'Anti symmetric' diaporamas de présentation

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F inite Element Method

F inite Element Method. for readers of all backgrounds. G. R. Liu and S. S. Quek. CHAPTER 11:. MODELLING TECHNIQUES. CONTENTS. INTRODUCTION CPU TIME ESTIMATION GEOMETRY MODELLING MESHING Mesh density Element distortion MESH COMPATIBILITY Different order of elements

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The spin-orbit interaction

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Discrete Mathematics

Discrete Mathematics. Lecture#11. Directed Graph of a Relation.

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CSRU 1100 Structures of Computer Science

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Discrete Mathematics

Discrete Mathematics. 3. MATRICES, RELATIONS, AND FUNCTIONS. Lecture 5. Dr.-Ing. Erwin Sitompul. http://zitompul.wordpress.com. Homework 4. Prove that for arbitrary sets A and B , the following set equation apply: a) A ? ( A ? B ) = A ? B b) A ? ( A ? B ) = A ? B.

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Discrete Mathematics

Discrete Mathematics. 3. MATRICES, RELATIONS, AND FUNCTIONS. Lecture 5. Dr.-Ing. Erwin Sitompul. http://zitompul.wordpress.com. Homework 4. Prove that for arbitrary sets A and B , the following set equation apply: a) A ? ( A ? B ) = A ? B b) A ? ( A ? B ) = A ? B.

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Bound States

Bound States. What is a Bound State?. Imagine a system of two bodies that interact. They can have relative movement. If this movement has sufficient energy, they will scatter and will eventually move far apart where their interaction will be negligible.

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Dates

Dates. Midterm: Nov 6 Final out Dec 4, due Dec 11 Project meetings: Oct 24, Nov 14, Nov 28 Final project presentation: Dec 12. d 0. Back to example. 1: x := ... 2: y := ... 3: y := ... 4: p := ... if(...). d 1 = F a (d 0 ). d 1. d 2 = F b (d 1 ). d 2. d 3 = F c (d 2 ). d 3.

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Dates

Dates. Midterm: Nov 6 Final out Dec 4, due Dec 11 Project meetings: Oct 24, Nov 14, Nov 28 Final project presentation: Dec 12. d 0. Back to example. 1: x := ... 2: y := ... 3: y := ... 4: p := ... if(...). d 1 = F a (d 0 ). d 1. d 2 = F b (d 1 ). d 2. d 3 = F c (d 2 ). d 3.

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SU(3) symmetry and Baryon wave functions

SU(3) symmetry and Baryon wave functions. Sedigheh Jowzaee PhD seminar- FZ Juelich, Feb 2013. Introduction. Fundamental symmetries of our universe Symmetry to the quark model: Hadron wave functions Existence (mesons) and qqq (baryons)

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Character Tables for Point Groups

Character Tables for Point Groups. Each point group has a complete set of possible symmetry operations that are conveniently listed as a matrix known as a Character Table . As an example, we will look at the character table for the C 2v point group. Point Group Label.

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Lecture 4.1: Relations Basics

Lecture 4.1: Relations Basics. CS 250, Discrete Structures, Fall 2011 Nitesh Saxena * Adopted from previous lectures by Cinda Heeren. Course Admin. Mid-Term 2 Exam How was it? Solution will be posted soon Should have the results by the coming weekend HW3 Was due yesterday

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Luminosity Tuning

Luminosity Tuning. Franz-Josef Decker 26-Oct-2006. Hints for tuning areas What tools are available besides tunes Examples for coupling and dispersion What is changing How to change a beta beat By 4 pattern tuning reveals coupling effect of parasitic crossing

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PRS Question

PRS Question. For a molecule to be stable, the following must hold Its energy should exceed the sum of the energy of its constituents Its energy should exactly equal the sum of the energy of its constituents Its energy should be less than the sum of the energy of its constituents.

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Luminosity Tuning

Luminosity Tuning. Franz-Josef Decker 26-Oct-2006. Hints for tuning areas What tools are available besides tunes Examples for coupling and dispersion What is changing How to change a beta beat By 4 pattern tuning reveals coupling effect of parasitic crossing

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Logics for Data and Knowledge Representation

Logics for Data and Knowledge Representation. Introduction to Algebra. Chiara Ghidini, Luciano Serafini, Fausto Giunchiglia and Vincenzo Maltese. Roadmap. Set theory Basic notions Operations Properties Relations Functions. Describing the world. individuals. Cita. Monkey. sets.

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Relation

Relation. Combining Relations. Because relations from A to B are subsets of A x B, two relations from A to B can be combined in any way two sets can be combined. Let A = {1, 2, 3} and B = {1, 2, 3, 4}. The relations R 1 ={(1, 1), (2, 2), (3, 3)} and

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Background material

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