’
π‘Žπ‘Ÿπ‘’π‘Ž π‘œπ‘“ π‘π‘™π‘Žπ‘›
β€’ 𝑃𝐷 = (2 π‘Žπ‘‘π‘œπ‘šπ‘ )/8𝑅2
2
SLIP SYSTEM
β€’ Dislocation does not move at the same degree of ease on all
crystallographic planes and direction of atoms
β€’ The preferred plane with specified directions along which dislocation
motion occurs is called slip plane.
β€’ The direction of the dislocation movement on slip plane is known as slip
direction.
β€’ The combination of slip plan and slip direction is know as slip system.
β€’ For a particular crystal structure:
β€’ Slip plane: plane with greatest planar density
β€’ Slip direction: direction with the highest linear density in slip plane.
TYPES OF SLIP SYSTEMS
β€’ Have 12 slip systems
β€’ Includes metals like copper, aluminium, nickel and silver
Face-centred cubic
(FCC) slip
β€’ Have 12 to 24 slip systems
β€’ Includes a wide range of metal alloys
Body-centred cubic
(BCC) slip
β€’ Presents much less slip system than BCC and FCC crystal structures
β€’ Includes metals like titanium, magnesium and zinc
Hexagonal close
packed (HCP) slip
FACE-CENTRED CUBIC (FCC) SLIP SYSTEM
Definition:
β€’ Slip in face centered cubic (fcc) crystals occurs along the close packed
plane.
Lattice configuration of the close packed slip plane in an
FCC material. The arrow represents the Burgers vector in
this dislocation glide system.
FCC SLIP SYSTEM
β€’ The slip plane belongs to the {111}
family
β€’ Slips occur at <110>-type direction,
within {111} planes
β€’ There are several slips direction for a
slip plane, forming different possible
combination of slip system
β€’ For FCC, 4 unique {111} planes and 3
independent <110> directions, results
in 12 slips system.
A TABLE OF SLIPS SYSTEM FOR FCC, BCC
AND HCP METALS
FCC & BCC
β€’ More slip systems, at lease 12
β€’ Metal is ductile
β€’ Plastic deformation is possible along
various systems.
β€’ Less slip systems
β€’ Metal is brittle
β€’ Plastic deformation is less possible in
various systems.
HCP
COMPARISON OF NUMBER OF SLIPS
SYSTEM OF FCC,BCC WITH HCP
BURGERS VECTOR
β€’ Defined as the magnitude of direction of lattice distortion associated
with a dislocation
β€’ In slip system:
β€’ Burgers vector direction is correspond to the dislocation slip direction
β€’ Magnitude of Burgers vector is equal to the unit slip distance.
β€’ Expressing Burgers vector, b in terms of unit cell length:
β€’ 𝒃 < 𝐹𝐢𝐢 > =
π‘Ž
2
< 110 >
β€’ 𝒃 < 𝐡𝐢𝐢 > =
π‘Ž
2
< 111 >
β€’ 𝒃 < 𝐻𝐢𝑃 > =
π‘Ž
3
< 11 𝟐0 >

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Presentation Slip System

  • 1. What is slip? Slip is lose one's footing and slide unintentionally for a short distance… or to fall down. SLIP SYSTEM
  • 2. CONCEPT Describes slips plane and slips direction Explain the types of dislocation. Understand the metallic crystal structure, FCC, BCC and HCP Understand the crystallographic direction and planes, and able to find the linear and planar density Explain about slip systems, the way to determine it and its effect on the metal characteritcs.
  • 3. SLIP PLANES β€’ A plane surface through a crystal along which slip can take place under some conditions without apparently disrupting the crystal. β€’ Slip planes are the plane with the highest density of atoms.
  • 4. SLIP DIRECTION Defintion: β€’ The direction in which the dislocation moves, which is the direction of the Burgers vector for edge dislocations. Burgers vector: β€’ the magnitude and direction of the lattice distortion resulting from a dislocation in a crystal lattice. β€’ Uni-directional.
