2.dislocations - 1.pdf

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    Dislocations (Contd )

    Be IV/IV metal forming

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    Motion of

    Edge

    dislocation

    Conservative

    (Glide)

    Non-conservative

    (Climb)

    For edge dislocation: as bt they define a plane theslip plane

    Climb involves addition or subtraction of a row of atoms below the

    half plane

    +ve climb = climb up removal of a plane of atoms

    ve climb = climb down addition of a plane of atoms

    Motion of dislocations

    On the slip plane

    Motion of dislocation

    to the slip plane

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    Edge Dislocation Glide

    Shear stress

    Surface

    step

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    Edge Climb

    Positive climb

    Removal of a row of atoms

    Negative climb

    Addition of a row of atoms

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    S crew Dislocation The motion of a screw dislocation is also a result of shear

    stress

    Motion is perpendicular to direction of stress, rather than

    parallel (edge)

    However, the net plastic deformation of both edge and

    screw dislocations is the same

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    Ref: Bryan Baker

    chemed.chem.purdue.edu/genchem/ topicreview/bp/materials/defects3.html -

    [1]

    Screw dislocation

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    Fig A and B Two views of a model

    of a right handed screw dislocation.

    The blue line indicates approximate

    location of the dislocation line

    Ref: Journal of Matl. Education

    Fig A

    Fig B

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    PropertyType of Screw dislocation

    Positive negative

    Symbol

    t and b direction 0180

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    Screw dislocation cross-slip

    Slip plane 1

    Slip plane 2

    b

    The dislocation is shown cross-slipping from the blue plane to the green plane

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    The dislocation line ends on:

    The free surface of the crystal

    Internal surface or interface

    Closes on itself to form a loop

    Ends in a node

    A node is the intersection point of more than two

    dislocations

    The vectoral sum of the Burgers vectors of dislocations

    meeting at a

    node = 0

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    Geometric properties of dislocations

    Dislocation PropertyType of dislocation

    Edge Screw

    Relation between dislocation

    line (t) and b ||

    Slip direction || to b || to b

    Direction of dislocation line

    movement (t) relative to b||

    Process by which dislocation

    may leave slip planeclimb Cross-slip

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    Mixed Dislocations

    In many materials, dislocations are foundwhere the line direction and Burgersvector are neither only perpendicular nor

    only parallel and these dislocations arecalled mixed dislocations, consisting ofboth screw and edge character

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    Mixed dislocations

    b

    tb

    Pure EdgePure screw

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    The same model but viewed frombehind. The same letter correspondsto identical locations in three figures

    The schematic model

    Ref: Journal of Materials Education

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    Ref: http://www.tf.uni-kiel.de/matwis/amat/def_en/kap_5/backbone/r5_1_2.html

    Motion of a mixed dislocation

    [1]

    We are looking at the plane of the cut (sort of a semicircle centered in the lower left

    corner). Blue circles denote atoms just below, red circles atoms just above the cut. Up

    on the right the dislocation is a pure edge dislocation on the lower left it is pure screw.

    In between it is mixed. In the link this dislocation is shown moving in an

    animated illustration.

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    Energy of dislocations

    Dislocations have distortion energy associated with them

    E per unit length

    Edge Compressive and tensile stress fields

    Screw Shear strains

    Energy of dislocationElastic

    Non-elastic (Core)

    E

    ~E/10

    2

    2

    1GbE Energy of a dislocation / unit length

    G () shear modulus

    b |b|

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    2

    2

    1GbE Dislocations will have as small a b as possible

    Dislocations

    (in terms of lattice translation)

    Full

    Partial

    b Full lattice translation

    b Fraction of latticetranslation

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    Dissociationof dislocations

    Consider the reaction:

    2b b + bChange in energy:

    G(2b)2/2 2[G(b)2/2]

    G(b)2

    The reaction would be favorable

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    Density of dislocations in a crystal

    Total length of the dislocation line per unit

    volume of the crystal (m.m^-3) or m^-2

    Well annealed crystal has a dislocation density

    of ~ 10^8-10^10

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    Next class topics

    Dislocations in FCC Lattice

    Stacking faults

    Frank partial dislocations

    Dislocations in HCP lattice Dislocations in BCC cubic lattice

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    References

    Dieter, G.E.,Mechanical metallurgy, 1988, SI metric edition, McGraw-

    Hill

    W.D. Callister,Fundamental of materials science and engineering/ an

    interactive e. text., 2001, John Willey & Sons, Inc.

    Sanford, R.J.,Principles of fracture mechanics, 2003, Prentice Hall Tapany Udomphol, Dislocation theory, Suranaree University of

    Technology

    R. Prasad,Models of Dislocations for Classroom , Department of Applied

    Mechanics, Indian Institute of Technology, Hauz Khas, New Delhi