The basics of structural biology. And Why we use synchrotron sources Sean McSweeney ESRF Structural Biology Group

Size: px
Start display at page:

Download "The basics of structural biology. And Why we use synchrotron sources Sean McSweeney ESRF Structural Biology Group"

Transcription

1 The basics of structural biology And Why we use synchrotron sources Sean McSweeney ESRF Structural Biology Group

2 The rise and rise of structural biology. 2

3 The aim of the game 3

4 What information does structure give you? 3-D view of macromolecules at near atomic resolution. The result of a successful structural project is a structure or model of the macromolecule in the crystal. You can assign: - secondary structure elements - position and conformation of side chains - position of ligands, inhibitors, metals etc. A model allows you: - to understand biochemical and genetic data (i.e., structural basis of functional changes in mutant or modified macromolecule). - generate hypotheses regarding the roles of particular residues or domains

5 A Problem to be resolved. A single molecule is a very weak scatterer of X-rays. Most of the X-rays will pass through the molecule without being diffracted. Those rays which are diffracted are too weak to be detected. Solution: Analyzing diffraction from crystals instead of single molecules. A crystal is made of a three-dimensional repeat of ordered molecules (1014) whose signals reinforce each other. The resulting diffracted rays are strong enough to be detected. A Crystal 3D repeating lattice; Unit cell is the smallest unit of the lattice; Come in all shapes and sizes. Crystals come from slowly precipitating the biological molecule out of solution under conditions that will not damage or denature it (sometimes).

6 A Birds eye view. 6

7 The Grenoble Site 7

8 Origins and evolution EVOLUTION First observation of synchrotron First particle radiation at accelerators General Electric (USA) First observation of synchrotron radiation More and more energetic particles, Bigger and bigger machines Although first considered as a nuisance by particle physicists, synchrotron radiation has now been fully recognised as having exceptional properties to explore matter Construction of the first dedicated machines Particle physics Synchrotron radiation 8

9 What is synchrotron radiation? The light produced when electrons travelling at the speed of light are forced to accelerate. For a long time considered a problem for particle accelerators - heat load. Early users (1970s) were parasitic users of the machines s saw the construction of dedicated machines to use the synchrotron light. Currently we are working at 3rd generation synchrotron sources. 9

10 To make a synchrotron Create (lots of) electrons Accelerate the electrons. Store the electrons. Use the light 10

11 To see the invisible Due to increasingly powerful methods, smaller and smaller structures can be seen. Electrons Colliders Synchrotron light X-rays House Neutrons Molecule/Atom Cell Nucleus/quark Electromagnetic waves Radio waves IR Visible light UV Soft X-rays Hard X-rays Gamma rays 11

12 Insertion devices Bending magnet Bending magnet 2 Wiggler Wiggler Brilliance 2 2 (photons/s/mm /mrad /0.1%BW ) Undulator 3 Undulator Electrons Energy (kev) 12

13 The reality 13

14 Experimental Facilities at the ESRF. Experimental facilities are distributed around the storage ring. Scientific areas served are wide spread Physics, materials science, biology, medicine, chemistry. Academic and Industrial research is supported. 14

15 Exploitation of the light for Biology. Changes of scales (resolution) Changes of experimental techniques. Changes of scientific discipline. Imaging Medicine Structural Biology. Pharmaceutical Research. 15

16 X-rays interact with matter. key ideas to keep in mind X-rays penetrate matter. Shorter wavelengths penetrate more. X-rays interact with individual atoms. Matter scatters X-rays. 16

17 Structural biology beamlines. 17

18 Beam lines produce intense beams of light. 18

19 nair X-ray microscopes nair nglass Lenses require a difference in refractive index between the air and lens material in order to 'bend' and redirect light (or any other form of electromagnetic radiation.) The refractive index for x-rays is almost exactly 1.00 for all materials. There are no lenses for xrays.

20 Fourier transformations Scattering = Fourier Transform of specimen Lens applies a second Fourier Transform to the scattered rays to give the image Since X-rays cannot be focused by lenses and refractive index of X-rays in all materials is very close to 1.0 how do we get an atomic image? Mark Rould 2007

21 X-ray Diffraction with The Fourier Duck The molecule Images by Kevin Cowtan The diffraction pattern

22 Animal Magic The diffraction pattern Images by Kevin Cowtan The CAT (molecule)

23 Choose the wavelength to fit the experiment. 23

24 The process of structure determination. 24

25 What is our job? 25

26 In practise the experiment can be tricky. 26

27 Resolution of diffraction limits precision of interpretation. 27

28 Protein Structure Determination is difficult... Hemoglobin and myglobin were amongst the first protein structures determined. Perutz and Kendrew took > 20 years to elucidate these structures. 28

