Metal Bonding 2

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    Solids: Conductors, Insulators

    and Semiconductors Conductors: mostly metals

    Insulators: mostly nonmetal materials

    well study allotropes of carbon and study

    their properties

    Semiconductors: metalloids

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    Solids: Conductors, Insulators

    and Semiconductors

    Conductor Insulator Semiconductor

    Valence Band

    in red

    Conduction Band: white

    Band gapNo gap

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    Bonding in Metals

    The electron-sea model is a simple

    depiction of a metal as an array of positive

    ions surrounded by delocalized valenceelectrons. Metals are good conductors of electricity because

    of the mobility of these delocalized valence

    electrons.

    A metal also conducts heat well because the mobile

    electrons can carry additional kinetic energy.

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    Bonding in Metals

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    Bonding in Metals

    Molecular orbital theory gives a more

    detailed picture of the bonding in metals.

    Because the energy levels in a metal

    crowd together into bands, this picture

    of metal bonding is called band theory.

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    Bonding in Metals

    Molecular orbital theory gives a more

    detailed picture of the bonding in metals.

    According to band theory, the electrons in a

    crystal become free to move when they are

    excited to the unoccupied orbitals of a

    band.

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    Bonding in Metals

    Molecular orbital theory gives a more

    detailed picture of the bonding in metals.

    In a metal, this requires little energy

    since the unoccupied orbitals lie just above

    the occupied orbitals of highest energy.

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    Bonding In

    Metals:

    Lithium

    according toMolecular

    OrbitalTheory

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    Sodium According to Band Theory

    Conduction band:

    empty 3s antibonding

    Valence band:

    full 3s bonding

    No gap

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    Magnesium

    3s bonding and antibonding should be full

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    Magnesium

    Conduction band:

    empty

    Valence band:

    full

    No gap: conductor

    Conductor

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    Solids: Conductors, Insulators

    and Semiconductors

    Conductor Insulator Semiconductor

    Valence Band

    in red

    Conduction Band: white

    Band gapNo gap

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    Allotropes of Carbon

    Diamond: high thermal conductivity,extremely strong, insulator

    Graphite: high thermal conductivity,conductor

    electrodes for electrolysis and batteries;essentially pencil lead

    Fullerenes: discovered in 1986, amazingpossibilities

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    Diamond

    Diamond has a three-dimensional networkstructure in which each carbon is singly-bondedto four others with sp3 hybridization.

    Diamond is a covalent network solid

    each carbon covalently bonded to 4 others.

    Diamonds are the hardest substance known.

    must break carbon-carbon bonds Diamonds have a melting point of 3550C.

    must break carbon-carbon bonds

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    Structure of Diamond

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    Diamond

    Diamond has a three-dimensional network structure inwhich each carbon is singly-bonded to four others withsp3 hybridization.

    Why do diamonds conduct heat? Metals conduct heat because the the mobile electrons can

    carry additional kinetic energy.

    Diamonds are insulators and have no mobile electrons.

    Diamonds conduct heat through high frequency (= high

    energy) vibrations that transmit over long distances Diamonds conduct heat 4 times better than copper!

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    Graphite

    Graphite has a layered structure, in which

    the carbon atoms in each layer bond to three

    other carbons with sp2 orbitals.

    Graphites primary use is in the

    manufacture of electrodes for electrolysis

    and batteries. Of the covalent network solids, only graphiteconducts electricity.

    This is due to the delocalization of the resonantelectrons in graphites sp

    2

    hybridization.

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    Structure of Graphite

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    Fullerenes

    The fullerenes are a family of molecules with a

    closed cage of carbon atoms arranged in

    pentagons and hexagons. Each carbon is sp2

    hybridized.

    The most symmetrical member is

    buckminsterfullerene, C60.

    Buckminsterfullerenes show potential forapplications in superconductivity and catalytic

    activity.

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    Figure 13.25:A frame

    model

    of C60.By permission of Dr.

    Richard Smalley, Rice

    University

    Buckminsterfullerene

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    Solids: Conductors, Insulators

    and Semiconductors

    Conductor Insulator

    Band gap = 5.5 eV

    530 kJ/molNo gap

    GraphiteDiamond

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    Solids: Conductors, Insulators

    and Semiconductors

    Semiconductor

    Band gap

    Band Gap for Semiconductors

    Diamond 5.5 eV

    Si 1.1 eV

    Ge 0.67 eV

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    Semiconductors

    Metalloids: semiconducting elements low electrical conductivity at room temperature

    Electrical conductivity increases with temp.

    Gap between valence and conduction band

    is intermediate in size

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    Semiconductors

    Semiconducting elements form the basis

    of solid state electronic devices.

    A striking property of these elements is that their

    conductivities increase markedly when they aredoped with small quantities of other elements.

    Metalloids (such as silicon or germanium) aresemiconducting elements whose electrical

    conductivity increases as temperature increases.

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    Semiconductors

    Semiconducting elements form the basis

    of solid state electronic devices.

    When silicon is doped with phosphorus, itbecomes an n-type semiconductor, in

    which electric current is carried by

    electrons.

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    Semiconductors

    Semiconducting elements form the basis

    of solid state electronic devices.

    When silicon is doped with boron, itbecomes a p-type semiconductor, in

    which an electrical current is carried by

    positively charged holes

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    Semiconductors

    Semiconducting elements form the basis

    of solid state electronic devices.

    Joining a p-type semiconductor to an n-type semiconductor produces a p-n

    junction, which can function as a rectifier.

    A rectifieris a device that allows current to

    flow in one direction, but not the other.

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    Figure 13.29: Effect of doping silicon.

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    Figure 13.30:

    Ap-njunction as a

    rectifier.