Wednesday, April 12. Today:

Similar documents
Crystallographic Point Groups and Space Groups

Demonstration of the Coupled Evolution Rules 163 APPENDIX F: DEMONSTRATION OF THE COUPLED EVOLUTION RULES

Fair Divsion in Theory and Practice

( ) R kj. = y k y j. y A ( ) z A. y a. z a. Derivatives of the second order electrostatic tensor with respect to the translation of ( ) δ yβ.

Symmetry in 2D. 4/24/2013 L. Viciu AC II Symmetry in 2D

Lecture Note on Crystal structures Masatsugu Sei Suzuki and Itsuko S. Suzuki Department of Physics, SUNY at Binghamton (Date: February 03, 2012)

SPACE GROUPS. International Tables for Crystallography, Volume A: Space-group Symmetry. Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain

13. LECTURE 13. Objectives

Lecture course on crystallography, 2015 Lecture 9: Space groups and International Tables for Crystallography

LOWELL WEEKLY JOURNAL

INTERNATIONAL SCHOOL ON FUNDAMENTAL CRYSTALLOGRAPHY

EJL R Sβ. sum. General objective: Reduce the complexity of the analysis by exploiting symmetry. Garth J. Simpson

SUPPLEMENTARY INFORMATION

Chemical Crystallography

character table, determine the reducible representation and irreducible components for the σ-bonding SALCs.

A DARK GREY P O N T, with a Switch Tail, and a small Star on the Forehead. Any

We need to be able to describe planes and directions.

Crystal Structure. Dr Bindu Krishnan

X-ray analysis. 1. Basic crystallography 2. Basic diffraction physics 3. Experimental methods

5 Symmetries and point group in a nut shell

PX-CBMSO Course (2) of Symmetry

Phys 460 Describing and Classifying Crystal Lattices

Crystallography Reading: Warren, Chapters 2.1, 2.2, 2.6, 8 Surface symmetry: Can be a clue to underlying structure. Examples:

Neatest and Promptest Manner. E d i t u r ami rul)lihher. FOIt THE CIIILDIIES'. Trifles.

Levi s Commutator Theorems for Cancellative Semigroups

SPACE GROUPS AND SYMMETRY

Introduction to Solid State Physics or the study of physical properties of matter in a solid phase

Translational symmetry, point and space groups in solids

Tables of crystallographic properties of double antisymmetry space groups

THE FIVE TYPES OF PLANAR 2-D LATTICES. (d) (e)

Crystallographic Symmetry. Jeremy Karl Cockcroft

UNIT I SOLID STATE PHYSICS

Protein Structure Determination. Part 1 -- X-ray Crystallography

Phys 412 Solid State Physics. Lecturer: Réka Albert

Condensed Matter Physics April, 8, LUMS School of Science and Engineering

DIFFRACTION METHODS IN MATERIAL SCIENCE. PD Dr. Nikolay Zotov Lecture 4_2

Basic Crystallography Part 1. Theory and Practice of X-ray Crystal Structure Determination

Symmetry Crystallography

Unit IV State of stress in Three Dimensions

Solid State Theory Physics 545

Crystallographic structure Physical vs Chemical bonding in solids

Tim Hughbanks CHEMISTRY 634. Two Covers. Required Books, etc.

1/2, 1/2,1/2, is the center of a cube. Induces of lattice directions and crystal planes (a) Directions in a crystal Directions in a crystal are

MANY BILLS OF CONCERN TO PUBLIC

Categories, Functors, Natural Transformations

Overview - Macromolecular Crystallography

Procedure for obtaining microscopic mechanisms of reconstructive phase transitions in crystalline solids

There are 230 spacespace-groups!

Realizations of Loops and Groups defined by short identities

The structure of liquids and glasses. The lattice and unit cell in 1D. The structure of crystalline materials. Describing condensed phase structures

Multivariable Calculus and Matrix Algebra-Summer 2017

OWELL WEEKLY JOURNAL

Raman and IR spectroscopy in materials science. Symmetry analysis of normal phonon modes Boriana Mihailova

Model sets, Meyer sets and quasicrystals

Resolution of Ambiguities and the Discovery of

Suggested Reading. Pages in Engler and Randle

Review of Last Class 1

Lecture 8. Stress Strain in Multi-dimension

Part IV Multiferroic RMnO 3. Ferroelectric & magnetic ordering SHG spectroscopy SHG topography Identification of multiferroic interactions

Mathematics 222a Quiz 2 CODE 111 November 21, 2002

Solid State Physics 460- Lecture 5 Diffraction and the Reciprocal Lattice Continued (Kittel Ch. 2)

Space groups. Bernd Souvignier

Group theory applied to crystallography

Nove fizickohemijske metode. Ivana Radosavljevic Evans Durham University, UK

IOAN ŞERDEAN, DANIEL SITARU

The least element is 0000, the greatest element is 1111.

Fundamentals of X-ray diffraction

TILES, TILES, TILES, TILES, TILES, TILES

Introduction to crystallography The unitcell The resiprocal space and unitcell Braggs law Structure factor F hkl and atomic scattering factor f zθ

n-dimensional, infinite, periodic array of points, each of which has identical surroundings.

Second-harmonic generation in nonpolar chiral materials: relationship between molecular and macroscopic properties

WALLPAPER GROUPS. Julija Zavadlav

Introduction to Condensed Matter Physics

... 3, , = a (1) 3 3 a 2 = a (2) The reciprocal lattice vectors are defined by the condition a b = 2πδ ij, which gives

Unit 3 Factors & Products

What is a Quasicrystal?

Practice Problems Set II

CSE 167: Introduction to Computer Graphics Lecture #2: Linear Algebra Primer

Introduction to mathematical quasicrystals

Crystals Statics. Structural Properties. Geometry of lattices. Aug 23, 2018

Physical Chemistry I. Crystal Structure

Chapter 7: Exponents

ISOTROPY. Tutorial. July 2013

GROUP THEORY AND THE 2 2 RUBIK S CUBE

Chem 728 Introduction to Solid Surfaces

CSE 167: Introduction to Computer Graphics Lecture #2: Linear Algebra Primer

Chapter 1. Crystal structure. 1.1 Crystal lattices

CSIR - Algebra Problems

Bulk Structures of Crystals

arxiv: v1 [math.ra] 3 Oct 2009

Symmetry. PlayMath, Summer, 2018

LESSON 7.1 FACTORING POLYNOMIALS I

Contents. 1 Introduction 2. 2 Unique and extraordinary properties 2. 3 Equations derived from the model of a particle in a box 4

ACCEPTS HUGE FLORAL KEY TO LOWELL. Mrs, Walter Laid to Rest Yesterday

Fundamentals. Crystal patterns and crystal structures. Lattices, their symmetry and related basic concepts

Classification of algebras with minimal quadratic growth of identities

Landau & Lifshits, Quantum Mechanics, Ch. 12. Tinkham, Group Theory and Quantum Mechanics

- A general combined symmetry operation, can be symbolized by β t. (SEITZ operator)

The Law of Averages. MARK FLANAGAN School of Electrical, Electronic and Communications Engineering University College Dublin

NIELINIOWA OPTYKA MOLEKULARNA

Transcription:

Wednesday, April 2 Last Time: - The solid state - atomic arrangement in solids - why do solids form: energetics - Lattices, translations, rotation, & other symmetry operations Today: Continue with lattices, translations, rotation, & other symmetry operations Describing solid structures Crystal lattice types Crystal structures & properties Locations, directions, & planes Readings: Chang & Thoman: Chapter 8 Solid state reading (posted on Blackboard) Reminders: Spectroscopy assignment due Friday Chemistry Senior Symposium: Tuesday, April 25, CC MR5, 0:30 2 and 4

3-D Structure

20 Nobel Prize in Chemistry "for the discovery of quasicrystals Daniel Shechtman Technion Israel Institute of Technology Haifa, Israel Images from nobelprize.org Figure 7. Pentagonal Penrose tiling. Note the local 5-fold symmetry that even in the absence of any tran

Rectangular 2mm p2mm Patterson symmetry p2mm p 2 mm No. 6 p3m 3m Hexagonal No. 5 p3m Patterson symmetry p6mm Origin at 2mm Asymmetric unit 0 x 2; 0 y 2 Symmetry operations () (2) 2 0,0 (3) m 0,y (4) m x,0 Generators selected (); t(,0); t(0,); (2); (3) Positions Multiplicity, Wyckoff letter, Site symmetry Coordinates Reflection conditions General: 4 i () x,y (2) x,ȳ (3) x,y (4) x,ȳ no conditions 2 h. m. 2,y 2,ȳ 2 g. m. 0,y 0,ȳ 2 f..m x, 2 x, 2 2 e..m x,0 x,0 d 2 mm 2, 2 c 2 mm 2,0 b 2 mm 0, 2 a 2 mm 0,0 Maximal non-isomorphic subgroups I [2] pm(pm,3) ; 3 [2] pm (pm,3) ; 4 [2] p2(p2, 2) ; 2 IIa none IIb [2] p2mg(a = 2a)(7);[2]p2gm(b = 2b)(p2mg,7);[2]c2mm(a = 2a,b = 2b)(9) Maximal isomorphic subgroups of lowest index IIc [2] p2mm(a = 2a or b = 2b)(6) Minimal non-isomorphic supergroups I [2] p4mm() II [2] c2mm(9) Special: Origin at 3m Asymmetric unit 0 x 2 3; 0 y 2; x ( + y)/2; y min( x,x) Vertices 0,0 2,0 2 3, 3 2, 2 Symmetry operations () (2) 3 + 0,0 (3) 3 0,0 (4) m x,x (5) m x,0 (6) m 0,y Generators selected (); t(,0); t(0,); (2); (4) Positions Multiplicity, Wyckoff letter, Site symmetry Coordinates 6 d () x,y (2) ȳ,x y (3) x + y, x (4) y,x (5) x y,ȳ (6) x, x + y 3 c..m x,0 0,x x, x 2 b 3.. 3, 2 3 a 3. m 0,0 2 3, 3 Maximal non-isomorphic subgroups I [2] p3(p3, 3) ; 2; 3 { [3] pm (cm,5) ; 4 [3] pm (cm,5) ; 5 [3] pm (cm,5) ; 6 IIa none IIb [3] h3m (a = 3a,b = 3b)(p3m, 4) Maximal isomorphic subgroups of lowest index IIc [4] p3m (a = 2a,b = 2b)(5) Minimal non-isomorphic supergroups I [2] p6mm(7) II [3] h3m (p3m, 4) Reflection conditions General: no conditions Special:

M.C. Escher p3m Reflection Crystallography (2006). Vol. A, Plane group 5, p. 06. 3m p3m Patterson sym x 2 3; 0 y 2; x ( + y)/2; y min( x,x) 2, 3 2, 2

4 Bravais Lattices P Primitive F Face-centered I Body-centered A, B, or C Side-centered R Rhombohedral

32 Crystallographic Point Groups

Pm 3m O h m 3m Cubic No. 22 P 4/m 3 2/m Patterson symmetry Pm 3m CONTINUED No. 22 Pm 3m Generators selected (); t(,0,0); t(0,,0); t(0,0,); (2); (3); (5); (3); (25) Positions Multiplicity, Wyckoff letter, Site symmetry Coordinates 48 n () x,y,z (2) x,ȳ,z (3) x,y, z (4) x,ȳ, z (5) z,x,y (6) z, x,ȳ (7) z, x,y (8) z,x,ȳ (9) y,z,x (0) ȳ,z, x () y, z, x (2) ȳ, z,x (3) y,x, z (4) ȳ, x, z (5) y, x,z (6) ȳ,x,z (7) x,z,ȳ (8) x,z,y (9) x, z,ȳ (20) x, z,y (2) z,y, x (22) z,ȳ,x (23) z,y,x (24) z,ȳ, x (25) x,ȳ, z (26) x,y, z (27) x,ȳ,z (28) x,y,z (29) z, x,ȳ (30) z,x,y (3) z,x,ȳ (32) z, x,y (33) ȳ, z, x (34) y, z,x (35) ȳ,z,x (36) y,z, x (37) ȳ, x,z (38) y,x,z (39) ȳ,x, z (40) y, x, z (4) x, z,y (42) x, z,ȳ (43) x,z,y (44) x,z,ȳ (45) z,ȳ,x (46) z,y, x (47) z,ȳ, x (48) z,y,x 24 m..m x,x,z x, x,z x,x, z x, x, z z,x,x z, x, x z, x,x z,x, x x,z,x x,z, x x, z, x x, z,x x,x, z x, x, z x, x,z x,x,z x,z, x x,z,x x, z, x x, z,x z,x, x z, x,x z,x,x z, x, x Reflection conditions h,k,l permutable General: no conditions Special: 24 l m.. 2,y,z 2,ȳ,z 2,y, z 2,ȳ, z z, 2,y z, 2,ȳ z, 2,y z, 2,ȳ y,z, 2 ȳ,z, 2 y, z, 2 ȳ, z, 2 y, 2, z ȳ, 2, z y, 2,z ȳ, 2,z 2,z,ȳ 2,z,y 2, z,ȳ 2, z,y z,y, 2 z,ȳ, 2 z,y, 2 z,ȳ, 2 24 k m.. 0,y,z 0,ȳ,z 0,y, z 0,ȳ, z z,0,y z,0,ȳ z,0,y z,0,ȳ y,z,0 ȳ,z,0 y, z,0 ȳ, z,0 y,0, z ȳ,0, z y,0,z ȳ,0,z 0,z,ȳ 0,z,y 0, z,ȳ 0, z,y z,y,0 z,ȳ,0 z,y,0 z,ȳ,0 2 j m. m2 2,y,y 2,ȳ,y 2,y,ȳ 2,ȳ,ȳ y, 2,y y, 2,ȳ ȳ, 2,y ȳ, 2,ȳ y,y, 2 ȳ,y, 2 y,ȳ, 2 ȳ,ȳ, 2 2 i m. m2 0,y,y 0,ȳ,y 0,y,ȳ 0,ȳ,ȳ y,0,y y,0,ȳ ȳ,0,y ȳ,0,ȳ y,y,0 ȳ,y,0 y,ȳ,0 ȳ,ȳ,0 2 h mm2.. x, 2,0 x, 2,0 0,x, 2 0, x, 2 2,0,x 2,0, x 2,x,0 2, x,0 x,0, 2 x,0, 2 0, 2, x 0, 2,x 8 g. 3 m x,x,x x, x,x x,x, x x, x, x x,x, x x, x, x x, x,x x,x,x 6 f 4 m.m x, 2, 2 x, 2, 2 2,x, 2 2, x, 2 2, 2,x 2, 2, x 6 e 4 m.m x,0,0 x,0,0 0,x,0 0, x,0 0,0,x 0,0, x 3 d 4/mm.m 2,0,0 0, 2,0 0,0, 2 3 c 4/mm.m 0, 2, 2 2,0, 2 2, 2,0 Origin at centre (m 3m) Asymmetric unit 0 x 2; 0 y 2; 0 z 2; y x; z y Vertices 0,0,0 2,0,0 2, 2,0 2, 2, 2 Symmetry operations (given on page 674) b m 3 m 2, 2, 2 a m 3 m 0,0,0 Symmetry of special projections Along [00] p4mm Along [] p6mm a = a b = b a = 3(2a b c) b = 3( a + 2b c) Origin at 0,0,z Origin at x,x,x Along [0] p2mm a = 2( a + b) b = c Origin at x,x,0

Im 3m O 9 h m 3m Cubic CONTINUED No. 229 Im 3m No. 229 I 4/m 3 2/m Patterson symmetry Im 3m Generators selected (); t(,0,0); t(0,,0); t(0,0,); t( 2, 2, 2); (2); (3); (5); (3); (25) Positions Multiplicity, Wyckoff letter, Site symmetry Coordinates (0,0,0)+ ( 2, 2, 2)+ 96 l () x,y,z (2) x,ȳ,z (3) x,y, z (4) x,ȳ, z (5) z,x,y (6) z, x,ȳ (7) z, x,y (8) z,x,ȳ (9) y,z,x (0) ȳ,z, x () y, z, x (2) ȳ, z,x (3) y,x, z (4) ȳ, x, z (5) y, x,z (6) ȳ,x,z (7) x,z,ȳ (8) x,z,y (9) x, z,ȳ (20) x, z,y (2) z,y, x (22) z,ȳ,x (23) z,y,x (24) z,ȳ, x (25) x,ȳ, z (26) x,y, z (27) x,ȳ,z (28) x,y,z (29) z, x,ȳ (30) z,x,y (3) z,x,ȳ (32) z, x,y (33) ȳ, z, x (34) y, z,x (35) ȳ,z,x (36) y,z, x (37) ȳ, x,z (38) y,x,z (39) ȳ,x, z (40) y, x, z (4) x, z,y (42) x, z,ȳ (43) x,z,y (44) x,z,ȳ (45) z,ȳ,x (46) z,y, x (47) z,ȳ, x (48) z,y,x 48 k..m x,x,z x, x,z x,x, z x, x, z z,x,x z, x, x z, x,x z,x, x x,z,x x,z, x x, z, x x, z,x x,x, z x, x, z x, x,z x,x,z x,z, x x,z,x x, z, x x, z,x z,x, x z, x,x z,x,x z, x, x 48 j m.. 0,y,z 0,ȳ,z 0,y, z 0,ȳ, z z,0,y z,0,ȳ z,0,y z,0,ȳ y,z,0 ȳ,z,0 y, z,0 ȳ, z,0 y,0, z ȳ,0, z y,0,z ȳ,0,z 0,z,ȳ 0,z,y 0, z,ȳ 0, z,y z,y,0 z,ȳ,0 z,y,0 z,ȳ,0 48 i..2 4,y,ȳ + 2 3 4,ȳ,ȳ + 2 3 4,y,y + 2 4,ȳ,y + 2 ȳ + 2, 4,y ȳ + 2, 3 4,ȳ y+ 2, 3 4,y y+ 2, 4,ȳ Reflection conditions h,k,l permutable General: hkl : h + k + l = 2n 0kl : k + l = 2n hhl : l = 2n h00 : h = 2n Special: as above, plus y,ȳ + 2, 4 ȳ,ȳ + 2, 3 4 y,y + 2, 3 4 ȳ,y + 2, 4 3 4,ȳ,y + 2 4,y,y + 2 4,ȳ,ȳ + 2 3 4,y,ȳ + 2 y + 2, 3 4,ȳ y+ 2, 4,y ȳ + 2, 4,ȳ ȳ + 2, 3 4,y ȳ,y + 2, 3 4 y,y + 2, 4 ȳ,ȳ + 2, 4 y,ȳ + 2, 3 4 24 h m. m2 0,y,y 0,ȳ,y 0,y,ȳ 0,ȳ,ȳ y,0,y y,0,ȳ ȳ,0,y ȳ,0,ȳ y,y,0 ȳ,y,0 y,ȳ,0 ȳ,ȳ,0 24 g mm2.. x,0, 2 x,0, 2 2,x,0 2, x,0 0, 2,x 0, 2, x 0,x, 2 0, x, 2 x, 2,0 x, 2,0 2,0, x 2,0,x 6 f. 3 m x,x,x x, x,x x,x, x x, x, x x,x, x x, x, x x, x,x x,x,x 2 e 4 m.m x,0,0 x,0,0 0,x,0 0, x,0 0,0,x 0,0, x 2 d 4 m.2 4,0, 2 8 c. 3 m 4, 4, 4 6 b 4/mm.m 0, 2, 2 3 4,0, 2 3 4, 3 4, 4 2,0, 2 2, 4,0 2, 3 4,0 0, 2, 4 0, 2, 3 4 3 4, 4, 3 4 4, 3 4, 3 4 hkl : k,l = 2n 2, 2,0 noextraconditions 2 a m 3 m 0,0,0 Symmetry of special projections Along [00] p4mm a = 2(a b) b = 2(a + b) Origin at 0,0,z Along [] p6mm a = 3(2a b c) b = 3( a + 2b c) Origin at x,x,x Along [0] p2mm a = 2( a + b) b = 2c Origin at x,x,0 Origin at centre (m 3m) 73 Asymmetric unit 0 x 2; 0 y 2; 0 z 4; y x; z min( 2 x,y) Vertices 0,0,0 2,0,0 2, 2,0 4, 4, 4 Symmetry operations (given on page 74)

Fm 3m O 5 h m 3m Cubic No. 225 F 4/m 3 2/m Patterson symmetry Fm 3m CONTINUED No. 225 Fm 3m Generators selected (); t(,0,0); t(0,,0); t(0,0,); t(0, 2, 2); t( 2,0, 2); (2); (3); (5); (3); (25) Positions Multiplicity, Wyckoff letter, Site symmetry Coordinates (0,0,0)+ (0, 2, 2)+ ( 2,0, 2)+ ( 2, 2,0)+ 92 l () x,y,z (2) x,ȳ,z (3) x,y, z (4) x,ȳ, z (5) z,x,y (6) z, x,ȳ (7) z, x,y (8) z,x,ȳ (9) y,z,x (0) ȳ,z, x () y, z, x (2) ȳ, z,x (3) y,x, z (4) ȳ, x, z (5) y, x,z (6) ȳ,x,z (7) x,z,ȳ (8) x,z,y (9) x, z,ȳ (20) x, z,y (2) z,y, x (22) z,ȳ,x (23) z,y,x (24) z,ȳ, x (25) x,ȳ, z (26) x,y, z (27) x,ȳ,z (28) x,y,z (29) z, x,ȳ (30) z,x,y (3) z,x,ȳ (32) z, x,y (33) ȳ, z, x (34) y, z,x (35) ȳ,z,x (36) y,z, x (37) ȳ, x,z (38) y,x,z (39) ȳ,x, z (40) y, x, z (4) x, z,y (42) x, z,ȳ (43) x,z,y (44) x,z,ȳ (45) z,ȳ,x (46) z,y, x (47) z,ȳ, x (48) z,y,x 96 k..m x,x,z x, x,z x,x, z x, x, z z,x,x z, x, x z, x,x z,x, x x,z,x x,z, x x, z, x x, z,x x,x, z x, x, z x, x,z x,x,z x,z, x x,z,x x, z, x x, z,x z,x, x z, x,x z,x,x z, x, x 96 j m.. 0,y,z 0,ȳ,z 0,y, z 0,ȳ, z z,0,y z,0,ȳ z,0,y z,0,ȳ y,z,0 ȳ,z,0 y, z,0 ȳ, z,0 y,0, z ȳ,0, z y,0,z ȳ,0,z 0,z,ȳ 0,z,y 0, z,ȳ 0, z,y z,y,0 z,ȳ,0 z,y,0 z,ȳ,0 48 i m. m2 2,y,y 2,ȳ,y 2,y,ȳ 2,ȳ,ȳ y, 2,y y, 2,ȳ ȳ, 2,y ȳ, 2,ȳ y,y, 2 ȳ,y, 2 y,ȳ, 2 ȳ,ȳ, 2 48 h m. m2 0,y,y 0,ȳ,y 0,y,ȳ 0,ȳ,ȳ y,0,y y,0,ȳ ȳ,0,y ȳ,0,ȳ y,y,0 ȳ,y,0 y,ȳ,0 ȳ,ȳ,0 Reflection conditions h,k,l permutable General: hkl : h+k,h+l,k+l = 2n 0kl : k,l = 2n hhl : h + l = 2n h00 : h = 2n Special: as above, plus 48 g 2. mm x, 4, 4 x, 3 4, 4 4,x, 4 4, x, 3 4 4,x, 3 4 3 4, x, 3 4 x, 4, 3 4 x, 4, 4 32 f. 3 m x,x,x x, x,x x,x, x x, x, x x,x, x x, x, x x, x,x x,x,x 4, 3 4,x 4, 4, x 4, 4, x 4, 3 4,x hkl : h = 2n 24 e 4 m.m x,0,0 x,0,0 0,x,0 0, x,0 0,0,x 0,0, x 24 d m. mm 0, 4, 4 0, 3 4, 4 8 c 43m 4, 4, 4 4,0, 4 4,0, 3 4 4, 3 4,0 4, 4,0 hkl : h = 2n 4, 4, 3 4 hkl : h = 2n 4 b m 3 m 2, 2, 2 4 a m 3 m 0,0,0 Symmetry of special projections Along [00] p4mm Along [] p6mm a = 2a b = 2b a = 6(2a b c) b = 6( a + 2b c) Origin at 0,0,z Origin at x,x,x Along [0] c2mm a = 2( a + b) b = c Origin at x,x,0 Origin at centre (m 3m) Asymmetric unit 0 x 2; 0 y 4; 0 z 4; y min(x, 2 x); z y Vertices 0,0,0 2,0,0 4, 4,0 4, 4, 4 Symmetry operations (given on page 69)

Body-centered cubic

Face-centered cubic

Mechanical Behavior Material Crystal Structure Modulus (GPa) Yield Strength (MPa) Tensile Strength (MPa) Percent Elongation (%) Aluminum FCC 68 80 250 34 Gold FCC - - 20 30 Nickel FCC 207 59 37 30 Magnesium HCP 45 83 50 2 Fe-C (Steel) BCC 200 600 750 7