  • 6. EDGE DISLOCATIONS β€’ One of the most common crystal structure defects is edge dislocations. β€’ This type of dislocation occurs when there are extra atoms inserted into a plane in the crystal lattice.
  • 7. SCREW DISLOCATION β€’ Defined as a dislocation in the lattice structure of a crystal in which the atoms are arranged in a helical pattern that is normal to the direction of the stress. β€’ The motion of screw dislocation is also a result of shear stress. β€’ Motion is perpendicular to the direction of stress.
  • 8. CLOSE-PACKING OF EQUAL SPHERES β€’ In geometry, close-packing of equal spheres is a dense arrangement of congruent spheres in an infinite, regular arrangement or lattice. β€’ We will discuss at the 3 most common metallic crystal structure. Face-centred cubic crystal structure (FCC) Body-centred cubic crystal structure (BCC) Hexagonal close-packed crystal structure (HCP)
  • 9. FCC β€’ Face-Centred Cubic (FCC) is a crystal structure found for many metals that has a unit cell of cubic geometry with atoms located at each of the corners and the centres of all the cube faces. above in front side
  • 10. FCC 1. 1. Unit cell of cubic geometry, with atoms located at each of the corners and centres of all cube faces. 2. 2. The unit cell length a and atomic radius R is related through 3. π‘Ž = 2𝑅 2 4. 3. Coordination number: 12 5. 4. examples: copper, aluminium, silver 6. Definition 7. Coordination number: 8. the number of attachments to the central atom in a coordination complex 9. Unit cell: 10. Small repeated entities that is subdivided from the structure of atomic arrangement. (a) A hard sphere-unit cell representation (b) A reduced-sphere unit cell representation (c) An aggregate of many atoms
  • 11. BCC 1. 1. Consist of a single atom at the centre of unit cell, surrounded by 8 one quarter of atoms, each shared among 8 unit cells. 2. 2. The unit cell length a and atomic radius R is related through 3. π‘Ž = 4𝑅 3 4. 3. Coordination number: 8 5. 4. examples: Chromium, iron, tungsten (a) A hard sphere-unit cell representation (b) A reduced-sphere unit cell representation (c) An aggregate of many atoms
  • 12. HCP 1. 1. Consist of 6 atoms that form hexagons and surround a single atoms at the centre of top and bottom face. In between top and bottom faces, there is a plane consist of 3 additional atoms 2. 2. The short unit cell length, a and long unit cell length, c is related through 3. 𝑐 π‘Ž = 1.633 (ideal value) 4. 3. Coordination number: 12 5. 4. examples: cadmium, magnesium, titanium. (a) A reduced-sphere unit cell representation (b) An aggregate of many atoms
  • 13. CRYSTALLOGRAPHIC DIRECTION Defined as a line between two points, or a vector. Denoted as [uvw], u,v,w are reduce projections along xyz axis. Equivalent direction can be grouped into family in < > Example: [100],[010],[001] can be grouped as <100>
  • 14. CRYSTALLOGRAPHIC DIRECTION FOR HCP β€’ The 3 π‘Ž1, π‘Ž2 π‘Žπ‘›π‘‘ π‘Ž3 axes are all contained in single plane (basal plane), and 120 degree to each other. β€’ z-axis is perpendicular to basal plane
