1 / 10

MATERIALS SCIENCE & ENGINEERING

MATERIALS SCIENCE & ENGINEERING. Part of. A Learner’s Guide. AN INTRODUCTORY E-BOOK. Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur- 208016 Email: anandh@iitk.ac.in, URL: home.iitk.ac.in/~anandh.

grandstaff
Download Presentation

MATERIALS SCIENCE & ENGINEERING

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. MATERIALS SCIENCE & ENGINEERING Part of A Learner’s Guide AN INTRODUCTORY E-BOOK Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur- 208016 Email:anandh@iitk.ac.in, URL:home.iitk.ac.in/~anandh http://home.iitk.ac.in/~anandh/E-book.htm

  2. How do these symmetries create this lattice? (in combination with translation ‘ofcourse’! t mh 2-fold2 i1 2-fold1 mv1 mv2 i2 Subscript 1  At lattice points Subscript 2  Between lattice points Click to proceed

  3. One of the 2-folds (2-fold2) and one of the inversion centres (i2) have been chosen for illustration t mv1* mv2 2-fold2 i2 Note: mh cannot create the lattice starting from a point m1*  this is actually (mv1 + t) ! t will be applied to all these operators  else we will get no lattice!

  4. Only points being added to the right are shown t mv1* mv2 2-fold2 i2

  5. t mv1* mv2 2-fold2 i2

  6. t mv1* mv2 2-fold2 i2

  7. t • Only points being added to the right are shown • Note that only a partial lattice is created • Similarly 2-fold1 and i1 will create partial lattices mv1* mv2 2-fold2 i2 and so forth..

  8. Q & A

  9. 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 them Origin of the Point Groups Symmetry operators (without translational component) acting at a point will leave a finite set of points around the point

  10. 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 them

More Related