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Estado sólido1

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    Copyright Houghton Mifflin Company. All rights reserved. 16a1

    Red Beryl, Be3Al2Si6O18-

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    Copyright Houghton Mifflin Company. All rights reserved. 16a2

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    Copyright Houghton Mifflin Company. All rights reserved. 16a3

    Figure 16.1: Schematic representation

    of the three states of matter

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    Copyright Houghton Mifflin Company. All rights reserved. 16a4

    Figure 16.2:

    (a) The

    electrostatic

    interaction of

    two polar

    molecules.

    (b) Theinteraction of

    many dipoles

    in a

    condensedstate.

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    Copyright Houghton Mifflin Company. All rights reserved. 16a5

    Figure 16.3: The polar water molecule.

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    Copyright Houghton Mifflin Company. All rights reserved. 16a6

    Figure 16.4: The boiling points of the covalent

    hydrides of elements in Groups 4A, 5A, 6A, and 7A.

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    7/38Copyright Houghton Mifflin Company. All rights reserved. 16a7

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    8/38Copyright Houghton Mifflin Company. All rights reserved. 16a8

    Figure 16.5: An instantaneous polarization can

    occur on atom a, creating instantaneous dipole.

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    9/38Copyright Houghton Mifflin Company. All rights reserved. 16a9

    Figure 16.6: A molecule in the interior of a liquid is attracted to the

    molecules surrounding it, whereas a molecule at the surface of liquid is

    attracted only by molecules below it and on each side of it.

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    10/38Copyright Houghton Mifflin Company. All rights reserved. 16a10

    Figure 16.7:

    Nonpolarliquid

    mercury

    forms a

    convexmeniscus in

    a glass tube.

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    11/38Copyright Houghton Mifflin Company. All rights reserved. 16a11

    Figure 16.8: Several crystalline solids

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    12/38Copyright Houghton Mifflin Company. All rights reserved. 16a12

    Figure 16.9: Three cubic unit cells and the

    corresponding lattices.

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    13/38Copyright Houghton Mifflin Company. All rights reserved. 16a13

    Figure 16.10: X-rays scattered from two different

    atoms may reinforce (constructive interference) or

    cancel (destructive interference) one another.

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    14/38Copyright Houghton Mifflin Company. All rights reserved. 16a14

    Figure 16.11: Reflection of X rays of

    wavelength

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    15/38Copyright Houghton Mifflin Company. All rights reserved. 16a15

    A conch

    shell on abeach.

    Source: Corbis

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    16/38Copyright Houghton Mifflin Company. All rights reserved. 16a16

    Figure 16.12: Examples of three types of

    cyrstalline solids.

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    17/38Copyright Houghton Mifflin Company. All rights reserved. 16a17

    Figure 16.13: The closest packing

    arrangement of uniform spheres.

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    18/38Copyright Houghton Mifflin Company. All rights reserved. 16a18

    Figure 16.14: When spheres are closest packed so that the spheres

    in the third layer are directlly over those in the first layer (aba),

    the unit cell is the hexagonal prism illustrated here in red.

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    19/38Copyright Houghton Mifflin Company. All rights reserved. 16a19

    A toy slide puzzle

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    20/38Copyright Houghton Mifflin Company. All rights reserved. 16b20

    A section of a surface containing copper atoms

    (red) and an indium atom (yellow).

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    21/38Copyright Houghton Mifflin Company. All rights reserved. 16b21

    Figure 16.15: When spheres are packed in the abc

    arrangement, the unit cell is face-centered cubic.

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    22/38Copyright Houghton Mifflin Company. All rights reserved. 16b22

    Figure 16.16:

    The indicatedsphere has

    12 equivalent

    nearest

    neighbors.

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    23/38Copyright Houghton Mifflin Company. All rights reserved. 16b23

    Figure 16.17: The net number of spheres

    in a face-centered cubic unit cell.

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    24/38Copyright Houghton Mifflin Company. All rights reserved. 16b24

    Volume of a

    unit cell(2r, 4r, r)

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    25/38Copyright Houghton Mifflin Company. All rights reserved. 16b25

    Figure 16.18: In the body-centered cubic unit cell

    the spheres touch along the body diagonal.

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    26/38Copyright Houghton Mifflin Company. All rights reserved. 16b26

    Figure 16.19: The body-centered cubic unit

    cell with the center sphere deleted.

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    Copyright Houghton Mifflin Company. All rights reserved. 16b27

    Figure 16.20: On the face of the

    body-centered cubic unit cell.

    Figure 16 21: The relationship of the body

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    Copyright Houghton Mifflin Company. All rights reserved. 16b28

    Figure 16.21: The relationship of the body

    diagonal (b) to the face diagonal (f) and the edge

    (e) for the body-centered cubic unit cell.

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    Copyright Houghton Mifflin Company. All rights reserved. 16b29

    Figure 16.22:

    The electron

    sea model for

    metals

    postulates a

    regular array of

    cationsin a "sea" of

    valence

    electrons.

    G i f h ll di ifi d

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    Copyright Houghton Mifflin Company. All rights reserved. 16b30

    Grains of nanophase palladium magnified

    200,000 times by an electron microscope.

    Source: Nanophase Technologies Corporation

    Figure 16 23: The molecular orbital energy

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    Copyright Houghton Mifflin Company. All rights reserved. 16b31

    Figure 16.23: The molecular orbital energy

    levels produced when various numbers

    of atomic orbitals interact.

    Fi 16 24 A t ti f th

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    Copyright Houghton Mifflin Company. All rights reserved. 16b32

    Figure 16.24: A representation of the energy

    levels (bands) in a magnesium crystal

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    Copyright Houghton Mifflin Company. All rights reserved. 16b33

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    Copyright Houghton Mifflin Company. All rights reserved. 16b34

    Figure 16.25:

    Two types ofalloys

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    Copyright Houghton Mifflin Company. All rights reserved. 16b35

    Figure 16.26:

    The

    structures of

    (a) diamond

    and (b)

    graphite.

    Fi 16 27 P ti l t ti f th MO

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    Copyright Houghton Mifflin Company. All rights reserved. 16b36

    Figure 16.27: Partial representation of the MO

    energies in (a) diamond and (b) a typical metal

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    Copyright Houghton Mifflin Company. All rights reserved. 16b37

    Graphite consitst of layers of carbon atoms.

    Figure 16 28: The p orbitals (a) perpendicular to the plane of

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    Figure 16.28: The p orbitals (a) perpendicular to the plane of

    th carbon ring system in graphite can combine to form

    (b) an extensive pie bonding network.


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