29 Complexity has increased dramatically. 29

30 Complex multicomponent systems form biological systems. 30

31 Commonality and diversity of kinases evolution and drug specificity. 31

32 Data Collection from micro crystals is challenging. 32

33 Structural and functional biology. The crystals available become smaller and smaller, whilst the proteins studied get bigger This is resulting in more screening of samples and more challenging phasing experiments Understanding the underlying biology implies many more experiments to be performed. Automation is Powering this > 160,000 samples tested on MX beamlines in % led to data collections. Order of magnitude increase in samples screens is expected once the automation really takes off. F Brueckner et-al Science, 315, ,

34 Future of structural biology is in Automation. 34

35 Automation of software processes. 35

36 Automation of sample evaluation. 36

37 Thank you for you attention. 37

38 Prototype robotics in action. 38

Synchrotron Methods in Nanomaterials Research

Synchrotron Methods in Nanomaterials Research Synchrotron Methods in Nanomaterials Research Marcel MiGLiERiNi Slovak University of Technology in Bratislava and Centre for Nanomaterials Research, Olomouc marcel.miglierini@stuba.sk www.nuc.elf.stuba.sk/bruno

More information

Introduction to Synchrotron Radiation

Introduction to Synchrotron Radiation Introduction to Synchrotron Radiation Frederico Alves Lima Centro Nacional de Pesquisa em Energia e Materiais - CNPEM Laboratório Nacional de Luz Síncrotron - LNLS International School on Laser-Beam Interactions

More information

RADIATION SOURCES AT SIBERIA-2 STORAGE RING

RADIATION SOURCES AT SIBERIA-2 STORAGE RING RADIATION SOURCES AT SIBERIA-2 STORAGE RING V.N. Korchuganov, N.Yu. Svechnikov, N.V. Smolyakov, S.I. Tomin RRC «Kurchatov Institute», Moscow, Russia Kurchatov Center Synchrotron Radiation undulator undulator

More information

object objective lens eyepiece lens

object objective lens eyepiece lens Advancing Physics G495 June 2015 SET #1 ANSWERS Field and Particle Pictures Seeing with electrons The compound optical microscope Q1. Before attempting this question it may be helpful to review ray diagram

More information

SAXS and SANS facilities and experimental practice. Clement Blanchet

SAXS and SANS facilities and experimental practice. Clement Blanchet SAXS and SANS facilities and experimental practice Clement Blanchet SAS experiment Detector X-ray or neutron Beam Sample 2 s Buffer X-rays Roengten, 1895 Electromagnetic wave The electromagnetic spectrum

More information

Research with Synchrotron Radiation. Part I

Research with Synchrotron Radiation. Part I Research with Synchrotron Radiation Part I Ralf Röhlsberger Generation and properties of synchrotron radiation Radiation sources at DESY Synchrotron Radiation Sources at DESY DORIS III 38 beamlines XFEL

More information

Synchrotron Radiation in IRAN

Synchrotron Radiation in IRAN Synchrotron Radiation in IRAN Helmut Wiedemann, Stanford University Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 1 Synchrotron Radiation is the tool of choice to study atomic

More information

3. Synchrotrons. Synchrotron Basics

3. Synchrotrons. Synchrotron Basics 1 3. Synchrotrons Synchrotron Basics What you will learn about 2 Overview of a Synchrotron Source Losing & Replenishing Electrons Storage Ring and Magnetic Lattice Synchrotron Radiation Flux, Brilliance

More information

First propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division

First propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division First propositions of a lattice for the future upgrade of SOLEIL A. Nadji On behalf of the Accelerators and Engineering Division 1 SOLEIL : A 3 rd generation synchrotron light source 29 beamlines operational

More information

Insertion Devices Lecture 2 Wigglers and Undulators. Jim Clarke ASTeC Daresbury Laboratory

Insertion Devices Lecture 2 Wigglers and Undulators. Jim Clarke ASTeC Daresbury Laboratory Insertion Devices Lecture 2 Wigglers and Undulators Jim Clarke ASTeC Daresbury Laboratory Summary from Lecture #1 Synchrotron Radiation is emitted by accelerated charged particles The combination of Lorentz

More information

Light Source I. Takashi TANAKA (RIKEN SPring-8 Center) Cheiron 2012: Light Source I

Light Source I. Takashi TANAKA (RIKEN SPring-8 Center) Cheiron 2012: Light Source I Light Source I Takashi TANAKA (RIKEN SPring-8 Center) Light Source I Light Source II CONTENTS Introduction Fundamentals of Light and SR Overview of SR Light Source Characteristics of SR (1) Characteristics

More information

Name Class Date. What two models do scientists use to describe light? What is the electromagnetic spectrum? How can electromagnetic waves be used?

