NOESY and ROESY type experiments exploring internuclear distances

Size: px
Start display at page:

Download "NOESY and ROESY type experiments exploring internuclear distances"

Transcription

1 NOEY and ROEY type experiments explorin internuclear distances Assistant Professor Kenneth Konstad Bioanalytical Chemistry and Metabolomics Research Group ection for Natural Products and Peptides Department of Dru Desin and Pharmacoloy Faculty of Health and Medical ciences University of Copenhaen Phone: ; Fax: Bioanalytical Chemistry and Metabolomics Research Group

2 Department of Dru Desin and Pharmacoloy Lecture outline ü Nuclear Overhauser Effect (a.k.a. the NOE) ü 1D NOE experiments ü D NOE experiments Dias

3 Dias 3 Department of Dru Desin and Pharmacoloy Relaxation in a two-spin system Two-spin system with the followin characteristics and definitions: ü Nuclei ( saturated ) ü Nuclei ( insensitive/interestin ) ü Not necessarily J-coupled but miht be ü Two spectral lines ü Close enouh to interact via dipole-dipole interaction (= T 1 relaxation) R 1 r -6 (DD) = = n 1 CH! CH T 1(DD) t c

4 Dias 4 Department of Dru Desin and Pharmacoloy ntroducin the enery diaram (two spin system)

5 Department of Dru Desin and Pharmacoloy Relaxation in a two-spin system enery diaram bb ba W 0 W ab aa Dias 5 inle-, zero- and double-quantum transitions ü NOE: Peak intensity of one nucleus chanes when equilibrium population of states of another nucleus is chaned (by saturation, inversion pulse) ü Necessity: The nuclei are close in space = able to undero T 1 relaxation ( dipole-dipole coupled spins ) ü NOE is due to W 0 and W processes (cross-relaxation between dipole-dipole coupled spins)

6 ú û ù ê ë é + µ ) ( c c r W w t t [ ] ú ú û ù ê ê ë é + µ 6 0 ) ( 1 c c r W t w w t [ ] ú ú û ù ê ê ë é + + µ 6 ) ( 1 1 c c r W t w w t ú û ù ê ë é µ r W c t ú û ù ê ë é µ 6 0 r W c t ú ú û ù ê ê ë é µ 6 1 r W c t 3 1 Transition probabilities (relaxation rates) Dias 6 Department of Dru Desin and Pharmacoloy

7 Department of Dru Desin and Pharmacoloy teady state NOE bb ba W 0 W ab W 0 W aa rapidly saturated (situation immediately after saturation) W Dias 7 W 0 relaxation via W (rapidly tumblin molecules) saturated (situation after relaxation has occurred: THE NTENTY OF NCREAED!)

8 Dias 8 Department of Dru Desin and Pharmacoloy bb Maximum homonuclear NOE effect mall molecules Rapid tumblin ba W W 0 aa ab Macromolecules low tumblin

9 Department of Dru Desin and Pharmacoloy 1D NOE experiment teady-state (equilibrium) NOE: ü Lon saturation period ü Applicable to small molecules ü Positive NOE ü Difficult to use for determination of (relative) intramolecular distances because it is a result of complex kinetics involvin many neihborin spins. elective saturation Dias 9

10 Department of Dru Desin and Pharmacoloy 1D NOE experiments Transient NOE: ü elective inversion (with transient = RF pulse) rather than saturation ü Build-up curves can be constructed with increasin t m - thereby allowin measurin internuclear distances t m t Dias 10

11 Department of Dru Desin and Pharmacoloy D transient NOE experiment: NOEY t 1 t m t preparation evolution mixin detection t 1 t Dias 11

12 Dias 1 Department of Dru Desin and Pharmacoloy D transient NOE experiment: NOEY FT(F) FT(F1) preparation evolution mixin detection t 1 t

13 Dias 13 Department of Dru Desin and Pharmacoloy D transient NOE experiment: NOEY A W BA B W 0 BA B A COY B A NOEY

14 Department of Dru Desin and Pharmacoloy D transient NOE experiment: NOEY ome experimental/practical considerations: ü t m of the order of T 1 ü Receiver ain: luckily the first increment ives the larest FD intensity ü Artefacts: Antiphase cross peaks ( COY-type cross peaks ) between coupled nuclei (maximized if second and third pulse 90 ) ü Cross peaks have the same sin as diaonal (slow tumblin) or opposite (rapid tumblin). ü Processin: p/ shifted sine bell or squared sine bell in both dimensions Dias 14

15 Dias 15 Department of Dru Desin and Pharmacoloy Maximum homonuclear NOE effect No NOE = no sinals in D NOEY for lare small-molecules

16 Dias 16 Department of Dru Desin and Pharmacoloy ROEY (= CAMELPN)

17 Department of Dru Desin and Pharmacoloy ROEY (= CAMELPN) ROEY: ü Rotatin frame Overhauser Effect pectroscopy CAMELPN: ü Cross-relaxation Appropriate for Mini-molecules EmuLated by PNlockin t 1 t m t p/ spin-lock y ROE cross-peaks neative, chemical exchane positive, complications due to TOCY transfers Dias 17

18 Department of Dru Desin and Pharmacoloy D NOEY spectrum OH H 3 C O O N H Dias 18 tandard NOEY experiment at 400 MHz; t m = 600 ms

