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3 D Symmetry (2 weeks). Next we would move a step further into 3D symmetry. Leonhard Euler :. http://en.wikipedia.org/wiki/Leonhard_Euler. Google search: Euler. Spherical trigonometry. Small circle R
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3D Symmetry_1(2 weeks)
Next we would move a step further into 3D symmetry.
Leonhard Euler :
http://en.wikipedia.org/wiki/Leonhard_Euler
Google search: Euler
For convenience, set R = 1Great circle (GC), R=1
Small circleR<1
A B
Spherical trigonometry
Distance: AOB = (GC)o
Pole 90o to arc AB.OP plane defined by OAB
A B
o
P
Well defined
angle
B’POA = /2; POB = /2; POB’ = /2
A B
C
ab
c
arc BC = aarc AC = barc AB = c.
GC
Spherical Angles
A
B C
BAC = B’OC’
B’OC’
oGC
?
Trigonometry: points on a surface of a sphere (directions that intersect the sphere) are connected using arcs of great circles
OA OBOA OCOB OC
angle
Center of the sphere
C’B’
A is the pole for plane defined by B’OC’
ABC and ABC are mutually polar!
Proof: B: pole of arc AC B is 90o away from point A. C: pole of arc AB C is 90o away from point A. A:pole of arc BC. Similarly, B: AC, C: pole of arc AB.
A
B C
A
B C
Polar triangle
A, pole of arc BCB, pole of arc ACC, pole of arc AB
GC
GC
A
B
C
B
C
P
Q
Proof: BAC = , arc BC = a, + a = .
a
B : pole of arc AC arc BQ = /2 C : pole of arc AB arc CP = /2 arc BQ + arc CP = = (arc BP+ arc PQ) + (arc PQ+ arc QC) = (arc BP+ arc PQ+ arc QC) + arc PQ = a + arc PQ
A A C
o
B
QC
Why! See pictures of spherical angle in page 4 (bottom)!
= POQ =
Law of cosines
Plane Trigonometry
AB C
a
bcAbccba cos2222
How about law of cosines in spherical trigonometry?
length
angle
Triangle is defined as
C is spherical angle at point u.
vOu = awOu = bvOw = c
a, b, c
Cbaba costantan2tantan 22
cbaba cossecsec2tantan2 22 cbaba cossecsec2secsec 22
cbaCba cossecsec1costantan
Cbabac cossinsincoscoscos
u
v
w
o
yz
b
a
90o
(1)
(2)
1a
(1)
(2)
(1)= tana
1/(2)= cosa (2) = seca
1b
(3)
(4)
(3)= tanb
1/(4)= cosb (4) = secbUnit circle
(3)
(4)
http://en.wikipedia.org/wiki/Spherical_law_of_cosines
OO
u uz y
2
yz (From uyz)(From oyz)
Stop here about spherical trigonometry!
We obtain all the relations needed forfurther discussion of the 3D point groups!
Combination of two rotation operations in 3 D:
A B
1 R
2 R
3 R
C ? AB
A : (1) (2)B : (2) (3)
(1) and (3) relation?
3-D: translation, reflection, rotation, and inversion.
CAB
must be crystallographic
c
A B
c
A BcA Bc
C
Locate the position of axis C
b a A B
C
c
ab
Euler construction:
A B
M
M’
N’
N C’
C
A: AMAM’. B: BNBN’.
C (the point unmoved). OC: the axis
A symmetry element is the locus of apoint that is left unmoved by an operation.
(1) A: leave A unmoved.(2) B: move A to A’.
A B
MN’ CA’
/2 /2
ABC = A’BC = /2 AB = A’B ABC = A’BC ACB = A’CB /2
A/2B
C
/2
/2
c
ab
The law of cosine (spherical trigonometry)
2cossinsincoscoscos
babac
2cossinsincoscoscos
cbcba
CAB
A/2 B
C
/2/2
c
ab180o-a 180o-b
180o-c
180o-/2180o-/2
180o-/2
Law of cosine to the polar triangle
)180cos()2
180sin()2
180sin(
)2
180cos()2
180cos()2
180cos(
ooo
ooo
c
2sin2sin
2cos2cos2coscos
c
Polartriangle
2sin2sin
2cos2cos2coscos
c
2sin2sin
2cos2cos2coscos
a
2sin2sin
2cos2cos2coscos
b
All the rotation combinations possible in 3D that need to betested: B
A 1
1 111112113114116
2 212213214216313314
3316
2
222223224226323
326324
4 414416
6 616
3 4 6
626 636 646 666
424426
434436
444446
333
336334
Axis atA, B, or C , , or
/2/2/2
1-fold2-fold3-fold4-fold6-fold
360o
180o
120o
90o
60o
180o
90o
60o
45o
30o
-10
1/21/21/2
31/2/2
01
31/2/2 1/21/2
1/2
)2cos(
)2cos(
)2cos(
)2sin(
)2sin(
)2sin(
Case: 11n
A: 1, = 360o, cos( /2) = -1; sin( /2) = 0
A/2B
C
/2
/2
c
ab
B: 1, = 360o, cos( /2) = -1; sin( /2) = 0
C: n, = 360o /n , cos( /2); sin( /2)
A B
C
180o
180o/n
c
ab 180o
2sin2sin
2cos2cos2coscos
c
0
12coscos
c None exist! Except, = 360 o
111
Case: 22n
A: 2, = 180o, cos( /2) = 0; sin( /2) = 1A
/2B
C
/2
/2
c
ab
B: 2, = 180o, cos( /2) = 0; sin( /2) = 1
C: n, = 360o /n , cos( /2); sin( /2)
A B
C
90o
180o/n
c
ab 90o
2sin2sin
2cos2cos2coscos
c
2cos1
02coscos
c
oo ccn 90 ; 0cos ; 02/cos ; 180 ; 2 oo ccn 60 ; 2/1cos ; 2/12/cos ; 120 ; 3
oo ccn 45 ; 2/1cos ; 2/12/cos ; 90 ; 4 oo ccn 30 ; /23cos ; /232/cos ; 60 ; 6
2
c
222
223
224
226
o90c
o60c
o45c
o30c
Angle between A and B axis
AB
A Bo60
o90
A Bo45
A Bo30
C
a b
What are a and b?
