m_03 symmetry operation
TRANSCRIPT
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MINERALOGY03 : SYMMETRY OPERATIONM03_Symmetry Operation
LECTURE NOTE
DEPARTMENT OF GEOLOGY
FACULTY OF GEOLOGY, PADJ ADJ ARAN UNIVERSITY
ACADEMIC : 2012/2013
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REcOGNITION Of MINERAL SYMMETRY External Crystal Form (Morphology)
- macroscopic observations/measurements of crystal faces- 32 crystal classes (point groups) possible symmetry elements orcombinations of elements
Internal Atomic Arrangement
- determined from X-ray diffraction- takes into account 3D translation- 14 lattice types (Bravais lattices)- Combination of 32 point groups and 14 lattice types yields 230space groups
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Symmetry
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OPERASISIMETRI
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Symmetry Plane (Bidang simetri)(mirror / m / P)
Axes (Sumbu Simetri) (axes / A)
Center of Symmetry (Pusat Simetri)(center / C)
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ExTERNAL SYMMETRY ELEMENTScRYSTAL MORPhOLOGY
(ELEMENT SYMMETRY)
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ExTERNAL SYMMETRY ELEMENTScRYSTAL MORPhOLOGY
(SYMMETRY OPERATION)
(a) Rotation (b) Reflection (c) Center of Symmetry (d) Rotation withInversion
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(Klein & Hulburt, J R., 1993)
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ExTERNAL SYMMETRY ELEMENTSMOTIf PATTERNS
Reflection
Center of Symmetry
Rotation with Inversion Mineralogy@Rosana 2013
(Klein & Hulburt, J R., 1993)
Rotation
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Bidang simetri utama (BSU) : bidang simetri yang padanyaterdapat dua atau lebih bidang simetri lain yang tegak lurusdan tegak lurus terhadap sumbu simetri berharga palingtinggi.
Bidang simetri biasa : bidang yang membagi kristalmenjadi dua bagian yang simetris yang padanya terdapatsatu sumbu simetri
Operasi bidang simetri ini disebut operasi pencerminan
(Reflection)
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SYMMETRY PLANE (BIdANG SIMETRI)
(Klein & Hulburt, J R., 1993) 10
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Bidang simetri vertikal, horizontal dan diagonal, serta simetri utama dantambahan
(Klein & Hulburt, J R., 1993)Mineralogy@Rosana 2013
SYMMETRY PLANE (BIdANG SIMETRI)
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SYMMETRY AxESAdalah suatu garis lurus yang dibuat melalui pusat kristaldan bila kristal tersebut diputar 360 pada sumbutersebut, maka pada kedudukan tertentu akan dijumpai
kenampakan yang sama dengan semula.
Sumbu simetri ada dua macam : Sumbu simetri biasa (bipoler) : sumbu khayal yang
melalui kristal yang apabila diputar 360, akan dijumpai
konfigurasi yang sama atau hal-hal yang sama yangmuncul lebih dari satu kali.
Sumbu poler : sumbu khayal (seperti halnya sumbubipoler), hanya kedua ujung sumbu menembus duakeadaan yang berbeda.