19 Dias 19 Department of Dru Desin and Pharmacoloy D NOEY experiment cross peak intensity Lare molecules Biopharmaceuticals mall molecules Natural products

20 Department of Dru Desin and Pharmacoloy Other NOE experiments - HOEY Heteronuclear Overhauser Effect pectroscopy: ü Double resonance experiment ü nterestin for other nuclei than 13 C t 1 t m t t m decouple Refocusin pulse Dias 0

21 Department of Dru Desin and Pharmacoloy Other NOE experiments - HOEY Heteronuclear Overhauser Effect pectroscopy: ü Double resonance experiment ü nterestin for other nuclei than 13 C ü pecial probe miht be needed Li N N CH 3 THF-d 8, 0 C, 400 MHz Dias 1

COSY type experiments exploring through-bond homonuclear correlations

COSY type experiments exploring through-bond homonuclear correlations COSY type experiments exploring through-bond homonuclear correlations Assistant Professor Kenneth Kongstad Bioanalytical Chemistry and Metabolomics Research Group Section for Natural Products and Peptides

More information

Lecture #6 (The NOE)

Lecture #6 (The NOE) Lecture #6 (The OE) 2/18/15 Clubb Determining Protein tructures by MR: Measure thousands of shorter inter-hydrogen atom distances. Use these to restrain the structure of protein computationally. Distance

More information

Lecture #6 (The NOE)

Lecture #6 (The NOE) Lecture #6 (The OE) 2/24/17 Clubb Determining Protein tructures by MR: Measure thousands of shorter inter-hydrogen atom distances. Use these to restrain the structure of protein computationally. Distances

More information

High-Resolutio n NMR Techniques i n Organic Chemistry TIMOTHY D W CLARIDGE

High-Resolutio n NMR Techniques i n Organic Chemistry TIMOTHY D W CLARIDGE High-Resolutio n NMR Techniques i n Organic Chemistry TIMOTHY D W CLARIDGE Foreword Preface Acknowledgements V VI I X Chapter 1. Introduction 1.1. The development of high-resolution NMR 1 1.2. Modern

More information

Spin Relaxation and NOEs BCMB/CHEM 8190

Spin Relaxation and NOEs BCMB/CHEM 8190 Spin Relaxation and NOEs BCMB/CHEM 8190 T 1, T 2 (reminder), NOE T 1 is the time constant for longitudinal relaxation - the process of re-establishing the Boltzmann distribution of the energy level populations

More information

The NMR Spectrum - 13 C. NMR Spectroscopy. Spin-Spin Coupling 13 C NMR. A comparison of two 13 C NMR Spectra. H Coupled (undecoupled) H Decoupled

The NMR Spectrum - 13 C. NMR Spectroscopy. Spin-Spin Coupling 13 C NMR. A comparison of two 13 C NMR Spectra. H Coupled (undecoupled) H Decoupled Spin-Spin oupling 13 NMR A comparison of two 13 NMR Spectra 1 oupled (undecoupled) 1 Decoupled 1 Proton Decoupled 13 NMR 6. To simplify the 13 spectrum, and to increase the intensity of the observed signals,

More information

T 1, T 2, NOE (reminder)

T 1, T 2, NOE (reminder) T 1, T 2, NOE (reminder) T 1 is the time constant for longitudinal relaxation - the process of re-establishing the Boltzmann distribution of the energy level populations of the system following perturbation

More information

THE NUCLEAR OVERHAUSER EFFECT IN STRUCTURAL AND CONFORMATIONAL ANALYSIS

THE NUCLEAR OVERHAUSER EFFECT IN STRUCTURAL AND CONFORMATIONAL ANALYSIS THE NUCLEAR OVERHAUSER EFFECT IN STRUCTURAL AND CONFORMATIONAL ANALYSIS David Neuhaus and Michael P. Williamson VCH CONTENTS Preface v Acknowledgments vii Symbols, Abbreviations, and Units xvii Introduction

More information

NMR Spectroscopy: A Quantum Phenomena

NMR Spectroscopy: A Quantum Phenomena NMR Spectroscopy: A Quantum Phenomena Pascale Legault Département de Biochimie Université de Montréal Outline 1) Energy Diagrams and Vector Diagrams 2) Simple 1D Spectra 3) Beyond Simple 1D Spectra 4)

More information

Introduction to 1D and 2D NMR Spectroscopy (4) Vector Model and Relaxations

Introduction to 1D and 2D NMR Spectroscopy (4) Vector Model and Relaxations Introduction to 1D and 2D NMR Spectroscopy (4) Vector Model and Relaxations Lecturer: Weiguo Hu 7-1428 weiguoh@polysci.umass.edu October 2009 1 Approximate Description 1: Energy level model Magnetic field

More information

Slow symmetric exchange

Slow symmetric exchange Slow symmetric exchange ϕ A k k B t A B There are three things you should notice compared with the Figure on the previous slide: 1) The lines are broader, 2) the intensities are reduced and 3) the peaks

More information

τ 1 > 1/J - if this lifetime is significantly shortened, the coupling (splitting of the signal) will not be observed

τ 1 > 1/J - if this lifetime is significantly shortened, the coupling (splitting of the signal) will not be observed It is often advantageous to reverse or remove the splitting caused by spin-spin coupling This is called spin decoupling Spin decoupling (or just decoupling) can be used for several reasons - to simplify