0)2/sin(1
)2/cos(00
2sin2sin
2cos2cos2coscos
b
A: 2, = 180o, cos( /2) = 0; sin( /2) = 1
B: 2, = 180o, cos( /2) = 0; sin( /2) = 1
C: n, = 360o /n , cos( /2); sin( /2)
0)2/sin(1
)2/cos(00
2sin2sin
2cos2cos2coscos
a
a = 90o.
b = 90o.
30o
222
90o
223
60o
224
45o
226
AB
C
A
B
C
A
B
C
A
B
C
Case: 23n
A: 2, = 180o, cos( /2) = 0; sin( /2) = 1
B: 3, = 120o, cos( /2) = 0.5; sin( /2) = 30.5/2
C: n, = 360o /n , cos( /2); sin( /2)
A B
C
90o
360o/n
c
ab 60o
)2/3(1
)5.0(02cos
2sin2sin
2cos2cos2coscos
c
'4454 ; 3/1cos ; 2/12/cos ; 120 ; 3 oo ccn
'1635 ; 6/2cos ; 2/12/cos ; 90 ; 4 oo ccn
oo ccn 0 ; 1cos ; /232/cos ; 60 ; 6 None exist
The rest of combination does not exist!
233
234
236
3
1
2/32/3
5.05.00
2sin2sin
2cos2cos2coscos
a
Case: 233
A: 2, = 180o, cos( /2) = 0; sin( /2) = 1
B: 3, = 120o, cos( /2) = 0.5; sin( /2) = 30.5/2
C: 3, = 120o, cos( /2) = 0.5; sin( /2) =30.5/2
a = 70o32.
3
1
2/31
5.005.0
2sin2sin
2cos2cos2coscos
b
b = 54o44.
70o32’
54o44’
54o44’ 233x
y
z
000
]111[]111[
]100[A
B
C
Angle between A and B is
'44543
1coscos311]111[]100[ occc
Angle between A and C is'4454
3
1coscos311]111[]100[ obbb
Angle between B and C is'3270
3
1coscos331]111[]111[ obbb
3
1
)2/1(2/3
)2/1(5.00
2sin2sin
2cos2cos2coscos
a
Case: 234
A: 2, = 180o, cos( /2) = 0; sin( /2) = 1
B: 3, = 120o, cos( /2) = 0.5; sin( /2) = 30.5/2
C: 4, = 90o, cos( /2) = 1/20.5; sin( /2) = 1/20.5
a = 54o44.
2
2
2/11
)2/1(05.0
2sin2sin
2cos2cos2coscos
b
b = 45o.
54o44’
234
45o
35o16’
x
y
z
000
]111[
]110[
]100[
AB
C
Angle between A and B is'1635
6
2coscos322]111[]110[ occc
Angle between A and C isobbb 45
2
1coscos121]100[]110[
Angle between B and C is'4454
3
1coscos131]100[]111[ obbb
Geometry of the permissible nontrivial combination of rotations:
Combination 2A = 2B = 2C = c a b
222223224226233234
180o
180o
180o
180o
180o
180o
90o
60o
45o
30o
54o4435o16
180o
180o
180o
180o
120o
120o
180o
120o
90o
60o
120o
90o
90o
90o
90o
90o
54o4445o
90o
90o
90o
90o
70o3254o44
222
International symbol
322
32(2)
Just like 3m(m)Only one independent
2 fold rotation axis
422
(1)(2)
(3)
(1) (2)
(3)
622
22 operation is basicallyon the plane!
Schonllies notation: T
n22 222 32(2) 422 622 Dn D2 D3 D4 D6
dihedral
233
Tetrahedral
Schonllies notation
different dihedral angleA
2/3C 2/3B
A
2/3B
23 is enough to specify the symmetry!
