Chapter 3: Crystallographic directions and planes
Chapter 3: Crystallographic directions and planes
Outline Crystallographic directions Crystallographic planes Linear and planar atomic densities Close-packed crystal structures
Crystallographic directions
Direction: a line between two points and a vector
General rules for defining a crystallographic direction
? pass through the origin of a coordinate system
? determine length of the vector projection in the unit cell dimensions a, b, and c
? remove the units [ua vb wc]---[uvw] e.g [2a 3b 5c]--[2 3 5]
? uvw are multiplied and divided by a common factor to reduce them to smallest integer values
1
Crystallographic directions (continue)
? denote the direction by [uvw] ? family direction , defined by transformation ? material properties along any direction in a family are the
same, e.g. [100],[010],[001] in simple cubic are same. ? for uniform crystal materials, all parallel directions have the
same properties ? negative index: a bar over the index
Determine a direction
Examples
Determine the indices of line directions
2
Examples
Sketch the following directions : [110], [1 2 1], [ 1 0 2]
Hexagonal crystal
4-index, or Miller-Bravais, coordinate system Conversion from 3-index to 4-index system
z
a2
-
a3 a1
Fig. 3.8(a), Callister 7e.
[u'v'w'] [uvtw]
u = 1 (2u'-v') 3
v = 1 (2v'-u') 3
t = -(u +v) w= w'
3
Crystallographic planes
Orientation representation (hkl)--Miller indices Parallel planes have same miller indices Determine (hkl)
? A plane can not pass the chosen origin ? A plane must intersect or parallel any axis ? If the above is not met, translation of the plane or origin is
needed ? Get the intercepts a, b, c. (infinite if the plane is parallel to an
axis) ? take the reciprocal ? smallest integer rule
(hkl) // (hkl) in opposite side of the origin For cubic only, plane orientations and directions with same indices are perpendicular to one another
Crystallographic planes (continue)
Adapted from Fig. 3.9, Callister 7e.
4
Crystallographic planes (continue)
Example 1. Intercepts 2. Reciprocals
3. Reduction
4. Miller Indices
a bc 1 1 1/1 1/1 1/ 1 10 1 10
(110)
Example 1. Intercepts 2. Reciprocals
3. Reduction
4. Miller Indices
a bc 1/2 1/? 1/ 1/ 20 0 20 0
(100)
z c
a x
z c
a x
y b
y b
Crystallographic planes (continue)
In hexagonal unit cells the same idea is used
z
Example 1. Intercepts 2. Reciprocals
3. Reduction
a1 a2 a3
1 -1 1 1/ -1 1 0 -1 1 0 -1
4. Miller-Bravais Indices (1011)
c
1
1
1
a2
1
a3
a1
Adapted from Fig. 3.8(a), Callister 7e.
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