Crystal Morphology Remember: Space groups for atom symmetry

Slides:



Advertisements
Similar presentations
INTRODUCTION TO CERAMIC MINERALS
Advertisements

Crystallography, Crystal Symmetry, and Crystal Systems
Crystallography: Forms and Planes
It is very easy to visualize the location of a simple face given miller index, or to derive a miller index from simple faces c -b b a -c Fig
Three-Dimensional Symmetry
t1 t2 6 t1 t2 7 8 t1 t2 9 t1 t2.
Introduction to Mineralogy Dr. Tark Hamilton Chapter 6: Lecture Crystallography & External Symmetry of Minerals Camosun College GEOS 250 Lectures:
Crystal Systems GLY 4200 Fall, 2012.
Lecture 2: Crystal Symmetry
Intercepts  Intercepts measure where a crystal face hits a crystal axis. The location on the axes corresponding to unit lengths is arbitrary and chosen.
Crystal Structure Continued! NOTE!! Again, much discussion & many figures in what follows was constructed from lectures posted on the web by Prof. Beşire.
Wigner-Seitz Cell The Wigner–Seitz cell around a lattice point is defined as the locus of points in space that are closer to that lattice point than to.
Lec. (4,5) Miller Indices Z X Y (100).
© Oxford Instruments Analytical Limited 2001 MODULE 2 - Introduction to Basic Crystallography Bravais Lattices Crystal system Miller Indices Crystallographic.
Crystals and Symmetry. Why Is Symmetry Important? Identification of Materials Prediction of Atomic Structure Relation to Physical Properties –Optical.
Indicatrix Imaginary figure, but very useful
Lecture 10 (10/16/2006) Crystallography Part 3: Crystallographic Axes Numerical Notation of Crystal Faces and Atomic Planes – Miller Indices.
Lecture 11 (10/18/2006) Crystallography Part 4: Crystal Forms Twinning
Symmetry Motif: the fundamental part of a symmetric design that, when repeated, creates the whole pattern Operation: some act that reproduces the.
CRYSTALLOGRAPHY TRIVIA ROUND 2!
17-plane groups When the three symmetry elements, mirrors, rotation axis and glide planes are shown on the five nets, 17-plane groups are derived.
Rotation with Inversion (Rotoinversion) Equivalency to other symmetry operations
Crystal Chem  Crystallography Chemistry behind minerals and how they are assembled –Bonding properties and ideas governing how atoms go together –Mineral.
CRYSTALLOGRAPHY TRIVIA FINAL ROUND!. Round 3 – Question 1 Twins are said to add another level of symmetry to a crystal. Why is this?
Crystallography Gypsum Monoclinic Dolomite Triclinic Emerald Hexagonal
Crystallography Motif: the fundamental part of a symmetric design that, when repeated, creates the whole pattern In 3-D, translation defines operations.
Crystallographic Axes are imaginary reference lines which often coincide with symmetry axes or normals to symmetry planes as in symmetry axes these aid.
Practical I - A. Crystallographic axis  One of three lines (sometimes four, in the case of a hexagonal crystal), passing through a common point, that.
Symmetry Motif: the fundamental part of a symmetric design that, when repeated, creates the whole pattern Operation: some act that reproduces the.
Introduction to Crystallography
Lecture 11 Crystallography
Crystallography and Diffraction Theory and Modern Methods of Analysis Lectures 1-2 Introduction to Crystal Symmetry Dr. I. Abrahams Queen Mary University.
Solid State Physics (1) Phys3710
Chem Lattices By definition, crystals are periodic in three dimensions and the X-ray diffraction experiment must be understood in the context of.
Introduction to Crystallography and Mineral Crystal Systems PD Dr. Andrea Koschinsky Geosciences and Astrophysics.
Crystal Morphology: External Form Klein, pages Geol 3055 Prof. Merle.
CRYSTALLOGRAPHY.
Crystal Structure A “unit cell” is a subdivision of the lattice that has all the geometric characteristics of the total crystal. The simplest choice of.
W.D. Callister, Materials science and engineering an introduction, 5 th Edition, Chapter 3 MM409: Advanced engineering materials Crystallography.
Lecture 12 Crystallography
PHY1039 Properties of Matter Crystallography, Lattice Planes, Miller Indices, and X-ray Diffraction (See on-line resource: )
IMPORTANT: We list and describe all the crystal classes/minerals
Crystalline Solids :-In Crystalline Solids the atoms are arranged in some regular periodic geometrical pattern in three dimensions- long range order Eg.
Symmetry, Groups and Crystal Structures
Crystallography lv.
ESO 214: Nature and Properties of Materials
Key things to know to describe a crystal
1 Crystallographic Concepts GLY 4200 Fall, Atomic Arrangement Minerals must have a highly ordered atomic arrangement The crystal structure of.
Crystallographic Axes
Optical Mineralogy in a Nutshell Use of the petrographic microscope in three easy lessons Part III © Jane Selverstone, University of New Mexico, 2003 Used.
Basic Crystallography for X-ray Diffraction Earle Ryba.
WHY CRYSTALLORAPHY WHY CRYSTALLORAPHY? perfect order … the perfect order of particles in the space is amazing… crystals ground"as is" To think that such.
بسم الله الرحمن الرحيم بسم الله الرحمن الرحيم  أفلا تبصرون  وفي الارض آيات للموقنين  أفلا تبصرون  وفي الارض آيات للموقنين من سورة الذاريات اية 20.
Crystal morphology I Free crystallizing solids will exhibit flat, smooth faces: euhedral all faces perfectly crystallized subhedralpartially crystallized.
Crystal Structure and Crystallography of Materials
Crystal Structure and Crystallography of Materials
SOLID STATE By: Dr.DEPINDER KAUR.
SOLID STATE By: Dr.Bhawna.
Miller indices/crystal forms/space groups
Groups: Fill in this Table for Cubic Structures
Crystal Structure and Crystallography of Materials
Symmetry, Groups and Crystal Structures
Crystallographic Concepts
Crystals Crystal consist of the periodic arrangement of building blocks Each building block, called a basis, is an atom, a molecule, or a group of atoms.
Symmetry, Groups and Crystal Structures
Crystallographic Concepts
Crystallographic Concepts
MILLER PLANES Atoms form periodically arranged planes Any set of planes is characterized by: (1) their orientation in the crystal (hkl) – Miller indices.
Crystallography.
Crystal Chem  Crystallography
Presentation transcript:

Crystal Morphology Remember: Space groups for atom symmetry Point groups for crystal face symmetry Crystal Faces = limiting surfaces of growth Depends in part on shape of building units & physical cond. (T, P, matrix, nature & flow direction of solutions, etc.)

Crystal Morphology Observation: The frequency with which a given face in a crystal is observed is proportional to the density of lattice nodes along that plane

Crystal Morphology Observation: The frequency with which a given face in a crystal is observed is proportional to the density of lattice nodes along that plane

Crystal Morphology Because faces have direct relationship to the internal structure, they must have a direct and consistent angular relationship to each other

Nicholas Steno (1669): Law of Constancy of Interfacial Angles Crystal Morphology Nicholas Steno (1669): Law of Constancy of Interfacial Angles Quartz

Diff planes have diff atomic environments Crystal Morphology Diff planes have diff atomic environments A note on directional properties: H, n, thermal exp...

Crystal Morphology Crystal symmetry conforms to 32 point groups  32 crystal classes in 6 crystal systems Crystal faces act just as our homework: symmetry about the center of the crystal so the point groups and the crystal classes are the same

Crystal Morphology Crystal Axes: generally taken as parallel to the edges (intersections) of prominent crystal faces a b c

Crystal Morphology Crystal Axes: generally taken as parallel to the edges (intersections) of prominent crystal faces The more faces the better  prism faces & quartz c-axis, halite cube, etc. We must also keep symmetry in mind: c = 6-fold in hexagonal With x-ray crystallography we can determine the internal structure and the unit cell directly and accurately The crystallographic axes determined by XRD and by the face method nearly always coincide This is not coincidence!!

How do we keep track of the faces of a crystal? Crystal Morphology How do we keep track of the faces of a crystal?

Crystal Morphology How do we keep track of the faces of a crystal? Remember, face sizes may vary, but angles can't Note: “interfacial angle” = the angle between the faces measured like this

Crystal Morphology How do we keep track of the faces of a crystal? Remember, face sizes may vary, but angles can't Thus it's the orientation & angles that are the best source of our indexing Miller Index is the accepted indexing method It uses the relative intercepts of the face in question with the crystal axes

Given the following crystal: Crystal Morphology Given the following crystal: 2-D view looking down c b a b a c

Given the following crystal: Crystal Morphology Given the following crystal: a b How reference faces? a face? b face? -a and -b faces?

Crystal Morphology Suppose we get another crystal of the same mineral with 2 other sets of faces: How do we reference them? b w x y b a a z

Miller Index uses the relative intercepts of the faces with the axes Pick a reference face that intersects both axes Which one? b b w x x y y a a z

Either x or y. The choice is arbitrary. Just pick one. Which one? Either x or y. The choice is arbitrary. Just pick one. Suppose we pick x b a w x y z b x y a

MI process is very structured (“cook book”) a b c unknown face (y) 1 1  reference face (x) 2 1 1 b a x y invert 2 1  clear of fractions 2 1 Miller index of face y using x as the a-b reference face (2 1 0)

What is the Miller Index of the reference face? a b c unknown face (x) 1 1  reference face (x) 1 1 1 b a x y invert 1  clear of fractions 1 Miller index of the reference face is always 1 - 1 (1 1 0) (2 1 0)

What if we pick y as the reference. What is the MI of x? a b c unknown face (x) 2 1  reference face (y) 1 1 1 b a x y invert 1 2  clear of fractions 1 2 Miller index of the reference face is always 1 - 1 (1 2 0) (1 1 0)

Which choice is correct? 1) x = (1 1 0) y = (2 1 0) 2) x = (1 2 0) y = (1 1 0) b a x y The choice is arbitrary What is the difference?

What is the difference? axial ratio = a/b = 0.80 y unit cell shape if y = (1 1 0) unit cell shape if x = (1 1 0) b b a a x b y a axial ratio = a/b = 0.80 axial ratio = a/b = 1.60

The technique above requires that we graph each face A simpler (?) way is to use trigonometry Measure the interfacial angles b a x y b a w x y z 148o ? ? interfacial angles 141o

The technique above requires that we graph each face A simpler (?) way is to use trigonometry b a x y b a w x y z tan 39 = a/b = 0.801 tan 58 = a/b = 1.600 58o 148o 39o 141o

What are the Miller Indices of all the faces if we choose x as the reference? Face Z? b a w (1 1 0) (2 1 0) z

1 The Miller Indices of face z using x as the reference a b c 1 ¥ ¥ 1 unknown face (z) 1 ¥ ¥ reference face (x) 1 1 1 invert 1 ¥ b w (1 1 0) clear of fractions 1 (2 1 0) Miller index of face z using x (or any face) as the reference face (1 0 0) a z

b Can you index the rest? (1 1 0) (2 1 0) (1 0 0) a

b (0 1 0) (1 1 0) (1 1 0) (2 1 0) (2 1 0) (1 0 0) a (1 0 0) (2 1 0) (2 1 0) (1 1 0) (1 1 0) (0 1 0)

Miller index of face XYZ using ABC as the reference face 3-D Miller Indices (an unusually complex example) a b c c unknown face (XYZ) 2 2 2 reference face (ABC) 1 4 3 C invert 1 2 4 3 Z clear of fractions (1 3) 4 Miller index of face XYZ using ABC as the reference face O A X Y B a b

Demonstrate MI on cardboard cube model

We can get the a:b:c axial ratios from the chosen (111) face We can also determine the true unit cell by XRD and of course determine the a:b:c axial ratios from it If the unit face is correctly selected, the ratios should be the same If not, will be off by some multiple - i.e. picked (211) and called it (111) Best to change it Mineralogy texts listed axial ratios long before XRD We had to change some after XRD developed

Form = a set of symmetrically equivalent faces braces indicate a form {210} b (0 1) (1 1) (1 1) (2 1) (2 1) (1 0) a (1 0) (2 1) (2 1) (1 1) (1 1) (0 1)

Form = a set of symmetrically equivalent faces braces indicate a form {210} Multiplicity of a form depends on symmetry {100} in monoclinic, orthorhombic, tetragonal, isometric

Form = a set of symmetrically equivalent faces braces indicate a form {210} F. 2.36 in your text (p. 49-52) pinacoid prism pyramid dipryamid related by a mirror or a 2-fold axis related by n-fold axis or mirrors

Form = a set of symmetrically equivalent faces braces indicate a form {210} Quartz = 2 forms: Hexagonal prism (m = 6) Hexagonal dipyramid (m = 12)

Isometric forms include Cube Octahedron Dodecahedron 111 _ __ 110 101 011 _

Octahedron to Cube to Dodecahedron Click on image to run animation

All three combined:

Zone Any group of faces || a common axis Use of h k l as variables for a, b, c intercepts (h k 0) = [001] If the MI’s of 2 non-parallel faces are added, the result = MI of a face between them & in the same zone

BUT doesn't say which face (100) Which?? (010) (110)?

BUT doesn't say which face (100) (010) (210) (110) (100) Which?? (010) (110)? (100) (010) (110) (120) Either is OK