More information

Principles of Nuclear Magnetic Resonance in One and Two Dimensions

Principles of Nuclear Magnetic Resonance in One and Two Dimensions Principles of Nuclear Magnetic Resonance in One and Two Dimensions Richard R. Ernst, Geoffrey Bodenhausen, and Alexander Wokaun Laboratorium für Physikalische Chemie Eidgenössische Technische Hochschule

More information

4. Basic Segments of Pulse Sequences

4. Basic Segments of Pulse Sequences 4. Basic egments of Pulse equences The first applications of 2D NMR for studies of proteins in aqueous solution used only very few pulse sequences [5 7]. Today, a vast number of experimental schemes exist

More information

Spin-spin coupling I Ravinder Reddy

Spin-spin coupling I Ravinder Reddy Spin-spin coupling I Ravinder Reddy Spin-interactions External interactions Magnetic field Bo, RF field B1 Internal Interactions Molecular motions Exchange Chemical shifts J-coupling Spin Diffusion Dipolar

More information

Solid-state NMR and proteins : basic concepts (a pictorial introduction) Barth van Rossum,

Solid-state NMR and proteins : basic concepts (a pictorial introduction) Barth van Rossum, Solid-state NMR and proteins : basic concepts (a pictorial introduction) Barth van Rossum, 16.02.2009 Solid-state and solution NMR spectroscopy have many things in common Several concepts have been/will

More information

Biophysical Chemistry: NMR Spectroscopy

Biophysical Chemistry: NMR Spectroscopy Relaxation & Multidimensional Spectrocopy Vrije Universiteit Brussel 9th December 2011 Outline 1 Relaxation 2 Principles 3 Outline 1 Relaxation 2 Principles 3 Establishment of Thermal Equilibrium As previously

More information

Principios Básicos de RMN en sólidos destinado a usuarios. Gustavo Monti. Fa.M.A.F. Universidad Nacional de Córdoba Argentina

Principios Básicos de RMN en sólidos destinado a usuarios. Gustavo Monti. Fa.M.A.F. Universidad Nacional de Córdoba Argentina Principios Básicos de RMN en sólidos destinado a usuarios Gustavo Monti Fa.M.A.F. Universidad Nacional de Córdoba Argentina CONTENIDOS MODULO 2: Alta resolución en sólidos para espines 1/2 Introducción

More information

Nuclear Magnetic Resonance Spectroscopy

Nuclear Magnetic Resonance Spectroscopy Nuclear Magnetic Resonance Spectroscopy Ecole Polytechnique Département de Chimie CHI 551 Dr. Grégory Nocton Bureau 01 30 11 A Tel: 44 02 Ecole polytechnique / CNRS Laboratoire de Chimie Moléculaire E-mail:

More information

8.2 The Nuclear Overhauser Effect

8.2 The Nuclear Overhauser Effect 8.2 The Nuclear Overhauser Effect Copyright Hans J. Reich 2016 All Rights Reserved University of Wisconsin An important consequence of DD relaxation is the Nuclear Overhauser Effect, which can be used

More information

NMR NEWS June To find tutorials, links and more, visit our website

NMR NEWS June To find tutorials, links and more, visit our website Department of Chemistry NMR Facilities Director: Dr. Carlos A. Steren NMR NEWS June 2014 To find tutorials, links and more, visit our website www.chem.utk.edu/facilities/nmr Computers and software updates

More information

Spectroscopy of Polymers

Spectroscopy of Polymers Spectroscopy of Polymers Jack L. Koenig Case Western Reserve University WOMACS Professional Reference Book American Chemical Society, Washington, DC 1992 Contents Preface m xiii Theory of Polymer Characterization

More information

NMR-spectroscopy of proteins in solution. Peter Schmieder

NMR-spectroscopy of proteins in solution. Peter Schmieder NMR-spectroscopy of proteins in solution Basic aspects of NMR-Spektroskopie Basic aspects of NMR-spectroscopy 3/84 Prerequisite for NMR-spectroscopy is a nuclear spin that can be thought of as a mixture

More information

Biochemistry 530 NMR Theory and Practice

Biochemistry 530 NMR Theory and Practice Biochemistry 530 NMR Theory and Practice Gabriele Varani Department of Biochemistry and Department of Chemistry University of Washington 1D spectra contain structural information.. but is hard to extract:

More information

Introduction to Relaxation Theory James Keeler

Introduction to Relaxation Theory James Keeler EUROMAR Zürich, 24 Introduction to Relaxation Theory James Keeler University of Cambridge Department of Chemistry What is relaxation? Why might it be interesting? relaxation is the process which drives

More information

ONE AND TWO DIMENSIONAL NMR SPECTROSCOPY

ONE AND TWO DIMENSIONAL NMR SPECTROSCOPY ONE AND TWO DIMENSIONAL NMR SPECTROSCOPY Atta-ur-Rahman H.E.J. Research Institute of Chemistry, University ofkarachi, Karachi 32, Pakistan ELSEVIER Amsterdam Oxford New York Tokyo 1989 IX CONTENTS Chapter-l

More information

Nuclear Magnetic Resonance

Nuclear Magnetic Resonance Nuclear Magnetic Resonance Lectures for CCB 538 James Aramini, PhD. CABM 014A jma@cabm.rutgers.edu J.A.! 04/21/14! April 21!!!!April 23!! April 28! Outline 1. Introduction / Spectroscopy Overview! 2. NMR