Name Class Date. What two models do scientists use to describe light? What is the electromagnetic spectrum? How can electromagnetic waves be used? CHAPTER 16 12 SECTION Sound and Light The Nature of Light KEY IDEAS As you read this section, keep these questions in mind: What two models do scientists use to describe light? What is the electromagnetic

More information

Which of the following can be used to calculate the resistive force acting on the brick? D (Total for Question = 1 mark)

Which of the following can be used to calculate the resistive force acting on the brick? D (Total for Question = 1 mark) 1 A brick of mass 5.0 kg falls through water with an acceleration of 0.90 m s 2. Which of the following can be used to calculate the resistive force acting on the brick? A 5.0 (0.90 9.81) B 5.0 (0.90 +

More information

JSPS Asien Science Seminar Synchrotron Radiation Science

JSPS Asien Science Seminar Synchrotron Radiation Science SESAME Synchrotron Light for Experimental Science and Applications in the Middle East JSPS Asien Science Seminar Synchrotron Radiation Science Dieter Einfeld Amman, October 2002 Introduction Based on the

More information

4.2 Properties of Visible Light Date: (pages )

4.2 Properties of Visible Light Date: (pages ) 4.2 Properties of Visible Light Date: (pages 144-149) Visible light is a mixture of all the colours of the rainbow. A prism refracts light separating the colours. A second prism can recombine the colours

More information

A2. Light Source. ( i ) Units of light intensity

A2. Light Source. ( i ) Units of light intensity A2. Light Source The important prerequisite for the success of a radiation eperiment is to properly understand the properties of each type of light source. The present document is part of the "SPring-8

More information

Electromagnetic Waves. Electromagnetic Spectrum. Electromagnetic Spectrum. Electromagnetic Waves. CH 27-Physics (B) Fall, 2010

Electromagnetic Waves. Electromagnetic Spectrum. Electromagnetic Spectrum. Electromagnetic Waves. CH 27-Physics (B) Fall, 2010 Electromagnetic Waves Electromagnetic Spectrum CH 27-Physics (B) Fall, 2010 Electric and magnetic fields always exist When ever one is. the other is The fields can exist in a... They are at. o to each

More information

Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to it, the particle radiates

Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to it, the particle radiates Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to it, the particle radiates energy according to Maxwell equations. A non-relativistic

More information

Chapter 10: Wave Properties of Particles

Chapter 10: Wave Properties of Particles Chapter 10: Wave Properties of Particles Particles such as electrons may demonstrate wave properties under certain conditions. The electron microscope uses these properties to produce magnified images

More information

The Light of Your Life. We can see the universe because atoms emit photons

The Light of Your Life. We can see the universe because atoms emit photons The Light of Your Life We can see the universe because atoms emit photons Astronomy is an observational science Our messengers are Light (electromagnetic waves) Gravitational waves Cosmic rays (particles)

More information

Biological Small Angle X-ray Scattering (SAXS) Dec 2, 2013

Biological Small Angle X-ray Scattering (SAXS) Dec 2, 2013 Biological Small Angle X-ray Scattering (SAXS) Dec 2, 2013 Structural Biology Shape Dynamic Light Scattering Electron Microscopy Small Angle X-ray Scattering Cryo-Electron Microscopy Wide Angle X- ray

More information

SECTION 3 & 4 LIGHT WAVES & INFORMATION TRANSFER

SECTION 3 & 4 LIGHT WAVES & INFORMATION TRANSFER SECTION 3 & 4 LIGHT WAVES & INFORMATION TRANSFER Light Waves Light is a type of energy that travels as waves. Light is different than other waves because it does not need matter to travel. Light waves

More information

PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. II - Synchrotron Radiation - Malcolm J. Cooper

PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. II - Synchrotron Radiation - Malcolm J. Cooper SYNCHROTRON RADIATION Malcolm J. Cooper University of Warwick, Coventry, UK Keywords: Accelerator, storage ring, X-rays, insertion devices, X-ray optics, diffraction, crystallography, X-ray spectroscopy,

More information

Advanced Storage Photon Ring Source Upgrade Project:

Advanced Storage Photon Ring Source Upgrade Project: Advanced Storage Photon Ring Source Upgrade Project: The Shielding World s for Leading the Hard X-ray Light Source Advanced Photon Source - Upgrade Bradley J. Micklich Radiation Physicist Argonne National

More information

Introduction to electron and photon beam physics. Zhirong Huang SLAC and Stanford University

Introduction to electron and photon beam physics. Zhirong Huang SLAC and Stanford University Introduction to electron and photon beam physics Zhirong Huang SLAC and Stanford University August 03, 2015 Lecture Plan Electron beams (1.5 hrs) Photon or radiation beams (1 hr) References: 1. J. D. Jackson,

More information

Characteristics and Properties of Synchrotron Radiation

Characteristics and Properties of Synchrotron Radiation Characteristics and Properties of Synchrotron Radiation Giorgio Margaritondo Vice-président pour les affaires académiques Ecole Polytechnique Fédérale de Lausanne (EPFL) Outline: How to build an excellent

More information

Collecting Macromolecular Crystallographic Data at Synchrotrons. Andrew Howard ACA Summer School 12 July 2007

Collecting Macromolecular Crystallographic Data at Synchrotrons. Andrew Howard ACA Summer School 12 July 2007 Collecting Macromolecular Crystallographic Data at Synchrotrons Andrew Howard ACA Summer School 12 July 2007 Synchrotrons are useful, not just fashionable You can do almost any experiment better and faster