Operasi dari sumbu lipat ini disebut sebagai operasi rotasi(perulangan periodik dari motif asli yang dijumpai setelahterjadinya perputaran motif tersebut dengan sudutsebesar 360 akibat beroperasinya sumbu rotasi atau
sumbu lipat). Mineralogy@Rosana 2013 12
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Operasi Rotasi (Klein & Hulburt, J R., 1993)
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Dibedakan lagi menjadi dua berdasarkan atas macamoperasinya :a. Gyre
b. Gyroida
Gyre : sumbu simetri biasa yang besarnya sudut putaradalah 360/n ; n adalah bilangan yang utuh sehingga akandiperoleh nilai n 180, 120, 90,60n = 2 (()) digyre/diadn = 3 () trigyre / triadn = 4 () Tetragyre / tetradn = 6 ( . ) Hexagyre / hexad
Gyroida ; sumbu simetri disini merupakan campuran dari
pemutaran melalui sumbu dan pencerminan pada bidangyang tegak lurus pada bidang tadi180 = digyroida ; C pusat simetri120 = Trigyroida90 = Tetragyroida
60 = Hexagyroida Mineralogy@Rosana 2013 14
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ROTATIONAL AxES As an external symmetry element, rotation
increments (n) range from 1 to
When considering the
limits of translation,
rotation increments are
limited to 1, 2, 3, 4,
and 6-fold
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2-D SYMMETRY
6
6
A Symmetr ical Pattern
Symmetry Elements
1. Rotation
a. Two-fold rotation= 360o/2 rotation
to reproduce a motif in asymmetrical pattern
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Motif
Element
Operation
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6
2-D SYMMETRY
Symmetry Elements
1. Rotation
a. Two-fold rotation
= 360o/2 rotation
to reproduce a
motif in asymmetricalpattern
= the symbol for a two-fold
rotation
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6
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firstoperationstep
2-D SYMMETRY
Symmetry Elements
1. Rotationa. Two-fold rotation
= 360o/2 rotationto reproduce a
motif in asymmetricalpattern
= the symbol for a two-foldrotation
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firstoperationstep
secondoperationstep
2-D SYMMETRY
Symmetry Elements
1. Rotationa. Two-fold rotation
= 360o/2 rotationto reproduce a
motif in asymmetricalpattern
= the symbol for a two-foldrotation
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2-D SYMMETRY
Symmetry
Elements
1. Rotation
a. Two-fold
rotation
Some familiarobjects have an
intrinsicsymmetry
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2-D SYMMETRY
Symmetry
Elements1. Rotation
a. Two-foldrotation
Some familiarobjects have an
intrinsicsymmetry
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2-D SYMMETRY
SymmetryElements
1. Rotation
a. Two-fold
rotation
Some familiar
objects have anintrinsicsymmetry
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2 D S
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2-D SYMMETRY
Symmetry
Elements1. Rotation
a. Two-fold
rotation
Some familiarobjects have an
intrinsicsymmetry
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2 D S
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2-D SYMMETRY
SymmetryElements
1. Rotation
a. Two-foldrotation
Some familiarobjects have anintrinsic
symmetry
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2 D S
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2-D SYMMETRY
Symmetry
Elements1. Rotation
a. Two-foldrotation
Some familiarobjects have an
intrinsicsymmetry
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2 D SYMMETRY
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2-D SYMMETRY
Symmetry Elements
1. Rotationa. Two-fold rotation
Some familiar
objects have anintrinsic symmetry
180o rotation makes itcoincident
Whats the motif here??
Second 180o brings the objectback to its original position
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3 D SYMMETRY
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3-D SYMMETRY
Symmetry Elements
1. Rotation
b. Three-fold
rotation
= 360o/3 rotation
to reproduce a
motif in asymmetricalpattern
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2 D SYMMETRY
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step 1
2-D SYMMETRY
Symmetry Elements
1. Rotation
b. Three-fold
rotation
= 360o/3 rotation
to reproduce a
motif in asymmetricalpattern
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2 D SYMMETRY
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step 1
step 2
2-D SYMMETRY
Symmetry Elements
1. Rotation
b. Three-foldrotation
= 360o
/3 rotationto reproduce amotif in asymmetricalpattern
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step 1
step 2
step 3
2-D SYMMETRY
Symmetry Elements
1. Rotation
b. Three-fold
rotation
= 360o/3 rotation
to reproduce a
motif in asymmetricalpattern
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2 D SYMMETRY
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2-D SYMMETRYSymmetry Elements
1. Rotation
6
6
666
6
6
6
1-fold 2-fold 3-fold 4-fold 6-fold
9t dZ5-fold and > 6-fold rotations will not work in combination with translations incrystals (as we shall see later). Thus we will exclude them now.
