Slide 1 Macquarie University 20041 The Heat Equation and Diffusion PHYS220 2004 by Lesa Moore DEPARTMENT OF PHYSICS Slide 2 Macquarie University 20042 Diffusion of Heat The…

Slide 1 Structure-Property Relationship Discotic Liquid Crystals M. Manickam School of Chemistry The University of Birmingham [email protected] CHM3T1 Lecture-3 Slide…

Slide 1 13.1. Period 3: Oxides and Chlorides IB Chem HL http://www.chemguide.co.uk/inorganic/period3/chlorides.h tml Slide 2 Sites http://martinbrakkeibchem.escuelacampoalegre.wikispaces.net/file/view/T13D01+-+10.31.11+-…

Slide 1 The particle method for simulation of self-organization phenomena Rafał Sienkiewicz Gdansk University of Technology, Gdańsk, Poland 1 Slide 2 The DigiHive environment…

Analyzing Kleinberg’s (and other) Small-world Models Chip Martel and Van Nguyen Computer Science Department; University of California at Davis Contents Part I: An introduction…

QCD-2004 Lesson 3 :Non-perturbative Simple quantities: masses and decay constants Sistematic errors 3) Semileptonic decays 4) Non leptonic decays Guido Martinelli Bejing…

Slide 1 The quantum kicked rotator First approach to âQuantum Chaosâ: take a system that is classically chaotic and quantize it. Classical kicked rotator One parameter…

Graphene Production and Future Use: An Investigation Into the Materials Application as a Hydrogen Gas Sensor Graphene Production and Future Use: An Investigation Into the…

Bonding Bonding Why Bonding? Some atoms are very reluctant to combine with other atoms and exist in the air around us as single atoms. These are the Noble Gases and have…

Slide 1 The quantum kicked rotator First approach to âQuantum Chaosâ: take a system that is classically chaotic and quantize it. Classical kicked rotator One parameter…