More information

PARTICLE BEAMS, TOOLS FOR MODERN SCIENCE AND MEDICINE Hans-H. Braun, CERN

PARTICLE BEAMS, TOOLS FOR MODERN SCIENCE AND MEDICINE Hans-H. Braun, CERN 5 th Particle Physics Workshop National Centre for Physics Quaid-i-Azam University Campus, Islamabad PARTICLE BEAMS, TOOLS FOR MODERN SCIENCE AND MEDICINE Hans-H. Braun, CERN 2 nd Lecture Examples of Modern

More information

Physics 201. Professor P. Q. Hung. 311B, Physics Building. Physics 201 p. 1/3

Physics 201. Professor P. Q. Hung. 311B, Physics Building. Physics 201 p. 1/3 Physics 201 p. 1/3 Physics 201 Professor P. Q. Hung 311B, Physics Building Physics 201 p. 2/3 What are electromagnetic waves? Electromagnetic waves consist of electric fields and magnetic fields which

More information

ADVANCED ANALYTICAL LABORATORY

ADVANCED ANALYTICAL LABORATORY An Information Brochure on ADVANCED ANALYTICAL LABORATORY ANDHRA UNIVERSITY Visakhapatnam - 530 003 Andhra Pradesh, India Sponsored by DEPARTMENT OF SCIENCE & TECHNOLOGY Government of India New Delhi 110016

More information

Telescopes (Chapter 6)

Telescopes (Chapter 6) Telescopes (Chapter 6) Based on Chapter 6 This material will be useful for understanding Chapters 7 and 10 on Our planetary system and Jovian planet systems Chapter 5 on Light will be useful for understanding

More information

Detection: from the Dark Ages to the X-ray Detectors for future SR and FEL Photon Sources

Detection: from the Dark Ages to the X-ray Detectors for future SR and FEL Photon Sources Detection: from the Dark Ages to the X-ray Detectors for future SR and FEL Photon Sources Michael Krisch Head of Instrumentation Services and Development Division European Synchrotron Radiation Facility

More information

3. The very long ones are called waves, and the very short ones are called waves.

3. The very long ones are called waves, and the very short ones are called waves. NASA Mission: Science Introduction to the Electromagnetic Spectrum Web Quest Directions: Load the following website which will discuss the electromagnetic spectrum in detail. http://missionscience.nasa.gov/ems/01_intro.html

More information

Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to this acceleration, the

Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to this acceleration, the Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to this acceleration, the particle radiates energy according to Maxwell equations.

More information

Photochemical principles

Photochemical principles Chapter 1 Photochemical principles Dr. Suzan A. Khayyat 1 Photochemistry Photochemistry is concerned with the absorption, excitation and emission of photons by atoms, atomic ions, molecules, molecular

More information

Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY

Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY Yvonne Bergmann, Klaus Ott Helmholtz- Zentrum Berlin BESSY II Radiation Protection Department yvonne.bergmann@helmholtz-berlin.de

More information

Electromagnetic Waves

Electromagnetic Waves 4/15/12 Chapter 26: Properties of Light Field Induction Ok, so a changing magnetic field causes a current (Faraday s law) Why do we have currents in the first place? electric fields of the charges Changing

More information

Free Electron Laser. Project report: Synchrotron radiation. Sadaf Jamil Rana

Free Electron Laser. Project report: Synchrotron radiation. Sadaf Jamil Rana Free Electron Laser Project report: Synchrotron radiation By Sadaf Jamil Rana History of Free-Electron Laser (FEL) The FEL is the result of many years of theoretical and experimental work on the generation

More information

Abstract. 1. Introduction

Abstract. 1. Introduction The New Upgrade of SESAME D.Einfeld1, R.H.Sarraf2, M.Attal3, H.Hashemi4, A.Elsisi5, A.Amro6, H.Hassanzadegan4, K.Tavakoli3, B.Kalantari7, S. Varnasery8, E. Al-Dmour8, D. Foudeh6, H.Tarawneh9, A.Aladwan7

More information

Review of Future European Synchrotron Radiation Projects

Review of Future European Synchrotron Radiation Projects Review of Future European Synchrotron Radiation Projects Lenny Rivkin Paul Scherrer Institute, Villigen, Switzerland Abstract The future European synchrotron radiation projects offer a wide and bright

More information

Comparison of the brilliance limit between MAX IV 3 GeV ring and NSLS II low beta straights using the same undulator technique

Comparison of the brilliance limit between MAX IV 3 GeV ring and NSLS II low beta straights using the same undulator technique Comparison of the brilliance limit between 3 GeV ring and low beta straights using the same undulator technique Erik Wallén Thu 10 Nov 2011 22:18:57 Contents Contents 1 1 Introduction 2 2 Undulator technique

More information

Imaging & Microscopy

Imaging & Microscopy Coherent X-ray X Imaging & Microscopy => Opportunities Using a Diffraction-Limited Energy Recovery Linac (ERL) Synchrotron Source Q. Shen D. Bilderback, K.D. Finkelstein, E. Fontes, & S. Gruner Cornell