aidentity
Objects with symmetry:
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Combination of Symmetry Elements Multiple Rotational Axes
Axes at 90 (except 3-fold axes in cubicsymmetry at 5444)
Axes intersect atpoint
Possible symmetrycombinations:
422, 622, 222, 32, 23,432
(View 422 Symmetry.ai)
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Combination of Symmetry Elements
Multiple Rotational Axes with 32 Symmetry
- motif projectionsdo not require asecond set of 2-fold
axes
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Combination of Symmetry Elements Multiple Rotational Axes in the Cubic System
432 Point Group
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Pusat Simetri / titik simetri
Adalah suatu titik yang apabila ditarik garis melalui titiktersebut dari sembarang titik pada permukaan kristalakan membagi garis tsb sama panjang
Operasi pusat simetri disebut juga operasi inversi (i)
Inversi : suatu operasi simetri yang dihasilkan denganjalan menghubungkan titik-titik dari salah satu bidangkristal melalui titik pusatnya, sehingga dihasilkan titikturunannya yang berjarak sama dari pusat simetri, tetapiberseberangan dan terbalik
Hasil inversi suatu bidang kristal adalah bidang yangsejajar, sama dan sebangun, tetapi terbalik, dengan letakyang berseberangan terhadap pusat simetrinya danberjarak sama terhadap titik inversi tersebut.
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Inversi = Pusat Simetri (C)
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Pusat Simetri ( C )
disebut juga titik simetri adalah suatu titik apabiladitarik garis melalui titik tsb dari sembarang titikpada permukaan kristal akan membagi garis tsb samapanjang. Operasi pusat simetri disebut juga operasiinversi (i).
Inversi:suatu operasi simetri yang dihasilkan dengan jalanmenghubungkan titik-titik dari salah satu bidang kristalmelalui titik pusatnya, sehingga dihasilkan titik turunan-nya yang berjarak sama dari pusat simetri, tetapiberseberangan dan terbalik.
Inversi = Pusat Simetri (C)
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2 D SYMMETRY
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2-D SYMMETRY
Symmetry Elements
2. Inversion (i)
inversion through acenter to reproduce amotif in a symmetricalpattern
= symbol for an inversioncenter
inversion is identical to 2-fold
rotation in 2-D, but is uniquein 3-D (try it with yourhands)
6
6
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Operasi Inversi
(Klein & Hulburt, J R., 1993)
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Bidang simetri
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2-D SYMMETRY
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2-D SYMMETRY
Symmetry Elements
3. Reflection (m)
Reflection across a
mirror planereproduces a motif
= symbol for a mirror
plane
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2 D SYMMETRY
We now have 6 unique 2-D symmetry
operations:
1 2 3 4 6 m
Rotations are congruent operations
reproductions are identical
Inversion and reflection are enantiomorphicoperations
reproductions are opposite-handed
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2-D SYMMETRY
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Combinations of symmetry elements are alsopossible
To create a complete analysis of symmetryabout a point in space, we must try all possiblecombinations of these symmetry elements
In the interest of clarity and ease of illustration,we continue to consider only 2-D examples
2 D SYMMETRY
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2-D SYMMETRY
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2 D SYMMETRY
Try combining a 2-fold rotation axis with a mirror
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2-D SYMMETRY
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2 D SYMMETRY
Try combining a 2-fold rotation axis with a mirror
Step 1: reflect
(could do either step first)
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2-D SYMMETRY
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2 D SYMMETRY
Try combining a 2-fold rotation axis with a mirror
Step 1: reflectStep 2: rotate (everything)
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2-D SYMMETRY
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2 D SYMMETRY
Try combining a 2-fold rotation axis with a mirror
Step 1: reflect
Step 2: rotate (everything)
Is that all??