More information

NMR, the vector model and the relaxation

NMR, the vector model and the relaxation NMR, the vector model and the relaxation Reading/Books: One and two dimensional NMR spectroscopy, VCH, Friebolin Spin Dynamics, Basics of NMR, Wiley, Levitt Molecular Quantum Mechanics, Oxford Univ. Press,

More information

NMR-spectroscopy in solution - an introduction. Peter Schmieder

NMR-spectroscopy in solution - an introduction. Peter Schmieder NMR-spectroscopy in solution - an introduction 2/92 Advanced Bioanalytics NMR-Spectroscopy Introductory session (11:00 12:30) Basic aspects of NMR-spectroscopy NMR parameter Multidimensional NMR-spectroscopy

More information

I690/B680 Structural Bioinformatics Spring Protein Structure Determination by NMR Spectroscopy

I690/B680 Structural Bioinformatics Spring Protein Structure Determination by NMR Spectroscopy I690/B680 Structural Bioinformatics Spring 2006 Protein Structure Determination by NMR Spectroscopy Suggested Reading (1) Van Holde, Johnson, Ho. Principles of Physical Biochemistry, 2 nd Ed., Prentice

More information

Spin Dynamics Basics of Nuclear Magnetic Resonance. Malcolm H. Levitt

Spin Dynamics Basics of Nuclear Magnetic Resonance. Malcolm H. Levitt Spin Dynamics Basics of Nuclear Magnetic Resonance Second edition Malcolm H. Levitt The University of Southampton, UK John Wiley &. Sons, Ltd Preface xxi Preface to the First Edition xxiii Introduction

More information

Classical behavior of magnetic dipole vector. P. J. Grandinetti

Classical behavior of magnetic dipole vector. P. J. Grandinetti Classical behavior of magnetic dipole vector Z μ Y X Z μ Y X Quantum behavior of magnetic dipole vector Random sample of spin 1/2 nuclei measure μ z μ z = + γ h/2 group μ z = γ h/2 group Quantum behavior

More information

NMR: PRACTICAL ASPECTS

NMR: PRACTICAL ASPECTS NMR: PRACTICAL ASPECTS Pedro M. Aguiar Sample Preparation Well prepared sample can yield high quality spectra Poorly prepared sample typically yields low quality spectra Tubes of appropriate quality Higher

More information

* 1s. --- if the sign does change it is called ungerade or u

* 1s. --- if the sign does change it is called ungerade or u Chapter Qualitative Theory of Chemical Bondin Backround: We have briefly mentioned bondin but it now time to talk about it for real. In this chapter we will delocalied orbitals and introduce Hückel MOT.

More information

Ibuprofen. Example of benchtop NMR on small organic molecules

Ibuprofen. Example of benchtop NMR on small organic molecules R Ibuprofen Example of benchtop NMR on small organic molecules Ibuprofen (C 13 H 18 O 2 ) is a non-steroidal antiinflammatory drug (NSAID) and is commonly used for pain relief, fever reduction and against

More information

Magnetic Resonance Spectroscopy

Magnetic Resonance Spectroscopy INTRODUCTION TO Magnetic Resonance Spectroscopy ESR, NMR, NQR D. N. SATHYANARAYANA Formerly, Chairman Department of Inorganic and Physical Chemistry Indian Institute of Science, Bangalore % I.K. International

More information

Carbon 13 NMR NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY

Carbon 13 NMR NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY PRINCIPLE AND APPLICATION IN STRUCTURE ELUCIDATION Carbon 13 NMR Professor S. SANKARARAMAN Department of Chemistry Indian Institute of Technology Madras Chennai

More information

Ch 14: Feedback Control systems

Ch 14: Feedback Control systems Ch 4: Feedback Control systems Part IV A is concerned with sinle loop control The followin topics are covered in chapter 4: The concept of feedback control Block diaram development Classical feedback controllers

More information

Biochemistry 530 NMR Theory and Practice

Biochemistry 530 NMR Theory and Practice Biochemistry 530 NMR Theory and Practice Gabriele Varani Department of Biochemistry and Department of Chemistry University of Washington Lecturer: Gabriele Varani Biochemistry and Chemistry Room J479 and

More information

Chem 325 NMR Intro. The Electromagnetic Spectrum. Physical properties, chemical properties, formulas Shedding real light on molecular structure:

Chem 325 NMR Intro. The Electromagnetic Spectrum. Physical properties, chemical properties, formulas Shedding real light on molecular structure: Physical properties, chemical properties, formulas Shedding real light on molecular structure: Wavelength Frequency ν Wavelength λ Frequency ν Velocity c = 2.998 10 8 m s -1 The Electromagnetic Spectrum

More information

Problem Set #6 BioE 326B/Rad 226B

Problem Set #6 BioE 326B/Rad 226B . Chemical shift anisotropy Problem Set #6 BioE 26B/Rad 226B 2. Scalar relaxation of the 2 nd kind. 0 imaging 4. NMRD curves Chemical Shift Anisotropy The Hamiltonian a single-spin system in a magnetic

More information

Polarised Nucleon Targets for Europe, 2nd meeting, Bochum 2005

Polarised Nucleon Targets for Europe, 2nd meeting, Bochum 2005 Polarised Nucleon Targets for Europe, nd meeting, Bochum Temperature dependence of nuclear spin-lattice relaxations in liquid ethanol with dissolved TEMPO radicals H. Štěpánková, J. Englich, J. Kohout,