23
=
International symbol
http://en.wikipedia.org/wiki/Tetrahedron
54o44’
234 or 432
45o
35o16’
2
A3
2B
C
Schonllies notation: O Octahedron
International symbol
http://en.wikipedia.org/wiki/Octahedron
11 axial combinations
1 2 3 4 6222 322 422 622233 432
11 axial combinations + Extender
vertical m
n
horizontal m
n 422 horizontal
vertical diagonal for Dn, T, O
Ways to add m:
Not for Cn
Extender: v, h, d, ! (+ extender create new rotation axis!)1
1 2 3 4 6 222 32 422 622 23 432
v
h
d
1
See readingcrystal4.pdf
Cnv, Dnv
Tv, Ov
Cnh, Dnh
Th, Oh
Cni, Dni
Ti, Oi
Dnd
Td, Od
http://ocw.mit.edu/courses/materials-science-and-engineering/3-60-symmetry-structure-and-tensor-properties-of-materials-fall-2005/readings/crystal4.pdf
4
We will explain it later
m
m
1
-
m
2
2mm
-
m
2
3m
63
m
3
4mm
1 2 3 4 6 222 32
v
h
d
1
Cnv, Dnv
Tv, Ov
Cnh, Dnh
Th, Oh
Cni, Dni
Ti, Oi
Dnd
Td, Od
-
m
4
-
m
4
4
6mm
m
6
-
m
6
mmm
222
mmm
222
mmmmmm
222
m24m
23
26m
26m
m
23
Let’s look at some cases
Two fold rotation (2) + horizontal mirror (h)
1 Ah
A
hR
R
L
?: (1) (3)
at the point of intersection
1
h
A
1
hA
1 A1
A
h
h
1A
h
A h11
1
1
1
11
mA h
2
m2
}1 1{ hA hC2
A
h
(1) R(2)R
(3)L
xyz
zyx
updown
RL
RL
L
R: right-handednessL: left-handedness
2/A
h
1
R
L
mA h
42 hC4
Four fold rotation (4) + horizontal mirror (h)
updown
RL
Four fold rotation (4) + vertical mirror (v)
updownR
R
RR
L
LL
L mmA v 42
The mirror that you put in
Mirror 45o with respect to the firstmirror set
vC4
3/A
h
1hC6
mA h
63
vC6mmA v 63
Six fold rotation (6) + horizontal mirror (h)
R R
R
R R
R
Down Up
L
L
L
L
L
L
Six fold rotation (6) + vertical mirror (v)
Group symmetry elements: 12
63
32 m
A h hC3
} 1{ 3/3/3/23/2 AAAA h
Three fold rotation (3) + horizontal mirror (h)
R R
R
updown
L
L
L
(1) (1) (1) (2) (1) (3) (1) (1) (1) (2) (1) (3)
13/2A
3/23/4 AAh
13/ A
13/ ANew two step operations
Roto-inversion
3/3/ 1 AA
3/3/ 1 AA
(1)
(2)(3)
(1)R
(2)R
(3)L
A~
n~
1~
2~
3~
4~
5~
6~
7~
8~
Roto-reflection
2~
1 1~
2 6~
3 4~
4
5 3~
6 7 8~
8
Roto-inversion
A
(1)R
(2)R
(3)L
nThe one used
313/2 A
(1)
(2) (3)(4)
(5)(6)
(1) (1)(1) (2)(1) (3)(1) (4)(1) (5)(1) (6)
13/2A
3/23/4 AA
3/23/2 1 AA
3/23/4 1 AA
1
}1 1{ 3/23/23/23/2 AAAA
ihv CCC 333 3 m
3 m3
Three fold rotation (3) + vertical mirror (v)
mA v 33/2 vC3
Three fold rotation (3) + inversion ( )1
iC3
R
R RL
LL Down Up
11
down up
12
R
L
111
m
212
?2
m2 SC
You can except 414
4
(1)(2) (1) To (1) 1
(3)
(1) To (2) 2/A
(4)(1) To (3) A
(1) To (4) 2/A
4S Sphenoid (Greek word for axe)
Not tetrahedron
Equal length The rest four: equal length.
nnn 1 odd is If
R L
RL
} 1{ 2/2/ AAA
nnn 1even is If
How about ? 6 Down Up
R
L R
L
R L 6
m
3
4 is a special one that you have to add to the11 axial combination
4
Add h m
4
L
L
R
R R
R R
R R
R
R
422
L R
R L L
R R L
R L
L R
R L L R
mmm
224
+ h
4
Add m
4
L
L
R
1
Homework!
R R
R L
R L
Look at the ppt file that I send you regarding to222 + Extender (v, h, d, ) as an example!1
T 23updown
all down.
all up.
T 23Add a horizontal
mirror plane Th 32
m
Create aninversion center
inversion
RR
R L
L R
R L
L R
Crystal System
Symmetry Direction
Primary Secondary Tertiary
Triclinic None
Monoclinic [010]
Orthorhombic [100] [010] [001]
Tetragonal [001] [100]/[010] [110]
Hexagonal/Trigonal [001] [100]/[010] [120]/[1 0]
Cubic[100]/[010]/
[001] [111] [110]
1
Buerger’s book
3D crystallographic point group
2D lattices: chapter 7 (pg. 69-83)
Euler’s construction: pg. 35-43
Some combination theorems: chapter 6
Points group: pg: 59-68