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2-D SYMMETRY
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2 D SYMMETRY
Try combining a 2-fold rotation axis with a mirror
Step 1: reflect
Step 2: rotate (everything)
No! A second mirror is required
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2 D SYMMETRY
Try combining a 2-fold rotation axis with a mirror
The result is Point Group 2mm
2mm indicates 2 mirrors
The mirrors are different
(notequivalent by symmetry)
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All other combinations are either:
Incompatible
(2 + 2 cannot be done in 2-D)
Redundantwith others already tried
m + m 2mm because creates 2-fold
This is the same as 2 + m 2mm
2-D Symmetry
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2-D SYMMETRY
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2 D SYMMETRY
Now try combining a 4-fold rotation axis with a
mirror
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2-D SYMMETRY
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S
Now try combining a 4-fold rotation axis with a
mirror
Step 1: reflect
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2-D SYMMETRY
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Now try combining a 4-fold rotation axis with a
mirror
Step 1: reflect
Step 2: rotate 1
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2-D SYMMETRY
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Now try combining a 4-fold rotation axis with a
mirror
Step 1: reflect
Step 2: rotate 2
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2-D SYMMETRY
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Now try combining a 4-fold rotation axis with a
mirror
Step 1: reflect
Step 2: rotate 3
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2 D Symmetry
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2-D Symmetry
Now try combining a 4-fold rotation axis with a mirror
Any other elements?
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2-D Symmetry
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2-D SymmetryNow try combining a 4-fold rotation axis with a mirror
Yes, two more mirrors
Any other elements?
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2-D Symmetry
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2-D SymmetryNow try combining a 4-fold rotation axis with a mirror
Point group name??
Yes, two more mirrors
Any other elements?
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2-D Symmetry
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2-D SymmetryNow try combining a 4-fold rotation axis with a mirror
4mm
Point group name??
Yes, two more mirrors
Any other elements?
Why not4mmmm?
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2-D Symmetry
3-fold rotation axis with a mirror creates point group 3m
Why not 3mmm?
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2-D Symmetry
6-fold rotation axis with a mirror creates point group6mm
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2-D Symmetry
The original 6 elements plus the 4 combinationscreates 10 possible 2-D Point Groups:
1 2 3 4 6 m 2mm 3m 4mm 6mm
Any 2-D pattern of objects surrounding a pointmust conform to one of these groups
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Gabungan Rotasi dan Inversi
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(Klein & Hulburt, J R., 1993)
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Gabungan Rotasi dan Inversi
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3-D Symmetry
New 3-D SymmetryElements
4. Rotoinversion
a. 2-fold rotoinversion ( 2 )
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
b. 2-fold rotoinversion ( 2 )
Step 1: rotate 360/2
Note: this is a temporarystep, the intermediate
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3-D Symmetry
New Symmetry Elements
4. Rotoinversion
b. 2-fold rotoinversion ( 2 )
Step 1: rotate 360/2
Step 2: invert
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3-D Symmetry
New Symmetry Elements
4. Rotoinversion
b. 2-fold rotoinversion ( 2 )
The result:
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
b. 2-fold rotoinversion ( 2 )
This is the same as m, so not
a new operation
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3-D Symmetry
New Symmetry Elements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Step 1: rotate 360o/3
Again, this is a temporary
step, the intermediatemotif element does notexist in the final pattern
1
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Step 2: invert throughcenter
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Completion of the firstsequence
1
2
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Rotate another 360/3
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Invert through center
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Complete second step tocreate face 3
1
2
3
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Third step creates face 4
(3 (1) 4)
1
2
3
4
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Fourth step creates face 5(4 (2) 5)
1
2
5
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
Fifth step creates face 6
(5 (3) 6)
Sixth step returns to face 1
1
6
5
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
c. 3-fold rotoinversion ( 3 )
This is unique
1
6
5
2
3
4
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
1: Rotate 360/4
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
1: Rotate 360/4
2: Invert
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
1: Rotate 360/4
2: Invert
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
3: Rotate 360/4
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
3: Rotate 360/4
4: Invert
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
3: Rotate 360/4
4: Invert
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
5: Rotate 360/4
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
5: Rotate 360/4
6: Invert
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3 D Symmetry
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
This is also a unique operation
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3-D Symmetry
New SymmetryElements
4. Rotoinversion
d. 4-fold rotoinversion ( 4 )
A more fundamentalrepresentative of the pattern
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3-D Symmetry
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y yWe now have 8 unique 3D symmetry operations:
1 2 3 4 6 m 3 4
Combinations of these elements are also possible
A complete analysis ofsymmetry about a point in spacerequires that we try all possible combinations of thesesymmetry elements
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SYSTEM & CLASSCRYSTALOGRAPHY
To be Continue