More information

Relaxation, Multi pulse Experiments and 2D NMR

Relaxation, Multi pulse Experiments and 2D NMR Relaxation, Multi pulse Experiments and 2D NMR To Do s Read Chapter 6 Complete the end of chapter problems; 6 1, 6 2, 6 3, 6 5, 6 9 and 6 10. Read Chapter 15 and do as many problems as you can. Relaxation

More information

Chapter 7. Nuclear Magnetic Resonance Spectroscopy

Chapter 7. Nuclear Magnetic Resonance Spectroscopy Chapter 7 Nuclear Magnetic Resonance Spectroscopy I. Introduction 1924, W. Pauli proposed that certain atomic nuclei have spin and magnetic moment and exposure to magnetic field would lead to energy level

More information

PROTEIN NMR SPECTROSCOPY

PROTEIN NMR SPECTROSCOPY List of Figures List of Tables xvii xxvi 1. NMR SPECTROSCOPY 1 1.1 Introduction to NMR Spectroscopy 2 1.2 One Dimensional NMR Spectroscopy 3 1.2.1 Classical Description of NMR Spectroscopy 3 1.2.2 Nuclear

More information

Chemistry 431. Lecture 23

Chemistry 431. Lecture 23 Chemistry 431 Lecture 23 Introduction The Larmor Frequency The Bloch Equations Measuring T 1 : Inversion Recovery Measuring T 2 : the Spin Echo NC State University NMR spectroscopy The Nuclear Magnetic

More information

H B. θ = 90 o. Lecture notes Part 4: Spin-Spin Coupling. θ θ

H B. θ = 90 o. Lecture notes Part 4: Spin-Spin Coupling. θ θ Lecture notes Part 4: Spin-Spin Coupling F. olger Försterling October 4, 2011 So far, spins were regarded spins isolated from each other. owever, the magnetic moment of nuclear spins also have effect on

More information

Biochemistry 530 NMR Theory and Practice

Biochemistry 530 NMR Theory and Practice Biochemistry 530 NMR Theory and Practice David Baker Autumn Quarter 2014 Slides Courtesy of Gabriele Varani Recommended NMR Textbooks Derome, A. E. (1987) Modern NMR Techniques for Chemistry Research,

More information

1. 3-hour Open book exam. No discussion among yourselves.

1. 3-hour Open book exam. No discussion among yourselves. Lecture 13 Review 1. 3-hour Open book exam. No discussion among yourselves. 2. Simple calculations. 3. Terminologies. 4. Decriptive questions. 5. Analyze a pulse program using density matrix approach (omonuclear

More information

North Carolina State University Department of Chemistry Varian NMR Training Manual

North Carolina State University Department of Chemistry Varian NMR Training Manual North Carolina State University Department of Chemistry Varian NMR Training Manual by J.B. Clark IV & Dr. S. Sankar 1 st Edition 05/15/2009 Section 3: Glide Program Operations for Advanced 1D & 2D Spectra

More information

Direct dipolar interaction - utilization

Direct dipolar interaction - utilization Direct dipolar interaction - utilization Two main uses: I: magnetization transfer II: probing internuclear distances Direct dipolar interaction - utilization Probing internuclear distances ˆ hetero D d

More information

CHEM3023: Spins, Atoms and Molecules

CHEM3023: Spins, Atoms and Molecules CHEM3023: Spins, Atoms and Molecules Lecture 3 The Born-Oppenheimer approximation C.-K. Skylaris Learning outcomes Separate molecular Hamiltonians to electronic and nuclear parts according to the Born-Oppenheimer

More information

Experiment 3 The Simple Pendulum

Experiment 3 The Simple Pendulum PHY191 Fall003 Experiment 3: The Simple Pendulum 10/7/004 Pae 1 Suested Readin for this lab Experiment 3 The Simple Pendulum Read Taylor chapter 5. (You can skip section 5.6.IV if you aren't comfortable

More information

Spectral Broadening Mechanisms

Spectral Broadening Mechanisms Spectral Broadening Mechanisms Lorentzian broadening (Homogeneous) Gaussian broadening (Inhomogeneous, Inertial) Doppler broadening (special case for gas phase) The Fourier Transform NC State University

More information

Arthur S. Edison Department of Biochemistry & Molecular Biology

Arthur S. Edison Department of Biochemistry & Molecular Biology Theory and Applications of NMR Spectroscopy Arthur S. Edison Department of Biochemistry & Molecular Biology Summary Week 1 Notes: Introduction to the basics: Bloch equations Week 1 Homework Week 2 Notes:

More information

Principles of Magnetic Resonance

Principles of Magnetic Resonance С. Р. Slichter Principles of Magnetic Resonance Third Enlarged and Updated Edition With 185 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Contents 1. Elements of Resonance

More information

Module 20: Applications of PMR in Structural Elucidation of Simple and Complex Compounds and 2-D NMR spectroscopy

Module 20: Applications of PMR in Structural Elucidation of Simple and Complex Compounds and 2-D NMR spectroscopy Subject Chemistry Paper No and Title Module No and Title Module Tag Paper 12: Organic Spectroscopy Module 20: Applications of PMR in Structural Elucidation of Simple and Complex Compounds and 2-D NMR spectroscopy