  • 16. CRYSTALLOGRAPHIC PLANE FOR HCP Accomplished by Miller-Bravais system The convention use (β„Žπ‘˜π‘–π‘™) i is determined through 𝑖 = βˆ’ β„Ž + π‘˜ β„Ž = 1 π‘˜ = βˆ’1 𝑙 = 1 𝑖 = βˆ’ β„Ž + π‘˜ 𝑖 = 0 β„Žπ‘˜π‘–π‘™ 𝑖𝑛𝑑𝑖𝑐𝑒𝑠 π‘Žπ‘Ÿπ‘’ (1101)
  • 17. LINEAR AND PLANAR DENSITIES β€’ Linear density (LD) is defined as β€’ 𝐿𝐷 = π‘›π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘Žπ‘‘π‘œπ‘šπ‘  π‘π‘’π‘›π‘‘π‘Ÿπ‘’π‘‘ π‘œπ‘› π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘› π‘£π‘’π‘π‘‘π‘œπ‘Ÿ π‘™π‘’π‘›π‘”π‘‘β„Ž π‘œπ‘“ π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘› π‘£π‘’π‘π‘‘π‘œπ‘Ÿ β€’ 𝐿𝐷110 = 2 π‘Žπ‘‘π‘œπ‘šπ‘  4𝑅 = 1 2𝑅 β€’ Planar density (PD) is defined as β€’ 𝑃𝐷 = π‘›π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘Žπ‘‘π‘œπ‘šπ‘  π‘π‘’π‘›π‘‘π‘Ÿπ‘’π‘‘ π‘œπ‘› π‘π‘™π‘Žπ‘›π‘’ π‘Žπ‘Ÿπ‘’π‘Ž π‘œπ‘“ π‘π‘™π‘Žπ‘› β€’ 𝑃𝐷 = (2 π‘Žπ‘‘π‘œπ‘šπ‘ )/8𝑅2 2
  • 18. SLIP SYSTEM β€’ Dislocation does not move at the same degree of ease on all crystallographic planes and direction of atoms β€’ The preferred plane with specified directions along which dislocation motion occurs is called slip plane. β€’ The direction of the dislocation movement on slip plane is known as slip direction. β€’ The combination of slip plan and slip direction is know as slip system. β€’ For a particular crystal structure: β€’ Slip plane: plane with greatest planar density β€’ Slip direction: direction with the highest linear density in slip plane.
  • 19. TYPES OF SLIP SYSTEMS β€’ Have 12 slip systems β€’ Includes metals like copper, aluminium, nickel and silver Face-centred cubic (FCC) slip β€’ Have 12 to 24 slip systems β€’ Includes a wide range of metal alloys Body-centred cubic (BCC) slip β€’ Presents much less slip system than BCC and FCC crystal structures β€’ Includes metals like titanium, magnesium and zinc Hexagonal close packed (HCP) slip
  • 20. FACE-CENTRED CUBIC (FCC) SLIP SYSTEM Definition: β€’ Slip in face centered cubic (fcc) crystals occurs along the close packed plane. Lattice configuration of the close packed slip plane in an FCC material. The arrow represents the Burgers vector in this dislocation glide system.
  • 21. FCC SLIP SYSTEM β€’ The slip plane belongs to the {111} family β€’ Slips occur at <110>-type direction, within {111} planes β€’ There are several slips direction for a slip plane, forming different possible combination of slip system β€’ For FCC, 4 unique {111} planes and 3 independent <110> directions, results in 12 slips system.
  • 22. A TABLE OF SLIPS SYSTEM FOR FCC, BCC AND HCP METALS
  • 23. FCC & BCC β€’ More slip systems, at lease 12 β€’ Metal is ductile β€’ Plastic deformation is possible along various systems. β€’ Less slip systems β€’ Metal is brittle β€’ Plastic deformation is less possible in various systems. HCP COMPARISON OF NUMBER OF SLIPS SYSTEM OF FCC,BCC WITH HCP
  • 24. BURGERS VECTOR β€’ Defined as the magnitude of direction of lattice distortion associated with a dislocation β€’ In slip system: β€’ Burgers vector direction is correspond to the dislocation slip direction β€’ Magnitude of Burgers vector is equal to the unit slip distance. β€’ Expressing Burgers vector, b in terms of unit cell length: β€’ 𝒃 < 𝐹𝐢𝐢 > = π‘Ž 2 < 110 > β€’ 𝒃 < 𝐡𝐢𝐢 > = π‘Ž 2 < 111 > β€’ 𝒃 < 𝐻𝐢𝑃 > = π‘Ž 3 < 11 𝟐0 >