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Crystallographic Axes
GEOL 3055 Morphological and optical crystallography JH Schellekens Crystallographic Axes Klein (2002) p 5 Crystallographic axes
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Which Crystal System? Orthorhombic Tetragonal Hexagonal
a=b=c = = = 90 a=b=c = = = 90 a1 = a2 = a3 (120), c perpendicular Orthorhombic Tetragonal Hexagonal
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Crystallographic axes
When we are describing crystals, it is convenient to use a reference system of three axes, comparable to the axes of analytical geometry. These imaginary axes are called the ‘crystallographic axes’ These axes are fixed by symmetry & Coincide with symmetry axes Parallel to intersections of major crystal faces
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Crystallographic axes
Ideally crystallographic axes should be parallel to the edges of the unit cell, and lengths proportional to the cell dimensions REMEMBER All crystals except hexagonal referred to by 3 axes: a, b and c Convention: a is angle between b and c b is angle between a and c g is angle between a and b
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Crystallographic axes
Hexagonal isometric
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Crystallographic axes
Axial Ratios All the crystal systems, except isometric & tetragonal, have crystallographic axes differing in length The steps on the crystallographic axes, because they are dependent on the unit cell, are different in size
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Crystallographic axes
For instance orthorhombic sulfur a= 10.47A, b=12.87A, c=24.49A We can write a, b and c as ratios of b a/b : b/b : c/b 10.47/ : : /12.87 : 1 : We are only interested in the proportional differences, the axial ratios
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Crystallographic axes
Crystal faces are defined by indicating their intercepts on the crystallographic axes Face AB is parallel to the c-axis and intercepts a and b Parameters of this face are 1a:1b: c It intercepts 1 length of the a axis, one length of the b-axis and is parallel to the c-axis 8 Fig.5.28
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Crystallographic axes
Crystal faces are defined by indicating their intercepts on the crystallographic axes Fig.5.28
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Face Intercepts… Lattice plane A-B B Y or b axis z or c axis
(vertical) A A A’ A’ B X or a axis Plane A-A Intercepts: 1a, ∞b, ∞c Intersects x axis at one unit (1), is parallel to the y axis ( ∞ ) and the z axis (∞ ) Plane A-B, intersects 1a and 1b, but is parallel to c or ∞c Parameters: 1a, 1b, ∞c
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Unit face If there are several faces of a crystal intersecting all three axes, the largest face at the positive end of the crystallographic axis is taken as the unit face. Consider this example: Unit face (the face with the clear shade)
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Steps to determine Miller Indices and the Miller-Bravais Indices
1. The first thing that must be ascertained are the fractional intercepts that the plane/face makes with the crystallographic axes. In other words, how far along the unit cell lengths does the plane intersect the axis. e.g: 1a, ∞b, ∞c and 1a, 1b, ∞c and 1a, 2b, 4c 2. Omit a, b, c and commas e.g: 1 ∞ ∞ and 1 1 ∞ and 1 2 4 3. Take the reciprocal of the fractional intercept of each unit length for each axis. e.g.: 1/1 1/∞ 1/∞ and 1/1 1/1 1/∞ and 1/1 ½ ¼
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Steps to determine Miller Indices and the Miller-Bravais Indices
4. Finally the fractions are cleared (using a common denominator). so: 1/1 1/∞ 1/∞ and 1/1 1/1 1/∞ and 1/1 ½ ¼ Becomes and and 4 2 1 5. Enclose the integers in parentheses So: (100) and (110) and (421) These designate that specific crystallographic plane within the lattice. Since the unit cell repeats in space, the notation actually represents a ‘family of planes’, all with the same orientation.
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Steps to determine Miller Indices and the Miller-Bravais Indices
(100) and (110) and (421) are called the Miller indices In the hexagonal system there are 3 horizontal axes and one vertical. The indices are called the Miller-Bravais indices
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Summary “When intercepts are assigned to the faces of
a crystal, without knowledge of its cell dimensions, one face that cuts all three axes is arbitrarily assigned the units 1a,1b,1c”
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Summary (hkl)
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The previous notation is called the Miller Indices and ONLY applies for the Triclinic, Monoclinic, Orthorhombic and Isometric systems…
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Two very important points about intercepts of faces:
The intercepts or parameters are relative values, and do not indicate any actual cutting lengths. Since they are relative, a face can be moved parallel to itself without changing its relative intercepts or parameters.
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Miller indices Try & work out how the shaded face (in each case) intersects the axes (111) (001) (110)
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How is it for hexagonal and trigonal systems?
Recall both systems have 4 crystallographic axes. In this case, the notation for the intersection of faces is called: Miller -Bravais Indices (hkil) (1010) One,zero,bar one, zero h + k + I (1+0-1)= 0
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