More information

Nuclear magnetic resonance spectroscopy II. 13 C NMR. Reading: Pavia Chapter , 6.7, 6.11, 6.13

Nuclear magnetic resonance spectroscopy II. 13 C NMR. Reading: Pavia Chapter , 6.7, 6.11, 6.13 Nuclear magnetic resonance spectroscopy II. 13 NMR Reading: Pavia hapter 6.1-6.5, 6.7, 6.11, 6.13 1. General - more/better/additional structural information for larger compounds -problems: a) isotopes

More information

Kay Saalwächter and Hans W. Spiess b) Max-Planck-Institute for Polymer Research, Postfach 3148, D Mainz, Germany

Kay Saalwächter and Hans W. Spiess b) Max-Planck-Institute for Polymer Research, Postfach 3148, D Mainz, Germany JOURNAL OF CHEMICAL PHYSICS VOLUME 114, NUMBER 13 1 APRIL 2001 Heteronuclear 1 H 13 C multiple-spin correlation in solid-state nuclear magnetic resonance: Combining rotational-echo double-resonance recoupling

More information

Spectral Broadening Mechanisms. Broadening mechanisms. Lineshape functions. Spectral lifetime broadening

Spectral Broadening Mechanisms. Broadening mechanisms. Lineshape functions. Spectral lifetime broadening Spectral Broadening echanisms Lorentzian broadening (Homogeneous) Gaussian broadening (Inhomogeneous, Inertial) Doppler broadening (special case for gas phase) The Fourier Transform NC State University

More information

This relationship is known as the ideal gas law and is mathematically described with the formula below:

This relationship is known as the ideal gas law and is mathematically described with the formula below: Chemistry 20 Ideal as law If we combine all the information contained in Boyle s, Charles and Avoadro s laws, we can derive an expression that describes the temperature, pressure and volume of a as. This

More information

Your Name: Answer Key

Your Name: Answer Key Question 1. NMR Basics. (20 points) (a) Indicate schematically the magnetic moments of individual nuclear spins (at least 10) as arrows for the following situations. Assume as always that the external

More information

CONTENTS. 2 CLASSICAL DESCRIPTION 2.1 The resonance phenomenon 2.2 The vector picture for pulse EPR experiments 2.3 Relaxation and the Bloch equations

CONTENTS. 2 CLASSICAL DESCRIPTION 2.1 The resonance phenomenon 2.2 The vector picture for pulse EPR experiments 2.3 Relaxation and the Bloch equations CONTENTS Preface Acknowledgements Symbols Abbreviations 1 INTRODUCTION 1.1 Scope of pulse EPR 1.2 A short history of pulse EPR 1.3 Examples of Applications 2 CLASSICAL DESCRIPTION 2.1 The resonance phenomenon

More information

CHEM / BCMB 4190/6190/8189. Introductory NMR. Lecture 10

CHEM / BCMB 4190/6190/8189. Introductory NMR. Lecture 10 CHEM / BCMB 490/690/889 Introductory NMR Lecture 0 - - CHEM 490/690 Spin-Echo The spin-echo pulse sequence: 90 - τ - 80 - τ(echo) Spins echoes are widely used as part of larger pulse sequence to refocus

More information

Magnetic Resonance Imaging. Pål Erik Goa Associate Professor in Medical Imaging Dept. of Physics

Magnetic Resonance Imaging. Pål Erik Goa Associate Professor in Medical Imaging Dept. of Physics Magnetic Resonance Imaging Pål Erik Goa Associate Professor in Medical Imaging Dept. of Physics pal.e.goa@ntnu.no 1 Why MRI? X-ray/CT: Great for bone structures and high spatial resolution Not so great

More information

Physical Background Of Nuclear Magnetic Resonance Spectroscopy

Physical Background Of Nuclear Magnetic Resonance Spectroscopy Physical Background Of Nuclear Magnetic Resonance Spectroscopy Michael McClellan Spring 2009 Department of Physics and Physical Oceanography University of North Carolina Wilmington What is Spectroscopy?

More information

8 NMR Interactions: Dipolar Coupling

8 NMR Interactions: Dipolar Coupling 8 NMR Interactions: Dipolar Coupling 8.1 Hamiltonian As discussed in the first lecture, a nucleus with spin I 1/2 has a magnetic moment, µ, associated with it given by µ = γ L. (8.1) If two different nuclear

More information

Selective polarization transfer using a single rf field

Selective polarization transfer using a single rf field Selective polarization transfer using a single rf field Eddy R. Rey Castellanos, Dominique P. Frueh, and Julien Wist Citation: J. Chem. Phys. 129, 014504 (2008); doi: 10.1063/1.2939572 View online: http://dx.doi.org/10.1063/1.2939572

More information

Can you differentiate A from B using 1 H NMR in each pair?

