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Solids crystalline amorphous well defined structures no orderly structure glass quartz SiO 2 crystal lattice system of points describes arrangement of partic

Lect3 Tinh thể

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Page 1: Lect3 Tinh thể

Solids

crystalline

amorphous

well defined structures

no orderly structure glass

quartz

SiO2

crystal lattice system of pointsdescribes arrangement of particles

Page 2: Lect3 Tinh thể

unit cell repeating structural unit lattice

7 unit cells

simple cubic

formed from packing spheres

Page 3: Lect3 Tinh thể

unit cells

crystalline solids

hexagonal closest packing

“abab” layers “abca” layers

cubic packing

“aaa” layers

in 3 dimensions

hexagonal closest pack cubic closest pack

“abab” layers

simple cubic body centered cubic

Page 4: Lect3 Tinh thể

Three-Dimensional Cubic Lattices

Simple cubic

Face-centered cubic

Body-centered cubic

1/8x 8 =1 particle

(1/8 )x 8 + 1 = 2 particles

(1/8 )x 8 (1/2 )x 6+ = 4 particles

cubic closest pack

a a a

a b a b

a b c a b c

coordination number = 6

coordination number = 8

coordination number = 12

Page 5: Lect3 Tinh thể

Calculation of atomic radii

Cu faced-centered cubic

density = 8.92 g/cm3

mass = 63.546 g/mol

63.546 gmol

1 mol6.022 x 1023 atoms

4 atomsunit cell 8.92 g

cm3

4.732 x 10-23 cm3 / unit cell( )1/3

= 3.617 x 10-8 cm

(3.617 x 10-8)2 + (3.617 x 10-8)2 = (4r)2

r = 1.279 x 10-8 cm1 cm1 x 10-2 m

1 x 10-12 m1 pm = 127 pm

r+2r+r

lattice parameter, a

Page 6: Lect3 Tinh thể

X-Ray Diffraction by Crystals

Bragg Equation n = 2d sin

diffraction interference between waves caused byobject in their pathconstructive or destructive

d

Page 7: Lect3 Tinh thể

Types of Crystalline Solids

Covalent Ionic Molecular atoms in lattice ions in lattice molecules in lattice

m.p. depends on bonding forces

Cdiamond 3550oC NaCl 800OC H2O 0oC

covalent ionic H-bonding

Page 8: Lect3 Tinh thể

Covalent solidsatoms in lattice

carbon

sp3 sp2 sp2

hardest material known conduct electricity - e-

diamond

doesn’t conduct electricity

graphite buckminsterfullerene

Page 9: Lect3 Tinh thể

Covalent solidsatoms in lattice

metals every lattice point - atom of 1 metal

body-centered cubicface-centered cubichexagonal close packed

brass substitutional alloy

steel interstitial alloy

share valence e- e- “sea”

melting pointNa 97oCCr 1890oC

good conductors

Page 10: Lect3 Tinh thể

Ionic Solids

trigonal hole tetrahedral hole octahedral holetoo small r = 0.225 R r = 0.414 R

composed of charged species –

anions and cationseach unit cell -

anions at lattice points cations in “holes”NaCl face-centered cubicCsCl simple cubic

unit cell neutralstoichiometry of compound

different in size

Page 11: Lect3 Tinh thể
Page 12: Lect3 Tinh thể

Molecular Solids molecules in lattice

hemoglobin reaction center

19881962Perutz and Kendrew Deisenhofer, Huber and Michel