More information

ELECTROMAGNETIC WAVES

ELECTROMAGNETIC WAVES UNIT V ELECTROMAGNETIC WAVES Weightage Marks : 03 Displacement current, electromagnetic waves and their characteristics (qualitative ideas only). Transverse nature of electromagnetic waves. Electromagnetic

More information

Introduction to Accelerator Physics Part 1

Introduction to Accelerator Physics Part 1 Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 28th July 2014 Pedro Castro / MPY Accelerator Physics 28 th July 2014

More information

X-Ray Nanoimaging: Instruments And Methods II (Proceedings Of SPIE)

X-Ray Nanoimaging: Instruments And Methods II (Proceedings Of SPIE) X-Ray Nanoimaging: Instruments And Methods II (Proceedings Of SPIE) If you are searched for a book X-Ray Nanoimaging: Instruments and Methods II (Proceedings of SPIE) in pdf form, then you've come to the

More information

OVERVIEW OF THE ADVANCED PHOTO&&~E (APS)* Marion M. White, Argonne National Laboratory, Argonne, IL, USA I. INTRODUCTION

OVERVIEW OF THE ADVANCED PHOTO&&~E (APS)* Marion M. White, Argonne National Laboratory, Argonne, IL, USA I. INTRODUCTION OVERVIEW OF THE ADVANCED PHOTO&&~E (APS)* Marion M White, Argonne National Laboratory, Argonne, IL, 60439 USA Abstract The Advanced Photon Source (APS)is a state-of-theart synchrotronlight source facility

More information

There and back again A short trip to Fourier Space. Janet Vonck 23 April 2014

There and back again A short trip to Fourier Space. Janet Vonck 23 April 2014 There and back again A short trip to Fourier Space Janet Vonck 23 April 2014 Where can I find a Fourier Transform? Fourier Transforms are ubiquitous in structural biology: X-ray diffraction Spectroscopy

More information

Protein crystallography. Garry Taylor

Protein crystallography. Garry Taylor Protein crystallography Garry Taylor X-ray Crystallography - the Basics Grow crystals Collect X-ray data Determine phases Calculate ρ-map Interpret map Refine coordinates Do the biology. Nitrogen at -180

More information

The Electromagnetic Spectrum

The Electromagnetic Spectrum The Electromagnetic Spectrum Learning Objectives! What is Electromagnetic Radiation?! What are spectra? How could we measure a spectrum?! How do wavelengths correspond to colors for optical light? Does

More information

Light and Matter(LC)

Light and Matter(LC) Light and Matter(LC) Every astronomy book that I ve seen has at least one chapter dedicated to the physics of light. Why are astronomers so interested in light? Everything* that we know about Astronomical

More information

NSRRC Current Status and the TPS Project

NSRRC Current Status and the TPS Project NSRRC Current Status and the TPS Project Chien-Te Chen July 21, 2005 1-1 Milestones 1981 Dec. Feasibility study began 1983 Jul. SRRC Project approved by the government 1986 Mar. Preparatory Office of SRRC

More information

Applications of scattering theory! From the structure of the proton! to protein structure!

Applications of scattering theory! From the structure of the proton! to protein structure! Applications of scattering theory From the structure of the proton to protein structure Nicuşor Tîmneanu 2016 Contents and goals What is scattering and why study it? How is the structure of matter determined?

More information

Unit 5 Lesson 1 Images from Space. Copyright Houghton Mifflin Harcourt Publishing Company

Unit 5 Lesson 1 Images from Space. Copyright Houghton Mifflin Harcourt Publishing Company Florida Benchmarks SC.8.N.4.2 Explain how political, social, and economic concerns can affect science, and vice versa. SC.8.E.5.10 Assess how technology is essential to science for such purposes as access

More information

Physics LESSON PLAN PERFORMANCE OBJECTIVE(S): STUDENTS WILL BE ABLE TO:

Physics LESSON PLAN PERFORMANCE OBJECTIVE(S): STUDENTS WILL BE ABLE TO: Physics LESSON PLAN Subject: Physics Grade: 7 12 Date: 6/21/2012 Concept: The wave nature of light, Estimated Time of Lesson: 100 Minutes PERFORMANCE OBJECTIVE(S): STUDENTS WILL BE ABLE TO: (1) Understand

More information

An Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney

An Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney An Introduction to Diffraction and Scattering Brendan J. Kennedy School of Chemistry The University of Sydney 1) Strong forces 2) Weak forces Types of Forces 3) Electromagnetic forces 4) Gravity Types

More information

Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 5

Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 5 Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 5 MULTIPLE CHOICE 1. What is the wavelength of the longest wavelength light visible to the human eye? a. 400 nm b. 4000 nm c. 7000 nm

More information

Radiation Protection At Synchrotron Radiation Facilities

Radiation Protection At Synchrotron Radiation Facilities 3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Radiation Protection At Synchrotron Radiation Facilities Ehsan Salimi Shielding and Radiation Safety Group

