1. Basic Crystallography
Prepared By:- Mr. Amit Phogat
(Lecturer in Mechanical Deptt.)

2. An unspeakable horror seized me
An unspeakable horror seized me. There was a darkness; then a dizzy, sickening sensation of sight that was not like seeing; I saw a line that was no line; space that was not space I shrieked aloud in agony, " Either this is madness or it is Hell." "It is neither," calmly replied the voice of the Sphere, "it is Knowledge; it is Three Dimensions: open your eye once again and try to look steadily

3. "Distress not yourself if you cannot at first understand the deeper mysteries of Spaceland. By degrees they will dawn upon you." On the occasion of the Square's first encounter with three dimensions, from E. A. Abbott's Flatland, (1884).

4. Repetition = Symmetry Types of repetition: Rotation Translation

5. Rotation What is rotational symmetry?

6. Imagine that this object will be rotated (maybe)

7. Was it?

8. The object is obviously symmetric…it has symmetry

9. The object is obviously symmetric…it has symmetry Can be rotated 90° w/o detection

10. …………so symmetry is really doing nothing

11. Symmetry is doing nothing - or at least doing something so that it looks like nothing was done!

12. What kind of symmetry does this object have?

13. What kind of symmetry does this object have?4

14. What kind of symmetry does this object have?4 m

15. What kind of symmetry does this object have?4 m

16. What kind of symmetry does this object have?4 m

17. What kind of symmetry does this object have?4
4mm m

18. Another example:

19. Another example: 6
6mm m

20. And another:

21. And another: 2 2

22. What about translation? Same as rotation

23. What about translation
What about translation? Same as rotation Ex: one dimensional array of points
Translations are restricted to only certain values to
get symmetry (periodicity)

24. 2D translations Lots of common examples

25. Each block is represented by a point

26. This array of points is a LATTICE

27. Lattice - infinite, perfectly periodic array of points in a space

28. Not a lattice:

29. Not a lattice:

30. Not a lattice - ….some kind of STRUCTURE becuz not just points

31. Another type of lattice - with a different symmetry rectangular

32. Another type of lattice - with a different symmetry square

33. Another type of lattice - with a different symmetry hexagonal

34. Back to rotation - This lattice exhibits 6-fold symmetry hexagonal

35. Periodicity and rotational symmetry What types of rotational symmetry allowed?

36. Periodicity and rotational symmetry Suppose periodic row of points is rotated through ± a:

37. Periodicity and rotational symmetry To maintain periodicity,
vector S = an integer x basis translation t

38. a S t
vector S = an integer x basis translation t
t cos a = S/2 = mt/2
m cos a a axis
π 1
/ π/3 5π/3 6
π/2 3π/2 4
/ π/3 4π/3 3
π π

39. m cos a a axis π
/ π/3 5π/3 6
π/2 3π/2 4
/ π/3 4π/3 3
π - π 2
Only rotation axes consistent with lattice
periodicity in 2-D or 3-D

40. We abstracted points from the shape:

41. We abstracted points from the shape:
Now we abstract further:

42. Now we abstract further:
This is a UNIT CELL

43. Now we abstract further:
This is a UNIT CELL
Represented by two lengths and an angle
…….or, alternatively, by two vectors

44. Basis vectors and unit cells
T = t a + t b a b
a and b are the basis vectors for the lattice T

45. In 3-D: a b
a, b, and c are the basis vectors for the lattice c

46. In 3-D:
T = t a + t b + t c a b T
a, b, and c are the basis vectors for the lattice c

47. a b c g
Lattice parameters:

48. The many thousands of lattices classified into crystal systems
System Interaxial Axes
Angles
Triclinic a ≠ b ≠ g ≠ 90° a ≠ b ≠ c
Monoclinic a = g = 90° ≠ b a ≠ b ≠ c
Orthorhombic a = b = g = 90° a ≠ b ≠ c
Tetragonal a = b = g = 90° a = b ≠ c
Cubic a = b = g = 90° a = b = c
Hexagonal a = b = 90°, g = 120° a = b ≠ c
Trigonal a = b = 90°, g = 120° a = b ≠ c

49. The many thousands of lattices classified into crystal systems
System Minimum symmetry
Triclinic or 1
Monoclinic or 2
Orthorhombic three 2s or 2s
Tetragonal or 4
Cubic four 3s or 3s
Hexagonal or 6
Trigonal or 3

50. Within each crystal system, different types of
centering consistent with symmetry
System Allowed
centering
Triclinic P (primitive)
Monoclinic P, I (innerzentiert)
Orthorhombic P, I, F (flächenzentiert), A (end centered) Tetragonal P, I
Cubic P, I, F
Hexagonal P
Trigonal P, R (rhombohedral centered)
The 14 Bravais lattices

51. For given lattice, infinite number of
unit cells possible:

52. When choosing unit cell, pick:
Simplest, smallest
Right angles, if possible
Cell shape consistent with symmetry