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Symmetry, Groups and Crystal Symmetry, Groups and Crystal Structures Structures The Seven Crystal Systems The Seven Crystal Systems
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Symmetry, Groups and Crystal Structures

Feb 08, 2016

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Symmetry, Groups and Crystal Structures. The Seven Crystal Systems. Minerals structures are described in terms of the unit cell. The Unit Cell. The unit cell of a mineral is the smallest divisible unit of mineral that possesses all the symmetry and properties of the mineral. - PowerPoint PPT Presentation
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Page 1: Symmetry, Groups and Crystal Structures

Symmetry, Groups and Symmetry, Groups and Crystal StructuresCrystal Structures

The Seven Crystal SystemsThe Seven Crystal Systems

Page 2: Symmetry, Groups and Crystal Structures
Page 3: Symmetry, Groups and Crystal Structures
Page 4: Symmetry, Groups and Crystal Structures

Minerals structures are described in terms of the unit cell

Page 5: Symmetry, Groups and Crystal Structures

The Unit Cell• The unit cell of a mineral is the smallest

divisible unit of mineral that possesses all the symmetry and properties of the mineral.

• It is a small group of atoms arranged in a “box” with parallel sides that is repeated in three dimensions to fill space.

• It has three principal axes (a, b and c) and• Three inter-axial angles (, , and )

Page 6: Symmetry, Groups and Crystal Structures

The Unit Cell• Three unit cell vectors a, b, c• Three angles between

vectors: • is angle between b and c• is angle between a and c• is angle between a and b

Page 7: Symmetry, Groups and Crystal Structures

Seven Crystal Systems• The presence of symmetry operators places

constraints on the geometry of the unit cell.• The different constraints generate the

seven crystal systems.– Triclinic Monoclinic– Orthorhombic Tetragonal– Trigonal Hexagonal– Cubic (Isometric)

Page 8: Symmetry, Groups and Crystal Structures

Seven Crystal Systems• Triclinic a b c; 90º 120º• Monoclinic a b c; = º 90º 120º• Orthorhombic a b c; = º• Tetragonala = b c; = º• Trigonal a = b c; = º; 120º• Hexagonal a = b c; = º; 120º• Cubic a = b = c; = º

Page 9: Symmetry, Groups and Crystal Structures

Symmetry Operations

• A symmetry operation is a transposition of an object that leaves the object invariant.– Rotations

• 360º, 180º, 120º, 90º, 60º – Inversions (Roto-Inversions)

• 360º, 180º, 120º, 90º, 60º – Translations:

• Unit cell axes and fraction thereof.– Combinations of the above.

Page 10: Symmetry, Groups and Crystal Structures

Rotations• 1-fold 360º I

Identity• 2-fold 180º 2• 3-fold 120º 3• 4-fold 90º 4• 6-fold 60º 6

Page 11: Symmetry, Groups and Crystal Structures

Roto-Inversions(Improper Rotations)

• 1-fold 360º• 2-fold 180º• 3-fold 120º• 4-fold 90º• 6-fold 60º

Page 12: Symmetry, Groups and Crystal Structures

Translations

• Unit Cell Vectors• Fractions of unit cell vectors

– (1/2, 1/3, 1/4, 1/6)• Vector Combinations

Page 13: Symmetry, Groups and Crystal Structures

Groups

• A set of elements form a group if the following properties hold:– Closure: Combining any two elements gives a third

element– Association: For any three elements: (ab)c = a(bc).– Identity: There is an element, I, such that Ia = aI =

a– Inverses: For each element, a, there is another

element, b, such that ab = I = ba

Page 14: Symmetry, Groups and Crystal Structures

Groups

• The elements of our groups are symmetry operators.

• The rules limit the number of groups that are valid combinations of symmetry operators.

• The order of the group is the number of elements.

Page 15: Symmetry, Groups and Crystal Structures

Point Groups (Crystal Classes)

• We can do symmetry operations in two dimensions or three dimensions.

• We can include or exclude the translation operations.

• Combining proper and improper rotation gives the point groups (Crystal Classes)– 32 possible combinations in 3 dimensions– 32 Crystal Classes (Point Groups)– Each belongs to one of the (seven) Crystal

Systems

Page 16: Symmetry, Groups and Crystal Structures

Space Groups• Including the translation operations gives

the space groups.– 17 two-dimensional space groups– 230 three dimensional space groups

• Each space group belongs to one of the 32 Crystal Classes (remove translations)

Page 17: Symmetry, Groups and Crystal Structures

Crystal Morphology• A face is designated by Miller indices in

parentheses, e.g. (100) (111) etc.• A form is a face plus its symmetric

equivalents (in curly brackets) e.g {100}, {111}.

• A direction in crystal space is given in square brackets e.g. [100], [111].

Page 18: Symmetry, Groups and Crystal Structures

Halite Cube

Page 19: Symmetry, Groups and Crystal Structures

Miller Indices• Plane cuts axes at

intercepts (,3,2).• To get Miller indices,

invert and clear fractions.• (1/, 1/3, 1/2) (x6)=• (0, 2, 3)• General face is (h,k,l)

Page 20: Symmetry, Groups and Crystal Structures

Miller Indices• The cube face is (100)• The cube form {100}

comprises faces (100),(010),(001), (-100),(0-10),(00-1)

Page 21: Symmetry, Groups and Crystal Structures

Halite Cube (100)

Page 22: Symmetry, Groups and Crystal Structures

Stereographic Projections

• Used to display crystal morphology.

• X for upper hemisphere.

• O for lower.

Page 23: Symmetry, Groups and Crystal Structures

Stereographic Projections

• We will use stereographic projections to plot the perpendicular to a general face and its symmetry equivalents (general form hkl).

• Illustrated above are the stereographic projections for Triclinic point groups 1 and -1.

Page 24: Symmetry, Groups and Crystal Structures

Anatase TiO2

(tetragonal)

Page 25: Symmetry, Groups and Crystal Structures

Halite Cube

Page 26: Symmetry, Groups and Crystal Structures

Halite Cube