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    COURSE1

    MATERIALS SCIENCE

    Prof.Dr.Eng. Brndua GHIBAN

    1

    11/3/2014

    Materials. Classification

    Crystalline structure

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    CONTACTDATA:

    Prof.Dr.Eng. Brndua GHIBAN

    Departament METALLIC MATERIALS SCIENCE, PHYSICAL METALLURGY

    Consultation: HALL JK 114, THURSDAY 10-12

    11/3/2014

    2

    ACTIVITATY during SEMESTRY

    Final

    VERIFICA-

    TIONNote

    presence

    course

    5p

    Note access

    moodle

    platform

    10p

    Note

    laboratory

    presence

    0

    Note

    course

    manuscript

    5p

    Note

    Laboratory

    colloquium

    20p

    Note

    semestry

    evaluation

    20p40 points

    60 points

    STUDENTSEVALUATION

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    MATERIALS SCIENCE11/3/2014

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    is an interdisciplinary science at the border between

    mathematics -physics- chemistry- technique, dealingwith complex characterization of materials, the study

    of correlations, functional links between chemical

    composition, structure, properties, technology

    (design, machining, heat treatment) and technical

    use of the materials in order to establish laws, rules,criteria and models that will produce

    materials with

    predetermined properties (design materials),

    optimum selection of material for a rational and

    scientific substantiation of materials technology.

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    Materials define the development of human society

    11/3/2014

    4

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    EXAMPLEOFEVOLUTIONOFMATERIALS

    USEDINAEROGASTURBINES11/3/2014

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    Utilization of the materials

    depends on the properties,

    resources, cost price,

    workability and compatibilitywith the environment

    11/3/2014

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    MATERIALSCLASSIFICATION11/3/2014

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    11/3/2014

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    Organic Materials(carbon, hidrogen, oxigen, nitrogen)

    Inorganic MaterialsSimple

    Complexe (salts, oxides, halides)

    After chemicalcomposition

    After the state of

    aggregation

    MATERIALSCLASSIFICATION

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    Interatomic Bonds

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    Ionic Bond

    Typically, the metal has a 1,2,3 electron valence shell, and has a non-

    metallic 5, 6, 7, electrons in the valence shell. Steady state occurs through

    the sharing of electrons in the valence shell. Solid materials with Ionic

    bonds are :

    Hard materials

    Insulating substances,

    Transparent

    Brittle,

    High melting point

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    Covalent bonds

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    Covalent bonds occur between atoms of metals. They have four or more

    electrons to the valence layer. To form a new connection would require

    very high energy, either for extraction or for adding a new electron. Steady

    state occurs through the sharing of electrons in the valence shell. The

    solids that are covalent :

    Hard materials

    Good insulation

    Transparent

    Brittle, deformable

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    Metallic Bonds

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    The metallic bonds may appear between the metal atoms. These materials have three

    valence shell electrons. When an item has a 1,2,3 valence electrons per layer, the link

    established is very poor (e.g aluminum). The connection is formed between a lot of

    metal atoms, creating a "cloud of electrons" as a negative value and "frame", with a

    positive valence. Solid materials with metallic bonds are

    Bohr Model for metal

    Good electrical and thermal conductor

    Opaque

    Relatively ductile

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    VAN DER WAALS BONDS

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    Van der Waals bonds occur, with few exceptions, in all materials, but

    usually in plastics and polymers. These materials have very longmolecular chains, link atomic carbon and other atoms, hydrogen,

    nitrogen, oxygen, fluorine. Covalent bonds between the molecules are

    very strong and break under extreme conditions. Polymers can be

    classified as behavior heating :

    Thermoplastic polymers which

    soften or liquefy the hot

    Thermoset polymers with irreversiblereaction,

    Elastomers, with intermediate

    behavior.

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    1

    1/3/2014

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    MATERIALSCLASSIFICATION

    After the nature of the

    atomic bonds

    Metallic Materials

    Ceramic Materials

    Polymeric Materials

    Composite Materials

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    Metallic Materials

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    Very good thermal and electrical conductivity,

    Good deformability,

    Excellent ferromagnetic properties,

    Hardening capacity by applying heat treatments.

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    CERAMICMATERIALS

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    Good optical properties,

    Good thermal insulation,

    High melting temperature,

    Relatively inert in contact with molten metal,

    Piezoelectric behavior and the ability to convert into electricity.

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    POLYMERICMATERIALS 11/3/2014

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    Excellent ductility, with high capacity to form flexible films,

    Good electrical insulators,

    High resistance to corrosion in aqueous solutions

    (moisture resistance).

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    COMPOSITE

    MATERIALS1

    1/3/2014

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    Metallicmaterials

    Organic

    polymericmaterials

    Ceramic

    materials

    Composite

    Polymer matrix

    composites reinforced

    with metal

    Polymer matrix

    composites reinforced

    with ceramics

    Metal matrix

    composites reinforced

    with ceramics

    consist of a matrix of soft material (plastic, tenacious,

    ductile) which includes a hard and brittle material

    filling (in the form of blades, isolated fibers or

    particles).

    1 + 1 = 3

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    Materials Structure

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    Structure represents the internal architecture of a

    materials system by its parts of components.