More information

Conceptual Understandings for K-2 Teachers

Conceptual Understandings for K-2 Teachers AFK12SE/NGSS Strand Disciplinary Core Ideas PS1: Matter and Its Interactions How can one explain the structure, properties, and interactions of matter? PS1. A: Structure and Properties of Matter How do

More information

Unit title: Atomic and Nuclear Physics for Spectroscopic Applications

Unit title: Atomic and Nuclear Physics for Spectroscopic Applications Unit title: Atomic and Nuclear Physics for Spectroscopic Applications Unit code: Y/601/0417 QCF level: 4 Credit value: 15 Aim This unit provides an understanding of the underlying atomic and nuclear physics

More information

Edge Radiation IR end-station at ESRF

Edge Radiation IR end-station at ESRF X-TIP Workshop Coupling of Synchrotron Radiation IR and X-rays with Tip based Scanning Probe Microscopies 16-18 November 2005 Edge Radiation IR end-station at ESRF Jean Susini European Synchrotron Radiation

More information

Lecture 1: Applications of High Power Electromagnetic Systems

Lecture 1: Applications of High Power Electromagnetic Systems Lecture 1: Applications of High Power Electromagnetic Systems Low Power (not covered in this class) + EM sensors + Radio communications and broadcast + Cellular communications High Power + High power microwaves

More information

ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM

ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM VISUAL PHYSICS ONLINE MODULE 7 NATURE OF LIGHT ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM When white light passes through a prism, it spreads out into a rainbow of colours, with red at one end and

More information

Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION

Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION CHAPTER 3 Telescopes Lecture Presentation 3.0 Imaging the universe Our original observations of the universe depended on our eyes! What other

More information

Light - electromagnetic radiation

Light - electromagnetic radiation Astronomy & Light Astronomy is a science In science we know by doing experiments When multiple experiments give the same results we develop theories and laws In astronomy many of the experiments are done

More information

Solution 3: A glass prism deviates the violet light most and the red light least.

Solution 3: A glass prism deviates the violet light most and the red light least. EXERCISE- 6 (A) Question 1: Name three factors on which the deviation produces by a prism depends and state how does it depend on the factors stated by you. Solution 1: The deviation produced by the prism

More information

Skoog Chapter 6 Introduction to Spectrometric Methods

Skoog Chapter 6 Introduction to Spectrometric Methods Skoog Chapter 6 Introduction to Spectrometric Methods General Properties of Electromagnetic Radiation (EM) Wave Properties of EM Quantum Mechanical Properties of EM Quantitative Aspects of Spectrochemical

More information

The Electromagnetic Spectrum

The Electromagnetic Spectrum The Electromagnetic Spectrum A Brief History of Light 1000 AD It was proposed that light consisted of tiny particles Newton Used this particle model to explain reflection and refraction Huygens 1678 Explained

More information

Focusing on Light What is light? Is it a particle or a wave? An age-old debate that has persisted among scientists is related to the question, "Is

Focusing on Light What is light? Is it a particle or a wave? An age-old debate that has persisted among scientists is related to the question, Is Focusing on Light What is light? Is it a particle or a wave? An age-old debate that has persisted among scientists is related to the question, "Is light a wave or a stream of particles?" Very noteworthy

More information

FCAT REVIEW Physical Science: Force and Energy

FCAT REVIEW Physical Science: Force and Energy FCAT REVIEW Physical Science: Force and Energy Force and Motion A force is a push or pull that starts, stops, or changes the direction of an object. Some examples of contact forces are gravity and friction.

More information

Scattering Lecture. February 24, 2014

Scattering Lecture. February 24, 2014 Scattering Lecture February 24, 2014 Structure Determination by Scattering Waves of radiation scattered by different objects interfere to give rise to an observable pattern! The wavelength needs to close

More information

X-Ray Damage to Biological Crystalline Samples

X-Ray Damage to Biological Crystalline Samples X-Ray Damage to Biological Crystalline Samples Gerd Rosenbaum Structural Biology Center, ANL and Dept. of Biochemistry, UGA ACA Summer School IIT, 19 July 2007 A U.S. Department of Energy laboratory managed

More information

Announcements Self-inductance. Self-inductance. RL Circuit. RL Circuit, cont 3/11/2011. Chapter (not.9-.10) τ = R. Electromagnetic Waves

Announcements Self-inductance. Self-inductance. RL Circuit. RL Circuit, cont 3/11/2011. Chapter (not.9-.10) τ = R. Electromagnetic Waves Chapter 21.8-13(not.9-.10) Electromagnetic Announcements Clicker quizzes NO LONGER GRADED! WebAssign HW Set 8 due this Friday Problems cover material from Chapters 21-22 Office hours: My office hours today

More information

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION Instructor: Kazumi Tolich Lecture 11 2 25.5 Electromagnetic waves Induced fields Properties of electromagnetic waves Polarization Energy of electromagnetic

