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    NAUMAN AHMAD

    Lecturer Chemistry

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    SOLID STATE

    CHEMISTRY 

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    contents

    • Introduction• Types of solids• Crystal Structures

    • Elements of Symmetry• Bragg’s equation• Allotropes of carbon: Diamond, grapite !

    "ullerene

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    INTRODUCTION

      Tree pases of matter: #as

      $iquid  Solid

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      #asmolecules

    5

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      $iquid

    molecules

    6

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      Solidmolecules

    7

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     What is solid?

    • Definite sape%•  Definite &olume%•  'igly incompressible%

    •  (igid%•  Constituent particles eld closely by strong

    intermolecular forces%

    •  "i)ed position of constituents%

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    TYPES OF SOLIDS

      T*o types +based upon atomic arrangement, binding energy, pysical ! cemical properties:

    -% Crystalline.% Amorpous

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    C!stalline solids

    •  Te building constituents arrange temsel&es in regularmanner trougout te entire tree dimensional net*or/%

    •  E)istence of crystalline lattice%•  A crystalline lattice is a solid figure *ic as a definite

    geometrical sape, *it flat faces and sarp edges%•  Incompressible orderly arranged units%•  Definite sarp melting point%•

     Anisotropy%•  Definite geometry%•  #i&e )0ray diffraction bands%•  E)amples: 1aCl, CsCl, etc%

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    AMORPHOUS SOLIDS

    • Deri&ed from #ree/ *ord 23morpe’ meaningsapeless% 

    •  1o regular but apa4ard arrangement of atoms ormolecules%

    •  Also considered as non0crystalline solids or super0cooled liquids%•  1o sarp m%p%•  Isotropic%•  1o definite geometrical sape%•  Do not gi&e )0ray diffraction bands%•  E)amples: glass, rubber, plastics%

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    T!"es o# c!stal st$ct$es

    •  Ionic crystals•  Co&alent crystals•  5olecular crystals

    •  5etallic crystals

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    Ionic c!stals•  $attice points are occupied by positi&e and negati&e ions%

    • 'ard and brittle solids%•  'ig m%p% due to &ery strong electrostatic forces of

    attraction%•  6oor conductors of electricity in solid state but good in

    molten state%•  6ac/ing of speres depends upon:

     presence of carged species present%

     difference in te si4e of anions and cations%• T*o types:  AB types%  AB. types%

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    Co%alent c!stals 

    •  $attice points are occupied by neutral atoms%•  Atoms are eld togeter by co&alent bonds• 'ard solids%

    •  'ig m%p%•  6oor conductors of electricity%•  T*o common e)amples: diamond ! grapite%

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    Molec$la c!stals

    • $attice points are occupied by neutral molecules%• Te molecules are eld togeter by &ander

    7aal’s forces% 

    • 8ery soft solids%•  $o* m%p%•  6oor conductors of electricity%

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    Metallic c!stals

    $attice points are occupied by positi&e metal ionssurrounded by a sea of mobile e0% • Soft to &ery ard%•  5etals a&e ig tensile strengt%

    •  #ood conductors of electricity%•  5alleable and ductile%•  Bonding electrons in metals remain delocali4ed o&er

    te entire crystal%•  'ig density%

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    La&s o# s!''et!

     

    • 6lane of symmetry•

    Centre of symmetry•  A)is of symmetry%

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    Ele'ents o# s!''et!in c$(ic c!stal

    •  (ectangular planes of symmetry: 9•  Diagonal planes of symmetry: •

     A)es of four0fold symmetry: 9•  A)es of tree0fold symmetry: ;•  A)es of t*o0fold symmetry:

    •  Centre of symmetry: -  Total symmetry elements: 23

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    Planes o# s!''et!

    (ectangular plane ofsymmetry: 9 Diagonal plane ofsymmetry:

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    A)is o# s!''et!

    "our0fold a)is ofsymmetry: 9 Tree0fold a)is ofsymmetry: ;

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    A)is * cente o# s!''et!

    T*o0fold a)is ofsymmetry: Centre of symmetry: -

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    T!"es o# c$(ic c!stals

    "our types:-% Simple or primiti&e type.% Body0centered

    9% "ace0centered;% End face0centered

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     Simple or primiti&e type +sc Body0centered cell +bcc

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    "ace0centered cell +fcc End face0centered cell

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    N$'(e o# ato's "e $nit cellin a c$(ic lattice

     • Simple cubic cell: -atom

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    Simple cube

    No of atoms per unit cell= 8 x 1/8=

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      No of atoms per unit cell= 8 x 1/8 =

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    Simple cubic arrangement

    e.g.Polonium52% of the space is occupied by the atoms

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    Body centered cubic lattice

    No of atoms present per unit cell

      = (8 x 1/8 ) + (1 x

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      No of atoms per unit cell= (8 x 1/8) +1= 2

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     Body centered cubic lattice

      e.g. CsCl, CsBr

    68% of the space is occupied by the atoms

    " d bi l i

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    "ace0centered cubic lattice

    No of atoms present per unit cell

    = (8 x 1/8 ) + (6 x

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    "ace0centered cubic lattice

    e.g. NaCl, NaF, KBr, MgO

    74% of the space is occupied by the atoms

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    End face0centered cubic lattice

    # ato's "esent "e $nit cell

    + - ) . - 1 2 ) . 2 +

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    Ato'ic adi$s o# a c$(ic lattice

    • Simple cubic cell:r = a

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    Radi$s atio $le

    • (elation bet*een te radius, co0ordinationnumber and te structural arrangement of temolecule%

      (adius ratio =

    • #reater te radius ratio, larger te si4e of te

    cation and ence te co0ordination number%

    E l # di3 t t l

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    E)a'"les o# di3eent c!stals!ste's

    S.No. System Example

    -% Cubic 1aCl, Cl, Ca"., Cu, nS, CsCl, Cu.3

    .% 3rtorombic BaS3;, 139, 5gSi39,  .S3;, CdS3;,AgBr 

    9% Tetragonal Sn3., Ti3., rSi3; ;% 5onoclinic CaS3;%.'.3, monoclinic S

    % Triclinic CuS3;%'.3, 1a'S3;, '9639

    % 'e)agonal 6bI., 5g, Cd, n, n3, B1, Si3., 'gS,CdS

    % (omboedral or Trigonal #rapite, ICl, Al.39, calcite +CaC39, As,Sb, Bi

    C bi l tti

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    Cubic lattice

    O th h bi l tti

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    Orthorhombic lattice

    T t l l tti

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    Tetragonal lattices

    li i l tti

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    onoclinic lattice

    T i li i l tti

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    Triclinic lattice

    !e agonal lattice

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    !exagonal lattice

    "hombohe#ral $Trigonal% lattice

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    "hombohe#ral $Trigonal% lattice

    St$ct$es o# i'"otant ionic

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    St$ct$es o# i'"otant ionicco'"o$nds

    -% AB type: 1aCl +roc/ salt  CsCl  nS +4inc blende < spalerite

    .% AB. type: Ca". +fluorite

    Ti3. +rutile

    Si3. 

    # l , 4

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    •  "CC type%

    •  Co0ordination number :%

    •  Calculation o& no. o& atoms o&

    NaCl'unitcell:Cl at corners: +? × -

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      St$ct$e o# sodi$' choide

    uic unit cell!mallest repeatale unit

    Structure o& CsCl

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    Structure o& CsCl

    •  bcc type%

    •  Co0ordination number ?:?%•  1umber of atoms

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    Structure o& (nS •

    fcc type%•  Co0ordination number

    ;:;%•  Calculation o& no. o&atoms'unit cell:

      Total S = ?)-

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    Structure o& Ca)2

    • fcc type%•  Co0ordination number: ?:;

     +? for cation, ; for anion

    G1ote: All te compounds of AB. type follo* te same pattern%

    "#

    Ca+ 

    Structure o& * O

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    Structure o& * 2O

    • fcc type%• Co0ordination number: ;:?

      ; for cation  ? for anion

    Na+

    $ #2

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    St$ct$e o# i'"otantco%alent co'"o$nds

    -% Diamond.% #rapite

    %iamon&

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    %iamon&

    'tructure of &iamon&

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    'tructure of &iamon&• fcc type%•

    Tetraedral• C0C bond lengt = -%9;A• (efracti&e inde) = .%;

    • 'ig dispersi&e po*er of ligt•  1on0conductor of electricity• 9d net*or/ 

    •  'ardest substance e&er /no*n%•  sed as abrasi&e%

    3#+ structure o& #iamon#

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    3#+ structure o& #iamon#

    raphite

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    raphite

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    Structure o& raphite

    3ne of te softest substances e&er /no*n%• .0d e)agonal layer structure• C0C bond lengt = -%;A• Inter layer distance = 9%;A• Sliding nature• sp. ybridisation *it one electron left o&er%• Specific gra&ity .%.• Electrical conductor • 5etallic lustre• sed as good lubricant%

    2#+ structure o& graphite

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    2#+ structure o& graphite