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SOLID STATE CHEMISTRY. Books for study. Engineering Chemistry by Jain & Jain. Engineering Chemistry by Sunita Rattan. Engineering Chemistry by O. G. Palanna . Physical Chemistry by Puri , Sharma, Pathania . Inorganic text books in general. contents. Introduction Types of solids
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SOLID STATE CHEMISTRY
Books for study • Engineering Chemistry by Jain & Jain. • Engineering Chemistry by Sunita Rattan. • Engineering Chemistry by O. G. Palanna. • Physical Chemistry by Puri, Sharma, Pathania. • Inorganic text books in general.
contents • Introduction • Types of solids • Crystal Structures • Elements of Symmetry • Bragg’s equation • Allotropes of carbon: Diamond, graphite & Fullerene
INTRODUCTION Three phases of matter: Gas Liquid Solid
Solid molecules
What is solid? • Definite shape. • Definite volume. • Highly incompressible. • Rigid. • Constituent particles held closely by strong intermolecular forces. • Fixed position of constituents.
TYPES OF SOLIDS Two types (based upon atomic arrangement, binding energy, physical & chemical properties): • Crystalline • Amorphous
Crystalline solids • The building constituents arrange themselves in regular manner throughout the entire three dimensional network. • Existence of crystalline lattice. • A crystalline lattice is a solid figure which has a definite geometrical shape, with flat faces and sharp edges. • Incompressible orderly arranged units. • Definite sharp melting point. • Anisotropy. • Definite geometry. • Give x-ray diffraction bands. • Examples: NaCl, CsCl, etc.
AMORPHOUS SOLIDS • Derived from Greek word ‘Omorphe’ meaning shapeless. • No regular but haphazard arrangement of atoms or molecules. • Also considered as non-crystalline solids or super-cooled liquids. • No sharp m.p. • Isotropic. • No definite geometrical shape. • Do not give x-ray diffraction bands. • Examples: glass, rubber, plastics.
Types of crystal structures • Ionic crystals • Covalent crystals • Molecular crystals • Metallic crystals
Ionic crystals • Lattice points are occupied by positive and negative ions. • Hard and brittle solids. • High m.p. due to very strong electrostatic forces of attraction. • Poor conductors of electricity in solid state but good in molten state. • Packing of spheres depends upon: • presence of charged species present. • difference in the size of anions and cations. • Two types: • AB types. • AB2 types.
Covalent crystals • Lattice points are occupied by neutral atoms. • Atoms are held together by covalent bonds • Hard solids. • High m.p. • Poor conductors of electricity. • Two common examples: diamond & graphite.
Molecular crystals • Lattice points are occupied by neutral molecules. • The molecules are held together by vander Waal’s forces. • Very soft solids. • Low m.p. • Poor conductors of electricity.
Metallic crystals • Lattice points are occupied by positive metal ions surrounded by a sea of mobile e-. • Soft to very hard. • Metals have high tensile strength. • Good conductors of electricity. • Malleable and ductile. • Bonding electrons in metals remain delocalized over the entire crystal. • High density.
Laws of symmetry • Plane of symmetry • Centre of symmetry • Axis of symmetry.
Elements of symmetry in cubic crystal • Rectangular planes of symmetry: 3 • Diagonal planes of symmetry: 6 • Axes of four-fold symmetry: 3 • Axes of three-fold symmetry: 4 • Axes of two-fold symmetry: 6 • Centre of symmetry: 1 Total symmetry elements: 23
Planes of symmetry Rectangular plane of symmetry: 3 Diagonal plane of symmetry: 6
Axis of symmetry Four-fold axis of symmetry: 3 Three-fold axis of symmetry: 4
Axis & centre of symmetry Two-fold axis of symmetry: 6 Centre of symmetry: 1
Types of cubic crystals Four types: • Simple or primitive type • Body-centered • Face-centered • End face-centered
Body-centered cell (bcc) Simple or primitive type (sc)
Face-centered cell (fcc) End face-centered cell
Number of atoms per unit cell in a cubic lattice • Simple cubic cell: 1atom/unit cell of sc • Body-centered cell: 2 atoms/unit cell of bcc • Face-centered cell: 4 atoms/unit cell of fcc • End face-centered cell: 2 atoms/unit cell
Simple cube No of atoms per unit cell= 8 x 1/8 = 1
Simple cubic arrangement e.g.Polonium 52% of the space is occupied by the atoms
Body centered cubic lattice No of atoms present per unit cell = (8 x 1/8 ) + (1 x 1) = 2
Body centered cubic lattice e.g. CsCl, CsBr 68% of the space is occupied by the atoms
Face-centered cubic lattice No of atoms present per unit cell = (8 x 1/8 ) + (6 x 1/2) = 4
Face-centered cubic lattice e.g. NaCl, NaF, KBr, MgO 74% of the space is occupied by the atoms
End face-centered cubic lattice No of atoms present per unit cell = (8 x 1/8 ) + (2 x 1/2) = 2
Atomic radius of a cubic lattice • Simple cubic cell: r = a/2 • Face-centered cubic cell: r = a/√8 • Body-centered cubic cell: r = √3a/4 (where a → length of cube)
Radius ratio rule • Relation between the radius, co-ordination number and the structural arrangement of the molecule. Radius ratio = • Greater the radius ratio, larger the size of the cation and hence the co-ordination number.
BRAVAIS LATTICES • Unit cell parameters: • Lengths a, b & c. • Angles α, β & γ. • Total crystal lattices: 7 • Total Bravais lattices: 14
Structures of important ionic compounds • AB type: NaCl (rock salt) CsCl ZnS (zinc blende / sphalerite) • AB2 type: CaF2 (fluorite) TiO2 (rutile) SiO2 • A2B type: K2O (antifluorite)
Structure of NaCl (Rock salt) • FCC type. • Co-ordination number 6:6. • Calculation of no. of atoms of NaCl/unit cell: • Cl at corners: (8 1/8) = 1 • Cl at face centres (6 1/2) = 3 • Na at edge centres (12 1/4) = 3 • Na at body centre = 1 • Unit cell contents are 4(Na+Cl-) • i.e. per each unit cell, 4 NaCl • units will be present.