| . |
Week 2: Jan 23 and 25
CRYSTALLOGRAPHY (cont'd)
-
Point symmetry - symmetry wherein a motif is
repeated about a point by some symmetry operation:
-
Reflection - produced by a mirror plane. The
mirror plane divides the object (crystal) into two symmetric halves, Denoted
by an m.
-
Rotation - repetition of a motif by rotation about a
symmetry
axis:
-
A2 - two fold symmetry axis
-
A3 - three-fold symmetry axis
-
A4 - four fold symmetry axis
-
A6 - six fold symmetry axis
-
Inversion - produced by a center of symmetry, denoted
by i. An object with a center of symmtery will have identical points
on opposite sides of the center of symmetry.
-
Roto-inversion - combinations of axes of rotation and
inversion. Some combinations produce new symmetries. An A2 combined
with i is equivalent to m (mirror plane).
-
Crystallographic axes - 3 or 4 (in case of hexagonal
system) imaginary axes in a crystal that can be used as a frame of
reference for naming crystal faces. They are oriented parallel to and their
lengths are proportional to the axes of the unit cell.
-
The Six Crystal Systems - six crystal systems
can be defined based on the characteristics of their crystallographic axes
and their symmetries:
| Crystal System Name |
Properties of axes |
Characteristic symmetry |
|
| isometric |
lengths:
a1=a2=a3
angles:
all angles (alpha, beta, and gamma) =90 degrees |
4 three-fold axes |
 |
| tetragonal |
lengths:
c not equal to a1=a2
angles: all equal to 90 |
1 four-fold axis |
 |
| orthorhombic |
lengths: all three unequal
angles: all 90 degrees |
2 mirror planes and/or 2
two-fold axes |
 |
| monoclinic |
lengths: all unequal
angles: alpha and beta = 90; beta not equal to 90 |
1 mirror plane and/or 1
two-fold axis |
 |
| triclinic |
lengths: all unequal
angles: all non-90 degrees |
center of symmetry only, or
no symmetry |
 |
| hexagonal |
lengths: c axis not equal to
3 equal horizontal axes (a1, a2, a3)
angles: angle between c and a-axes = 90; angle between 'a' axes = 120 |
1 six=fold axis |
 |
(Images of crystallographic axes are from: http://webmineral.com/help/CellDimensions.shtml)
-
Miller Indices - a system for naming crystal
faces based on their relationship to the crystallographic axes. In principle,
they are derived by:
-
determining the face intercepts - the distance
along each axis that the face intersects
-
taking the inverse of the face intercept
-
clearing fractions and simplifying
-
Law of Hauy - crystal faces make simple rational
intercepts on crystal axes (and Miller Indices end up being small whole
numbers)
-
Law of Bravais - Common crystal faces are parallel
to lattice planes that have a high lattic node density
-
Crystal Forms - a group of faces having the same
relationship to the symmetry elements of the crystal. Denoted as {hkl},
rather than (hkl), which refers to a single face.
-
open forms and closed forms
-
Forms to know: cube, octahedron, tetrahedron, dodecahedron,
pedion, pinacoid, dome, sphenoid, prism, pyramid, dipyramid, trapezohedron,
scalenohedron, rhombohedron
-
Note: Given the crystal system of a crystal,
its symmetry, and the forms that are present, it is now possible sketch
or imagine what the crystal will look like (in a general way -- additional
descriptors will be covered under mineral habit)
Mineralogy
homepage | Saint Louis University
| Earth & Atmospheric Sciences
|