    (Structure may be observed with naked eye or with glasseye)

    1. Macrostructure > 10-2 cm

    (Type and proportion of constituents observed by opticmicroscope)

    2. Microstructure, 10-810-1cm

    (Type of crystalline lattice observed by electron microscope)

    3. Crystalline structure, 10-810-1 cm

    (Type or chemical bond realized with valence electron of theatoms,observed by electron microscope)

    4. Atomic structure, 10-8cm

    (Number, cuantic numbers, electron distribution in layers,sublayers and orbitals observed by X-Rays)

    5. Electronic structure of the atoms, 10-8cm

    (Nature and number of nuclear particles observed by X-Rays)

    6. Nuclear structure, 10-13cm

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    SCALE OF MATERLS FOR NANOTECHNOLOGY

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    Length scale showing the nanometre in context. The length scale at the top ranges from 1m to 10 -10m, and

    illustrates the size of a football compared to a carbon 60 (C60) molecule, also known as a buckyball. For

    comparison the world is approximately one hundred million times larger than a football, which is in turn one

    hundred million times larger than a buckyball. The section from 10-7m (100nm) to 10-9m (1nm) is expanded below.

    The length scale of interest for nanoscience and nanotechnologies is from 100nm down to the atomic scale -approximately 0.2nm.

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    Crystalline structure of metals and alloys

    Crystalline structure and metallic bond represent the most important and decisive

    characteristic of the metallic materials, main physical-chemical properties, respectively

    mechanical characteristics being influenced by them.

    The lower portion of a space lattice which store the symmetry of the entirenetwork is unit cell. The unit cell is defined by its parameters, which are the vectors a,

    b andc (unit cell edge) and angle (between b and c), angle (between a and c) and

    angle (between a and b).

    Dimensional periodic repetition of the unit cell leads to obtaining of the network

    space, on whose regularity and symmetry properties relies almost all metals.

    Unit cell

    Orderly arrangement of atoms in a real crystal is its crystalline structure;

    symmetry of the crystal structure corresponds to the spatial network structure, but it

    must be noted that the atoms do not occupy those positions in complete immobility,

    but it vibrates (oscillates) around these positions, which leads to the real crystals with

    many imperfections.

    Space lattice

    1

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    Main elements which characterize the crystalline lattice

    1. Lattice parameter(a,b,c,)represents the distance

    between the centers of two

    atoms imaginary neighbors

    leading edge of the network

    2. ,,angles they makebetween them and edges of

    the unit cell with lattice

    parameters that determine the

    crystal system

    cwbvaur

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    3. DIRECTIONSOFHIGHDENSITYINATOMS

    Miller index - for directions are , ,

    - for family directions are [110] [111].

    Crystalline direction is defined through three index (u,v,w), whichrepresent the smallest entire coordinates of a vector which passthrough origin of the axes of a cell and is parallel with the crystallinedirection.

    those directions in which two or more atoms

    are tangent between them.1

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    Notation for - atomic planes are (111), (100), etc.

    - and of planes family {111}, {100}, etc.

    Crystallographic plane is defined by the indices h, k, l, which represents

    the inverse value of the full segments which form the intersection of theplane with the coordinate axes.

    1

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    4. Planes with high atomic density {111}

    those planes formed by atoms that have the

    most compact settlement (the most compact

    planes are those in which each atom is

    surrounded by six atoms willing hexagonal.

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    Represent the number of atoms which

    are at a minimum distance of a given

    atom. With the increasing amount of

    coordination number, atomic radius

    increases.

    C = 12 atoms

    C= 8 atoms

    C = 12 atoms

    5. Coordination n umber, C,

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    FCC

    BCC

    HC

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    6. Number of atoms A, which belong to a unit cell

    1

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    FCC

    BCC

    HC

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    7. Close-packed factor

    1

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    cellunitofvolum

    atomofvolumecellunitperatomsofnumber ))((

    %52100.3

    8

    3.

    3

    4

    r

    r

    %68100.

    3.

    3

    3

    4

    3.

    3

    4.2

    r

    r

    %74100.3

    .

    3

    )22(

    3.3

    4.4

    r

    r

    Simple Cube

    Body cubic centered

    Face cubic centered

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    The main crystalline systems

    Cristalline system Crystalline parameters Cristalline lattice

    Angles Distances

    Cube = = 90 a = b= c Cubicsimpl

    Cubiccu volum centrat (CVC)

    Cubiccufeecentrate (CFC)

    Tetragonal = = = 90 a= bc Tetragonalsimpl

    Tetragonalcu volum centrat (TVC)

    Orthorombic = = = 90 abc Simple Orthorombic

    Body centered orthorombic

    Base centered orthorombic

    Face centered orthorombic

    1

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    Cristalline system Crystalline parameters Cristalline lattice

    Angles Distances

    Rombohedric = = 90 a= b= c Simple Rombohedric

    Hexagonal = = 90

    = 120

    a= bc Simple Hexagonal

    Compact Hexagonal (HC)

    Monoclinic = = 90 abc Simple monoclinic

    Base centered monoclinic

    Triclinic 90 abc Simple triclinic

    1

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    BCC

    Unit cel ls for the mos t frequent metals:

    1

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    FCC

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    Unit cel ls for the mos t frequent metals:

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    HC11/3/2014

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    Unit cel ls for the mos t frequent metals: