MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur- 208016.

Slides:



Advertisements
Similar presentations
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Advertisements

In this section we’ll consider space groups Pm, Cm, Pc and Cc
Why Study Solid State Physics?
XRD Line Broadening With effects on Selected Area Diffraction (SAD) Patterns in a TEM MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Weak Interactions Non-Covalent Interactions MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE)
Anandh Subramaniam & Kantesh Balani
Lecture 2: Crystal Symmetry
1 Watkins/Fronczek - Space Groups Translational + Rotational Symmetry Introduction to Space Groups.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Mineralogy Carleton College Winter Lattice and its properties Lattice: An imaginary 3-D framework, that can be referenced to a network of regularly.
Symmetry Motif: the fundamental part of a symmetric design that, when repeated, creates the whole pattern Operation: some act that reproduces the.
Title How to read and understand…. Page Left system crystal system.
CRYSTALLOGRAPHY TRIVIA FINAL ROUND!. Round 3 – Question 1 Twins are said to add another level of symmetry to a crystal. Why is this?
MOHAMMAD IMRAN DEPARTMENT OF APPLIED SCIENCES JAHANGIRABAD EDUCATIONAL GROUP OF INSTITUTES.
Anandh Subramaniam & Kantesh Balani
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
PH0101 UNIT 4 LECTURE 3 CRYSTAL SYMMETRY CENTRE OF SYMMETRY
 In these set of slides we will try to visualize how constructive and destructive interference take place (using the Bragg’s view of diffraction as ‘reflection’
FASCINATING QUASICRYSTALS Based on atomic order quasicrystals are one of the 3 fundamental phases of matter MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam.
Elementary Crystallography for X-ray Diffraction
KINETICS MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur-
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
DISLOCATION STRESS FIELDS  Dislocation stress fields → infinite body  Dislocation stress fields → finite body  Image forces  Interaction between dislocations.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
2D Symmetry (1.5 weeks). From previous lecture, we know that, in 2D, there are 3 basics symmetry elements: Translation,mirror (reflection),and rotation.
Symmetry Figures are identical upon an operation Reflection Mirror Line of symmetry.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Solidification, Crystallization & Glass Transition  Cooling the Melt  solidification  Crystallization versus Formation of Glass  Parameters related.
 Constructing crystals in 1D, 2D & 3D  Understanding them using the language of:  Lattices  Symmetry LET US MAKE SOME CRYSTALS
FATIGUE Fatigue of Materials (Cambridge Solid State Science Series) S. Suresh Cambridge University Press, Cambridge (1998) MATERIALS SCIENCE &ENGINEERING.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Graphene MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur-
Anandh Subramaniam & Kantesh Balani
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
SAMPLE XRD PATTERNS MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology,
المحاضرة 4 التركيب البلوري-التماثل
Lesson 11: Adding Translation Define pure translation within a cell—centering Combine translation with other symmetry operations to produce a new operations.
Crystal Structure and Crystallography of Materials
Periodic patterns.
Point Groups Roya Majidi 1393.
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
1D, 2D, 3D…. nD Euclidian, Spherical, Hyperbolic General Riemannian
Crystal Structure and Crystallography of Materials
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
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.
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Symmetry “the correspondence in size, form and
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Crystallography.
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Presentation transcript:

MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur URL: home.iitk.ac.in/~anandh AN INTRODUCTORY E-BOOK Part of A Learner’s Guide

How do these symmetries create this lattice? (in combination with translation ‘ofcourse’! 2-fold 1 i2i2 i1i1 2-fold 2 m v2 m v1 mhmh Subscript 1  At lattice pointsSubscript 2  Between lattice points t Click to proceed

t m v1 * Note: m h cannot create the lattice starting from a point m v2 2-fold 2 i2i2 m 1 *  this is actually (m v1 + t) ! t will be applied to all these operators  else we will get no lattice! One of the 2-folds (2-fold 2 ) and one of the inversion centres (i 2 ) have been chosen for illustration

t m v1 * m v2 2-fold 2 i2i2  Only points being added to the right are shown

t m v1 * m v2 2-fold 2 i2i2

t m v1 * m v2 2-fold 2 i2i2

t m v1 * m v2 2-fold 2 i2i2  Only points being added to the right are shown  Note that only a partial lattice is created  Similarly 2-fold 1 and i 1 will create partial lattices and so forth..

Q & A

Time for some Q & A  Why do we have to invoke translation (‘ofcourse’!) to construct the lattice?  Without the translation the point will not move!  There are some symmetry operators like Glide Reflection which can create a lattice by themselves as they have translation built into themGlide Reflection Origin of the Point Groups Point Groups Symmetry operators (without translational component) acting at a point will leave a finite set of points around the point

 Many of the symmetry operators seem to produce the same effect. Then why use them?  There will always be some redundancy with respect to the effect of symmetry operators (or their combinations)  This problem is pronounced in lower dimension where many of them produce identical effects. There are no left or right handed objects in 1D hence a 2-fold, an inversion centre and a mirror all may produce the same effect. Analogy: This is like a tensor looking like a ‘vector’ in 1-D, looking like a ‘scalar’ in 0D!  Hence, when we go to higher dimensions some of the differences will become clear  If translation is doing all the job of creating a lattice, then why the symmetry operators?  As we know lattices are being used to make crystals  crystals are based on symmetry  One should note that as translation can create a lattice an array of symmetry operators can also create a lattice (this array itself can be considered a lattice or even a crystal!)  Symmetry operators are present in the lattice even if one decides to ignore themmake crystals