Can you differentiate A from B using 1 H NMR in each pair? Can you differentiate A from B using 1 H NMR in each pair? To be NMR active any nucleus must have a spin quantum number, different from zero (I 0) As in 1 H, the spin quantum number (I) of 13 C is 1/2

More information

Chemistry: The Central Science. Chapter 9: Molecular Geometry and Bonding Theory

Chemistry: The Central Science. Chapter 9: Molecular Geometry and Bonding Theory Chemistry: The Central Science Chapter 9: Molecular Geometry and Bonding Theory The shape and size of a molecule of a particular substance, together with the strength and polarity of its bonds, largely

More information

An introduction to Solid State NMR and its Interactions

An introduction to Solid State NMR and its Interactions An introduction to Solid State NMR and its Interactions From tensor to NMR spectra CECAM Tutorial September 9 Calculation of Solid-State NMR Parameters Using the GIPAW Method Thibault Charpentier - CEA

More information

NMR IMAGING OF SOLIDS WITH A SURFACE COIL. J.B. Miller and A.N. Garroway

NMR IMAGING OF SOLIDS WITH A SURFACE COIL. J.B. Miller and A.N. Garroway NMR IMAGING OF SOLIDS WITH A SURFACE COIL J.B. Miller and A.N. Garroway Chemistry Division, Code 6120 Naval Research Laboratory Washington, D.C. 20375-5000 INTRODUCTION Nuclear magnetic resonance (NMR)

More information

PRACTICAL ASPECTS OF NMR RELAXATION STUDIES OF BIOMOLECULAR DYNAMICS

PRACTICAL ASPECTS OF NMR RELAXATION STUDIES OF BIOMOLECULAR DYNAMICS PRACTICAL ASPECTS OF MR RELAXATIO STUDIES OF BIOMOLECULAR DYAMICS Further reading: Can be downloaded from my web page Korzhnev D.E., Billeter M., Arseniev A.S., and Orekhov V. Y., MR Studies of Brownian

More information

Decoupling Theory and Practice

Decoupling Theory and Practice Decoupling Theory and Practice General Concepts We have spent the last two lectures discussing the structural implications of -coupling analysis and overall have discovered that the interaction may readily

More information

VALENCE Hilary Term 2018

VALENCE Hilary Term 2018 VALENCE Hilary Term 2018 8 Lectures Prof M. Brouard Valence is the theory of the chemical bond Outline plan 1. The Born-Oppenheimer approximation 2. Bonding in H + 2 the LCAO approximation 3. Many electron

More information

Ethyl crotonate. Example of benchtop NMR on small organic molecules

Ethyl crotonate. Example of benchtop NMR on small organic molecules R Ethyl crotonate Example of benchtop NMR on small organic molecules Ethyl crotonate (C 6 H 10 O 2 ) is a colourless liquid at room temperature. It is soluble in water, and is used as a solvent for cellulose

More information

Cross Polarization 53 53

Cross Polarization 53 53 Cross Polarization 53 Why don t we normally detect protons in the solid-state BPTI Strong couplings between protons ( >20kHz) Homogeneous interaction Not readily averaged at moderate spinning speeds Rhodopsin

More information

A Hands on Introduction to NMR Lecture #1 Nuclear Spin and Magnetic Resonance

A Hands on Introduction to NMR Lecture #1 Nuclear Spin and Magnetic Resonance A Hands on Introduction to NMR 22.920 Lecture #1 Nuclear Spin and Magnetic Resonance Introduction - The aim of this short course is to present a physical picture of the basic principles of Nuclear Magnetic

More information

Introduction to solution NMR. Alexandre Bonvin. The NMR research group. Bijvoet Center for Biomolecular Research

Introduction to solution NMR. Alexandre Bonvin. The NMR research group. Bijvoet Center for Biomolecular Research Introduction to solution NMR 1 Alexandre Bonvin Bijvoet Center for Biomolecular Research with thanks to Dr. Klaartje Houben Bente%Vestergaard% The NMR research group Prof. Marc Baldus Prof. Rolf Boelens

More information

Introduction of Key Concepts of Nuclear Magnetic Resonance

Introduction of Key Concepts of Nuclear Magnetic Resonance I have not yet lost that sense of wonder, and delight, that this delicate motion should reside in all ordinary things around us, revealing itself only to those who looks for it. E. M. Purcell, Nobel Lecture.

More information

Band-Selective Homonuclear 2D Correlation Experiments

Band-Selective Homonuclear 2D Correlation Experiments Band-Selective Homonuclear 2D Correlation Experiments Application Note Authors Péter Sándor Agilent Technologies GmbH D76337 Waldbronn Germany Abstract This application note demonstrates the utility of

More information

NMR = Nuclear Magnetic Resonance

NMR = Nuclear Magnetic Resonance NMR = Nuclear Magnetic Resonance NMR spectroscopy is the most powerful technique available to organic chemists for determining molecular structures. Looks at nuclei with odd mass numbers or odd number

More information

Carbon and Heteronuclear NMR on the Bruker

Carbon and Heteronuclear NMR on the Bruker Carbon and Heteronuclear NMR on the Bruker There are several different types of carbon spectra such as a normal qualitative spectrum, DEPT, coupled, and those with and without NOE. This handout discusses

More information

Superoperators for NMR Quantum Information Processing. Osama Usman June 15, 2012

Superoperators for NMR Quantum Information Processing. Osama Usman June 15, 2012 Superoperators for NMR Quantum Information Processing Osama Usman June 15, 2012 Outline 1 Prerequisites 2 Relaxation and spin Echo 3 Spherical Tensor Operators 4 Superoperators 5 My research work 6 References.

