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The internal order of minerals: Lattices, Unit Cell

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The internal order of minerals: Lattices, Unit Cell ... Rhombus: a1=a2, ?=60o. or 120o; Fig 5.50d. Parallelogram: ab, ?90o. Fig 5.50a. Rectangles ab, ?=90o ... – PowerPoint PPT presentation

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Title: The internal order of minerals: Lattices, Unit Cell


1
The internal order of minerals Lattices, Unit
Cell Bravais Lattices
  • Geol 3055
  • Klein (22nd ed), pages 213-221
  • 229-234

2
Definition of a mineral
  • Naturally occuring
  • Homogenous solid
  • Definite (but not fixed) chemical composition
  • Defined physical properties
  • Highly ordered atomic arrangement
  • Usually formed by inorganic processes

3
  • Ordered atoms distinguished crystals (solids)
    from liquids, gases and glasses
  • Orderedperiodic repetition of atoms of atom or
    ion througout an infinite atomic array.
  • An atom is surrounded by an identical arrangement
    of neighboring atoms, which are n quantity of
    unit cells
  • Unit cells dimensions 5-20 angstroms
  • (1A10-8cm)

4
Translation
  • Example of translation (vectors)
  • , , , ,
  • , , , ,

Translation in y-axis
Translation in x-axis
Translation symbols are t1 for the y axis
translation and t2 for the x-axis translation
for 2-D figures. 3-D figures have a t3
5
One-dimensional order (rows)
  • Motifs, nodes or objects in a row
  • In a row the magnitude of one translation
    determines spacing (distance)

6
Two dimensional order (plane lattices)
  • Regular translation in two different directions
  • The connection of four nodes in the figure
    represent a unit cell (smallest building unit).
    Various unit cells produce a plane lattice.

y
?
x
Unit cell
7
Lattices
  • When motifs (commas) are substitute by points
    (nodes) the pattern is called a lattice. The
    nodes represent atoms or ions.
  • Lattice is an imaginary pattern of points (or
    nodes) in which every point has an environment
    that is identical to that of any other point
    (node) in a pattern. A lattice has no specific
    origin, as it can be shifted parallel to itself

a
8
Plane lattices
  • The are ONLY 5 possible and distinct plane
    lattices or nets (see figure 5.50)
  • Result by the repetition of a row (translation
    along y)
  • Depend on the angle ? between x and y, and the
    size of the b translation along y
  • See Fig 5.50

9
Unit cells produce by arrays of nodes
Parallelogram a?b, ??90o Fig 5.50a
Rectangles a?b, ?90o Figs 5.50a b
Square, a1a2, ?90o fig 5.50 e
Diamond a1a2, ??90o,60o,120o fig 5.50c
Rhombus a1a2, ?60o or 120o Fig 5.50d
P primitive (only nodes that produce the unit
cell are _at_ corners of figure C centered (node
at center of unit cell, is called non primitive
10
Three-dimensional order
  • Three vectors (a, b, c) instead of two (a b)
  • The stacking in the c-axis, of the five planar
    nets discussed in 2-dimensional figures (fig.
    5.50), will produce 14 different lattice types
    known as the Bravais Lattices (see figs. 5.62
    5.63)
  • ONLY possible ways which points can be arranged
    periodically in 3 dimensions
  • Coincide with the 32 crystal classes studied in
    class!
  • (see CD-ROM Three dimensional order Generation
    of the Bravais Lattices)

11
Three-dimensional order unit cells
  • Since a lot of unit cells are possible in 3-d
    figures, crystallographer drawn some rules to
    minimize the number
  • Edges of unit cells should coincide, if possible,
    with symmetry axes of the lattice
  • Edges should be related to each other by the
    symmetry of the lattice
  • The smallest possible cell should be chosen in
    accordance with first two rules.

12
14 Bravais Lattices
P primitive C centered I body centered
node at center of figure F face centered
(node at the center of face(s)
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