More information

Electromagnetic Waves Properties. The electric and the magnetic field, associated with an electromagnetic wave, propagating along the z=axis. Can be represented by E = E kˆ, = iˆ E = E ˆj, = ˆj b) E =

More information

Introduction to Accelerator Physics Part 1

Introduction to Accelerator Physics Part 1 Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 27th July 2015 Pedro Castro / MPY Introduction to Accelerator Physics

More information

CHEM 681 Seminar Mingqi Zhao April 20, 1998 Room 2104, 4:00 p.m. High Resolution Transmission Electron Microscopy: theories and applications

CHEM 681 Seminar Mingqi Zhao April 20, 1998 Room 2104, 4:00 p.m. High Resolution Transmission Electron Microscopy: theories and applications CHEM 681 Seminar Mingqi Zhao April 20, 1998 Room 2104, 4:00 p.m. High Resolution Transmission Electron Microscopy: theories and applications In materials science, people are always interested in viewing

More information

Shielding Design for the Imaging and Medical Beamline at the Australian Synchrotron

Shielding Design for the Imaging and Medical Beamline at the Australian Synchrotron Shielding Design for the Imaging and Medical Beamline at the Australian Synchrotron P. Berkvens and D. Häusermann European Synchrotron Radiation Facility BP 0, Grenoble Cedex 0, France Australian Synchrotron

More information

Name Date Class _. Please turn to the section titled The Nature of Light.

Name Date Class _. Please turn to the section titled The Nature of Light. Please turn to the section titled The Nature of Light. In this section, you will learn that light has both wave and particle characteristics. You will also see that visible light is just part of a wide

More information

studies for designer materials, sustainable energy and healthy lives

studies for designer materials, sustainable energy and healthy lives Neutron and synchrotron radiaiton studies for designer materials, sustainable energy and healthy lives J. Murray Gibson Director Advanced Photon Source, Associate Laboratory Director for Photon Sciences

More information

Planetary Science: Investigations 9-10 I-Check Quiz STUDY GUIDE Name HR Date

Planetary Science: Investigations 9-10 I-Check Quiz STUDY GUIDE Name HR Date 1. How are different types of radiation arranged along the electromagnetic spectrum? A. By how fast they travel incorrect answer B. By their sources incorrect answer C. By the amount of energy they carry

More information

Shielding calculations for the design of new Beamlines at ALBA Synchrotron

Shielding calculations for the design of new Beamlines at ALBA Synchrotron Shielding calculations for the design of new Beamlines at ALBA Synchrotron A. Devienne 1, M.J. García-Fusté 1 1 Health & Safety Department, ALBA Synchrotron, Carrer de la Llum -6, 0890 Cerdanyola del Vallès,

More information

Molecular Biology Course 2006 Protein Crystallography Part I

Molecular Biology Course 2006 Protein Crystallography Part I Molecular Biology Course 2006 Protein Crystallography Part I Tim Grüne University of Göttingen Dept. of Structural Chemistry November 2006 http://shelx.uni-ac.gwdg.de tg@shelx.uni-ac.gwdg.de Overview Overview

More information

Electron Linear Accelerators & Free-Electron Lasers

Electron Linear Accelerators & Free-Electron Lasers Electron Linear Accelerators & Free-Electron Lasers Bryant Garcia Wednesday, July 13 2016. SASS Summer Seminar Bryant Garcia Linacs & FELs 1 of 24 Light Sources Why? Synchrotron Radiation discovered in

More information

f= = s = Hz m Thus (B) is the correct answer.

f= = s = Hz m Thus (B) is the correct answer. MCAT Physics Problem Solving Drill 17: Electromagnetic Radiation Question No. 1 of 10 Question 1. Violet light has a wavelength of 700 nm. What is the frequency of this radiation? Question #01 (A) 2.3

More information

X-ray Optics needs for 3 rd and 4 th generation Light Source. Mourad Idir BNL/NSLS II 1 BROOKHAVEN SCIENCE ASSOCIATES

X-ray Optics needs for 3 rd and 4 th generation Light Source. Mourad Idir BNL/NSLS II 1 BROOKHAVEN SCIENCE ASSOCIATES X-ray Optics needs for 3 rd and 4 th generation Light Source Mourad Idir midir@bnl.gov BNL/NSLS II 1 BROOKHAVEN SCIENCE ASSOCIATES OUTLINE 3 rd and 4 th generation Light source Optics needs NSLS II Example

More information

How does your eye form an Refraction

How does your eye form an Refraction Astronomical Instruments Eyes and Cameras: Everyday Light Sensors How does your eye form an image? How do we record images? How does your eye form an image? Refraction Refraction is the bending of light

More information

Lecture Outlines. Chapter 5. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

Lecture Outlines. Chapter 5. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc. Lecture Outlines Chapter 5 Astronomy Today 8th Edition Chaisson/McMillan Chapter 5 Telescopes Units of Chapter 5 5.1 Optical Telescopes 5.2 Telescope Size 5.3 Images and Detectors 5.4 High-Resolution Astronomy