More information

Filtered/edited NOESY spectra

Filtered/edited NOESY spectra Filtered/edited NOESY spectra NMR Seminar HS 207 Nina Ripin 22..7 Overview NMR of biomolecular complexes Problems and Solutions Filtered/edited nomenclature Experimental elements NOESY vs filtered pulse

More information

Lecture Notes Chem 51A S. King

Lecture Notes Chem 51A S. King Lecture Notes hem 51A S. King hapter 14 Nuclear Magnetic Resonance Spectroscopy Nuclear Magnetic Resonance (NMR) spectroscopy uses energy in the radiowave portion of the electromagnetic spectrum. The nuclei

More information

Lecture 10. Born-Oppenheimer approximation LCAO-MO application to H + The potential energy surface MOs for diatomic molecules. NC State University

Lecture 10. Born-Oppenheimer approximation LCAO-MO application to H + The potential energy surface MOs for diatomic molecules. NC State University Chemistry 431 Lecture 10 Diatomic molecules Born-Oppenheimer approximation LCAO-MO application to H + 2 The potential energy surface MOs for diatomic molecules NC State University Born-Oppenheimer approximation

More information

Supplementary Information: Dependence of nuclear spin singlet lifetimes on RF spin-locking power

Supplementary Information: Dependence of nuclear spin singlet lifetimes on RF spin-locking power Supplementary Information: Dependence of nuclear spin singlet lifetimes on RF spin-locking power Stephen J. DeVience a, Ronald L. Walsworth b,c, Matthew S. Rosen c,d,e a Department of Chemistry and Chemical

More information

Lecture #7 In Vivo Water

Lecture #7 In Vivo Water Lecture #7 In Vivo Water Topics Hydration layers Tissue relaxation times Magic angle effects Magnetization Transfer Contrast (MTC) CEST Handouts and Reading assignments Mathur-De Vre, R., The NMR studies

More information

NMR BMB 173 Lecture 16, February

NMR BMB 173 Lecture 16, February NMR The Structural Biology Continuum Today s lecture: NMR Lots of slides adapted from Levitt, Spin Dynamics; Creighton, Proteins; And Andy Rawlinson There are three types of particles in the universe Quarks

More information

NMR-spectroscopy. I: basics. Peter Schmieder

NMR-spectroscopy. I: basics. Peter Schmieder NMR-spectroscopy I: basics Why spectroscopy? 2/102 Why spectroscopy It is well established that all biological relevant processes take place via interactions of molecules, either small ones (metall ions,

More information

Schematic of the COSY Experiment

Schematic of the COSY Experiment Schematic of the COSY Experiment 9 o 9 o (d) t 2 (aq) homonuclear COSY But what happens for a heteronuclear experiment? The 9 o pulses will not cover both sets of nuclei, and there would be issues with

More information

Principles of Molecular Spectroscopy: Electromagnetic Radiation and Molecular structure. Nuclear Magnetic Resonance (NMR)

Principles of Molecular Spectroscopy: Electromagnetic Radiation and Molecular structure. Nuclear Magnetic Resonance (NMR) Principles of Molecular Spectroscopy: Electromagnetic Radiation and Molecular structure Nuclear Magnetic Resonance (NMR) !E = h" Electromagnetic radiation is absorbed when the energy of photon corresponds

More information

SSSC Discovery Series NMR2 Multidimensional NMR Spectroscopy

SSSC Discovery Series NMR2 Multidimensional NMR Spectroscopy SSSC Discovery Series NMR2 Multidimensional NMR Spectroscopy Topics: 1. Some Common Experiments 2. Anatomy of a 2D experiment 3. 3D NMR spectroscopy no quantum mechanics! Some Common 2D Experiments Very

More information

eigenvalues eigenfunctions

eigenvalues eigenfunctions Born-Oppenheimer Approximation Atoms and molecules consist of heavy nuclei and light electrons. Consider (for simplicity) a diatomic molecule (e.g. HCl). Clamp/freeze the nuclei in space, a distance r

More information

Chapter 15 Lecture Outline

Chapter 15 Lecture Outline Organic Chemistry, First Edition Janice Gorzynski Smith University of Hawaii Chapter 5 Lecture Outline Introduction to NMR Two common types of NMR spectroscopy are used to characterize organic structure:

More information

1H 1D-NOE Difference Spectra and Spin-Saturation Transfer Experiments on the GN500

1H 1D-NOE Difference Spectra and Spin-Saturation Transfer Experiments on the GN500 UGN526 VVM-21JUN88CD VVM-31OCT91UD 1H 1D-NOE Difference Spectra and Spin-Saturation Transfer Experiments on the GN500 Double-resonance experiments are techniques which use a second irradiating field (B

More information

Lecture #6 Chemical Exchange

Lecture #6 Chemical Exchange Lecture #6 Chemical Exchange Topics Introduction Effects on longitudinal magnetization Effects on transverse magnetization Examples Handouts and Reading assignments Kowalewski, Chapter 13 Levitt, sections

More information

Chem8028(1314) - Spin Dynamics: Spin Interactions

Chem8028(1314) - Spin Dynamics: Spin Interactions Chem8028(1314) - Spin Dynamics: Spin Interactions Malcolm Levitt see also IK m106 1 Nuclear spin interactions (diamagnetic materials) 2 Chemical Shift 3 Direct dipole-dipole coupling 4 J-coupling 5 Nuclear

More information

Double-Resonance Experiments

Double-Resonance Experiments Double-Resonance Eperiments The aim - to simplify complicated spectra by eliminating J-couplings. omonuclear Decoupling A double resonance eperiment is carried out using a second rf source B 2 in addition

More information