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Crystalline Arrangement of atoms

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Title: Crystalline Arrangement of atoms


1
Crystalline Arrangement of atoms
2
Chapter 4IMPERFECTIONS IN SOLIDS
  • The atomic arrangements in a crystalline lattice
    is almost always not perfect.
  • There are defects in the way atoms are arranged
    in the crystalline solids.
  • So we can say that in crystalline solids some
    Lattice Irregularities are always present.
  • These crystalline defects are not bad. Some are
    intentionally introduced to improve the material.

3
Types of Crystalline Defects
  • POINT DEFECTS are classified on the basis of
    their geometry and dimensionallity.
  • POINT DEFECTS
  • (Vacancies, self interstitials, impurity atoms)
  • LINE DEFECTS (one dimensional) (Dislocations)
  • INTERFACIAL DEFECTS (two dimensional) (Grain
    Boundaries)

4
VACANCYi.e. an atom missing from lattice position
5
IMPURITY ATOMS
6
POINT DEFECTS
7
Interstitials
8
Crystalline Defects
9
Vacancies
  • Vacancies are always present in the crystalline
    solids.
  • Vacancies are created during process of
    solidification or due to thermal agitations of
    lattice atoms.
  • At a given temperature there is always present an
    EQUILIBRIUM CONCENTRATION of VACANCIES.

10
EQUILIBRIUM CONCENTRATION OFVACANCIES
  • Equilibrium concentration of vacancies increase
    with temperature!

11
MEASURING ACTIVATION ENERGY
We can get Q from an experiment.
Measure this...
Replot it...
5
12
ESTIMATING VACANCY CONC.
3
Find the equil. of vacancies in 1 m of Cu
at 1000 oC.
Given
Answer
6
13
Impurities in Solids
  • Pure metal containing only one type of atoms
    Not Possible
  • Impurity atoms are always present.
  • These atoms exists as point defects.
  • In alloys, impurity atoms (alloying element
    atoms) are intentionally added.
  • An alloy is usually a solid solution of two or
    more types of atoms.
  • e.g. Fe C ? Steel

SOLVENT
SOLID SOLUTION
SOLUTE
14
TYPES OF SOLID SOLUTIONS
  • SOLID SOLUTION

SUBSTITUTIONAL SOLID SOLUTION Solute atoms
replace (substitute) the solvent atoms in the
solvent lattice
INTERSTITIAL SOLID SOLUTION Solute atoms occupy
the interstitial sites of the solvent lattice
15
Solid Solutions
16
Conditions For Substitutionl Solid Solubility
  • Four Conditions must be satisfied for obtaining
    appreciable (large) solubility of the
    substitutional solute in a given solvent lattice.
  • Atomic Size Factor The atomic size difference
    between the solute and solvent atoms must be less
    than ? 15.
  • Crystal Structure Crystal structure of both
    solute and solvent must be same.
  • Electronegative The electro negativity
    difference must be small. If this difference is
    large ionic compound will form instead of solid
    solution.
  • Valence Higher valance metals will dissolve
    easily than low valance metals.

17
Ni Cu Will they have large Solid
Solubility? Check! 4 conditions
Ni Cu Atomic Size 0.125
nm 0.128 nm Crystal structure FCC
FCC Electronegativity 1.8
1.9 Valence 2
1 Answer Yes they will
18
HOW about CU Zn
Zn Cu Atomic Size
0.133 nm 0.128 nm Crystal structure
HCP FCC Electronegativity 1.6
1.9 Valence 2
1 Answer No they wont
19
SPECIFICATION OF COMPOSITION
  • Two most common ways to specify the composition
    or concentration are
  • Weight or mass percent weight of a particular
    element relative to the total alloy weight.
  • Atom percent number of moles of an element in
    relation to the total moles of the elements in
    the alloy.
  • Weight
  • where m1 and m2 represent the weight or mass of
    elements.
  • Atom
  • where No. of moles (nm) (mass in grams) /
    Atomic weight

20
SPECIFICATION OF COMPOSITION (Contd.)
  • COMPOSITION CONVERSIONS
  • Weight to Atom
  • Atom to Weight

21
SPECIFICATION OF COMPOSITION (Contd.)
  • Weight to Kg/m3 ( mass of one component per
    unit volume of material)

22
Example 4.2
  • Derive Equation 4.6a
  • Solution
  • Total alloy mass,

Atom of element 1,
Simplifies to
23
DISLOCATIONS
  • Dislocations are LINEAR DEFECT and represent a
    line around which atoms in the crystalline
    lattice are misaligned.
  • Two Types of Dislocations
  • EDGE DISLOCATION
  • SCREW DISLOCATION
  • Also MIXED DISLOCATION

24
EDGE DISLOCATIONRepresented by a half atomic
plane the edge of which ends within the crystal
25
EDGE DISLOCATION
26
EDGE DISLOCATION
27
SCREW DISLOCATION
28
SCREW DISLOCATION
29
MIXED DISLOCATION
30
MIXED DISLOCATION
31
BURGERS VECTOR
  • Burgers Vector b represents the magnitude and
    direction of lattice distortion created by the
    dislocation.
  • FOR EDGE DISLOCATION b is perpendicular to
    dislocation line.
  • FOR SCREW DISLOCATION b is parallel to
    dislocation line.

32
BURGERS VECTOR
  • FOR METALLIC MATERIALS
  • The BURGERS VECTOR for a dislocation lies along a
    closed packed direction.
  • The Magnitude of the BURGERS VECTOR is equal to
    the interatomic or interpalnar spacing.

33
BURGERS VECTOR
34
DISLOCATIONS
35
4.5 Interfacial Defects
  • Interfacial defects are boundaries that have two
    dimensions and normally separate regions of the
    materials that have different crystal structures
    and/or crystallographic orientations.
  • These imperfections include external surfaces,
    grain boundaries, twin boundaries, stacking
    faults, and phase boundaries.
  • EXTERNAL SURFACES
  • One of the most obvious imperfection boundaries
    is the external surface
  • The crystal structure terminates
  • Surface atoms are not bonded to the maximum
    number of nearest neighbors ? higher energy state
    than interior atoms.
  • To reduce this energy, if possible materials tend
    to minimize surface area ? not possible for
    solids.

36
INTERFACIAL DEFECTS(GRAIN BOUNDARIES)
  • Boundary separating two small grains or crystals
    having different crystallographic orientations in
    polycrystalline materials.
  • Within the boundary region, which is probably
    just several atom distances wide, there is some
    atomic mismatch in a transition from the
    crystalline orientation of one grain to that of
    an adjacent one.
  • Various degrees of crystallographic misalignment
    between adjacent grains are possible ( Figure
    4.7).

37
4.5 Interfacial Defects (Contd.)
  • Tilt boundary
  • One simple small-angle grain boundary
  • Figure demonstrates how a tilt boundary having an
    angle of misorientation q results from an
    alignment of edge dislocations.
  • Twist boundary
  • When the angle of misorientation is parallel to
    the boundary
  • Due to an array of screw dislocations

38
  • The atoms are bonded less regularly along a grain
    boundary ? interfacial or grain boundary energy
    similar to surface energy.
  • Grain boundaries are more chemically reactive
    than the grains themselves as a consequence of
    this boundary energy.
  • Impurity atoms often preferentially segregate
    along these boundaries because of their higher
    energy state.
  • Because of less total boundary area, the total
    interfacial energy is lower in large or
    coarse-grained materials than in fine-grained
    ones.
  • Grains grow at elevated energy to reduce the
    total boundary energy
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