More information

High Precision Alignment at the European Synchrotron Radiation Facility

High Precision Alignment at the European Synchrotron Radiation Facility High Precision Alignment at the European Synchrotron Radiation Facility David MARTIN, France Key words: metrology, precision alignment SUMMARY The European Synchrotron Radiation Facility (ESRF) is an accelerator

More information

X-Ray Scattering Studies of Thin Polymer Films

X-Ray Scattering Studies of Thin Polymer Films X-Ray Scattering Studies of Thin Polymer Films Introduction to Neutron and X-Ray Scattering Sunil K. Sinha UCSD/LANL Acknowledgements: Prof. R.Pynn( Indiana U.) Prof. M.Tolan (U. Dortmund) Wilhelm Conrad

More information

UNIVERSITY OF TECHNOLOGY Laser & Opto-Electronic Eng. Dept rd YEAR. The Electromagnetic Waves

UNIVERSITY OF TECHNOLOGY Laser & Opto-Electronic Eng. Dept rd YEAR. The Electromagnetic Waves Spectroscopy Interaction of electromagnetic radiation with matter yields that energy is absorbed or emitted by matter in discrete quantities (quanta). Measurement of the frequency or (wave length) of the

More information

Particle accelerators. Dr. Alessandro Cianchi

Particle accelerators. Dr. Alessandro Cianchi Particle accelerators Dr. Alessandro Cianchi Particle accelerators: instructions 48 hrs lectures (Wednesday 6, Friday 6 9:00) All the documentation is available via web in pdf @ http://people.roma2.infn.it/~cianchi/didattica.html

More information

SPECTRUM. Dispersion. This phenomenon can be observed in a lab environment using a

SPECTRUM. Dispersion. This phenomenon can be observed in a lab environment using a SPECTRUM Dispersion The phenomenon due to which a polychromatic light, like sunlight, splits into its component colours, when passed through a transparent medium like a glass prism, is called dispersion

More information

ZAHID IQBAL WARRAICH

ZAHID IQBAL WARRAICH Q1 Chromatography is an important analytical technique in chemistry. There is a number of techniques under the general heading of chromatography. (a) Paper and gas chromatography rely on partition to separate

More information

Physical Science DCI Progression Chart

Physical Science DCI Progression Chart DCI Progression Chart PS1: Matter and Its Interactions Grade Bands PS1.A Structure & Properties of Matter Grades K-2 Grades 3-5 Grades 6-8 Grades 9-12 Second Grade * Different kinds of matter exist and

More information

USPAS course on Recirculated and Energy Recovered Linacs Ivan Bazarov, Cornell University Geoff Krafft, JLAB. ERL as a X-ray Light Source

USPAS course on Recirculated and Energy Recovered Linacs Ivan Bazarov, Cornell University Geoff Krafft, JLAB. ERL as a X-ray Light Source USPAS course on Recirculated and Energy Recovered Linacs Ivan Bazarov, Cornell University Geoff Krafft, JLAB ERL as a X-ray Light Source Contents Introduction Light sources landscape General motivation

More information

David Martin Challenges in High Precision Beamline Alignment at the ESRF FIG Working Week Christchurch New Zealand 2016

David Martin Challenges in High Precision Beamline Alignment at the ESRF FIG Working Week Christchurch New Zealand 2016 Presented at the FIG Working Week 2016, May 2-6, 2016 in Christchurch, New Zealand David Martin Challenges in High Precision Beamline Alignment at the ESRF FIG Working Week Christchurch New Zealand 2016

More information

Protein Crystallography

Protein Crystallography Protein Crystallography Part II Tim Grüne Dept. of Structural Chemistry Prof. G. Sheldrick University of Göttingen http://shelx.uni-ac.gwdg.de tg@shelx.uni-ac.gwdg.de Overview The Reciprocal Lattice The

More information

Introduction. Chem 6850/8850 X-ray Crystallography The University of Toledo.

Introduction. Chem 6850/8850 X-ray Crystallography The University of Toledo. Introduction Chem 6850/8850 X-ray Crystallography The University of Toledo cora.lind@utoledo.edu Course Goals To develop an understanding of basic crystallographic concepts - Helpful if you ever need to

More information

Lecture 1. Introduction to X-ray Crystallography. Tuesday, February 1, 2011

Lecture 1. Introduction to X-ray Crystallography. Tuesday, February 1, 2011 Lecture 1 Introduction to X-ray Crystallography Tuesday, February 1, 2011 Protein Crystallography Crystal Structure Determination in Principle: From Crystal to Structure Dr. Susan Yates Contact Information

More information

Microscopy, Staining, and Classification

Microscopy, Staining, and Classification PowerPoint Lecture Presentations prepared by Mindy Miller-Kittrell, North Carolina State University C H A P T E R 4 Microscopy, Staining, and Classification Microscopy Light Microscopy 1) Bright-field

More information