epl206-01.pdf

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    L01-2011 1

    Arrangement of Carbon atoms can do wonders!

    Carbon Nano Tube (CNT)=Rolled Graphene

    BUCKMINISTER

    FULLERINE (C60)

    =Balled Graphene

    Superconducting

    DIAMOND

    High thermal

    conductivity,Insulating

    GRAPHENE

    Ultra high mobility

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    L01-2011 2

    GAS /LIQUID PHASE

    coolingAMORPHOUS, NANO XTALLINE

    POLY CRYSTALLINE

    AND/OR

    SINGLE CRYSTAL

    Window glass isamorphous

    Amorphous Solid

    Supercooled Liquid

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    L01-2011 3

    Crystalline and amorphous structures illustrated schematically in 2D

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    L01-2011 4

    CRYSTALLINE SOLIDS : PERFECT PERIODICITY OF

    ATOMIC STRUCTURE; BETTERUNDERSTOOD

    AMORPHOUS SOLIDS: LITTLE OR NO PERIODCITY

    SOLIDS - 2 VARIETIES

    CRYSTALLINE AMORPHOUS

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    L01-2011 5

    (a) A simple square lattice. The unit cell is a square with a side a.

    (b) Basis has two atoms.

    (c) Crystal = Lattice + Basis. The unit cell is a simple square with two atoms.

    (d) Placement of basis atoms in the crystal unit cell.

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    Oblique Net

    Square Net

    Centered Rect. NetRectangular Net

    Hexagonal Net

    2D Bravais Lattice (Surface Crystallography)

    http://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svghttp://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svghttp://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svghttp://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svghttp://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svghttp://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svghttp://upload.wikimedia.org/wikipedia/commons/e/ee/2d-bravais.svg
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    L01-2011 8

    BRAVAIS LATTICES (3-D)

    1. Every lattice point in a 3-D lattice can be described by vectort(defined above)

    2. 3-D space can be filled by repeating a smallest volume called

    unit cell, defined by vectors a, b, c called lattice parametersand the angles , ,

    3. The vectors a, b, c are primitive vectors if the parallelopiped

    defined by them does not include any more lattice point.

    integersare,,

    &vector,naltranslatio

    lkh

    t

    clbkaht

    =++=r

    r

    r

    rr

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    L01-2011 9

    6. There are 7 ways (obtained by giving different values to a, b,

    c, , , and ) which can produce unit cells of variousshapes, and therefore various kinds ofpoint lattice. Theseare referred to as CRYSTAL SYSTEMS (points at corners)

    7. As required by crystal symmetry, in 3D, there are 14 waysof arranging points in space lattices such that all the lattice

    points have exactly the same surroundings. These are 14

    BRAVAIS LATTICES (extra points at center of

    cell/face/base)

    4. The parallelopiped defined by

    primitive vectors is called

    primitive unit cell, and it hasthe smallest volume

    5. Volume = a1.(a2a3) OR a. (bc)

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    The seven crystal systems (unit cell geometries) and fourteen Bravais lattices.

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    L01-2011 11

    Contd..The 7 crystal systems (unit cell geometries) and 14 Bravais lattices.

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    L01-2011 12

    Q : Why not a new class Base-Centered Tetragonl (See Below) ?

    Ans : It does not generate a new on.

    It actually yields a Simple Tetragonal.

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    L01-2011 13

    Primitive Cell of a Face Centered Cell

    Its a Rhombohedral, its axis angle is 60.,each axis is (1/2)times the length of the axes of the cubic unit cell (Volume=1/4)

    It possess a cubic symmetry (it possess four 3-fold axes)

    It does not belong to the usual Rhombohedral (

    =

    = 90),

    which does not have cubic symmetry (as it only possesses

    one 3-fold axis)

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    L01-2011 14

    (a) Copper -

    face centered cubic (FCC). The atoms are positioned at

    well defined sites arranged periodically and there is a long range

    order in the crystal.

    (b) An FCC unit cell with closed packed spheres.

    (c) Reduced sphere representation of the unit cell. Examples: Ag,

    Al, Au, Ca, Cu,

    -Fe (>912 C), Ni, Pd, Pt, Rh.

    Packing of atoms: Face Cenetered Cubic

    Cu : Lattice Parameter a = 0.362 nm

    Atomic Radius r = 0.128 nm

    Face diagonal = 2 a = 4 r

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    L01-2011 15

    Examples: Alkali metals (Li, Na, K, Rb), Cr, Mo, W, Mn,

    -Fe (< 912 C), -Ti (> 882 C)

    Body diagonal = 3 a = 4 r

    Body Centered Cubic crystal (BCC) crystal structure.

    (a)

    A BCC unit cell with closely packed hard spheres

    representing the

    Fe atoms.(b)A reduced-sphere unit cell.

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    L01-2011 16

    %68)3/4(

    )3/4(2BCC,For

    cellunitinatomsofNumberVolumeCellUnit

    meAtomicVolu(APF)FractionPackingAtomic

    3

    3

    =

    =

    =

    r

    rAPF

    N

    N

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    L01-2011 17

    (a) The Hexagonal

    Close Packed (HCP)

    Structure. A collectionof many Zn atoms.

    Color difference

    distinguishes layers

    (stacks).

    (b) The stacking

    sequence of closely

    packed layers isABAB

    (c) A unit cell withreduced spheres

    (d) The smallest unit cell

    with reduced spheres.