Lecture 3 NMR Spectroscopy. January 26, 2016 Chemistry 328N

Similar documents
January 29, 2019 Chemistry 328N

Lecture 2 nmr Spectroscopy

William H. Brown & Christopher S. Foote

7a. Structure Elucidation: IR and 13 C-NMR Spectroscopies (text , , 12.10)

Nuclear Magnetic Resonance (NMR) Spectroscopy Introduction:

January 30, 2018 Chemistry 328N

NMR Spectroscopy. for 1 st B.Tech INTRODUCTION Lecture -1 Indian Institute of Technology, Dhanbad

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

Chapter 13 Spectroscopy

Nuclear Magnetic Resonance H-NMR Part 1 Introduction to NMR, Instrumentation, Sample Prep, Chemical Shift. Dr. Sapna Gupta

Química Orgânica I. Nuclear Magnetic Resonance Spectroscopy (I) Ciências Farmacêuticas Bioquímica Química AFB QO I 2007/08 1 AFB QO I 2007/08 2

Nuclear Magnetic Resonance

NMR Nuclear Magnetic Resonance Spectroscopy p. 83. a hydrogen nucleus (a proton) has a charge, spread over the surface

Chapter 15 Lecture Outline

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

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

16.1 Introduction to NMR Spectroscopy. Spectroscopy. Spectroscopy. Spectroscopy. Spectroscopy. Spectroscopy 4/11/2013

Physical Background Of Nuclear Magnetic Resonance Spectroscopy

Unit 11 Instrumentation. Mass, Infrared and NMR Spectroscopy

NMR = Nuclear Magnetic Resonance

10.3 NMR Fundamentals

Chapter 6 Part 1 Structure of the atom

With that first concept in mind, it is seen that a spinning nucleus creates a magnetic field, like a bar magnet

16.1 Introduction to NMR. Spectroscopy

3.15 Nuclear Magnetic Resonance Spectroscopy, NMR

Magnetic Resonance Spectroscopy EPR and NMR

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

1. neopentyl benzene. 4 of 6

Chapter 13 Nuclear Magnetic Resonance Spectroscopy

Chapter 14. Nuclear Magnetic Resonance Spectroscopy

Chemistry Instrumental Analysis Lecture 2. Chem 4631

Unit title: Atomic and Nuclear Physics for Spectroscopic Applications

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

Electron Spin Resonance, Basic principle of NMR, Application of NMR in the study of Biomolecules, NMR imaging and in vivo NMR spectromicroscopy

Nuclear Magnetic Resonance Spectroscopy: Tools for Structure Determination

Chemistry Instrumental Analysis Lecture 3. Chem 4631

Module 13: Chemical Shift and Its Measurement

1. The most important aspects of the quantum theory.

Introduction. The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants

Nuclear Magnetic Resonance Spectroscopy

CHEM6416 Theory of Molecular Spectroscopy 2013Jan Spectroscopy frequency dependence of the interaction of light with matter

Lecture 19: Building Atoms and Molecules

Biophysical Chemistry: NMR Spectroscopy

Chapter 7. Characteristics of Atoms. 7.1 Electromagnetic Radiation. Chapter 7 1. The Quantum Mechanical Atom. Atoms: How do we study atoms?

Chemistry 213 Practical Spectroscopy

Chapter 7. Nuclear Magnetic Resonance Spectroscopy

Lecture 02 Nuclear Magnetic Resonance Spectroscopy Principle and Application in Structure Elucidation

Chancellor Phyllis Wise invites you to a birthday party!

Chapter 13: Molecular Spectroscopy

Lecture 19: Building Atoms and Molecules

Fundamental MRI Principles Module Two

Chapter 9. Nuclear Magnetic Resonance. Ch. 9-1

Chapter 16 Nuclear Magnetic Resonance Spectroscopy

Fundamental MRI Principles Module 2 N. Nuclear Magnetic Resonance. X-ray. MRI Hydrogen Protons. Page 1. Electrons

CH Exam #4 (Take Home) Date Due: 11/25,26/2013

- 1/2. = kb o = hνν + 1/2. B o increasing magnetic field strength. degenerate at B o = 0

Magnetic Resonance Spectroscopy ( )

Chapter 9: Electrons and the Periodic Table

Chapter 14 Spectroscopy

NPTEL/IITM. Molecular Spectroscopy Lectures 1 & 2. Prof.K. Mangala Sunder Page 1 of 15. Topics. Part I : Introductory concepts Topics

Lecture Notes Chem 51A S. King

NMR Spectroscopy Laboratory Experiment Introduction. 2. Theory

MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY

Ch 7 Quantum Theory of the Atom (light and atomic structure)

The early periodic table based on atomic weight. (Section 5.1) Lets review: What is a hydrogen atom? 1 electron * nucleus H 1 proton

CVB102 Lecture 1 - Chemical Structure and Reactivity. Contact Information: Dr. Bill Lot Electronic Structure of Atoms

ATOMIC PHYSICS. history/cosmology/tools/ tools-spectroscopy.htm CHAPTER 9 - FROM SPECTROSCOPY TO ATOMS

Nuclear magnetic resonance spectroscopy

Democritus & Leucippus (~400 BC) Greek philosophers: first to propose that matter is made up of particles called atomos, the Greek word for atoms

Ch. 7 The Quantum Mechanical Atom. Brady & Senese, 5th Ed.

Introduction of Key Concepts of Nuclear Magnetic Resonance

Worksheet 2.1. Chapter 2: Atomic structure glossary

ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY

MRI Homework. i. (0.5 pt each) Consider the following arrangements of bar magnets in a strong magnetic field.

Light. Light (con t.) 2/28/11. Examples

Lectures Spectroscopy. Fall 2012

AST 105 Intro Astronomy The Solar System. MIDTERM II: Tuesday, April 5 [covering Lectures 10 through 16]

Homework Problem Set 10 Iverson CH320M/CH328M Due Monday, December 10

Experiment 2 - NMR Spectroscopy

Nuclear Magnetic Resonance (NMR)

Atomic Structure. Standing Waves x10 8 m/s. (or Hz or 1/s) λ Node

ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.

Introduction. Electromagnetic Waves. Electromagnetic Waves

NUCLEAR MAGNETIC RESONANCE AND INTRODUCTION TO MASS SPECTROMETRY

CHM 1045 Test #4 December 4, 2000

CHAPTER 28 Quantum Mechanics of Atoms Units

ESSENTIAL QUANTUM PHYSICS PETER LANDSHOFF. University of Cambridge ALLEN METHERELL. University of Central Florida GARETH REES. University of Cambridge

Lectures Spectroscopy. Fall 2012

Increasing energy. ( 10 4 cm -1 ) ( 10 2 cm -1 )

10/27/2017 [pgs ]

Accounts for certain objects being colored. Used in medicine (examples?) Allows us to learn about structure of the atom

Electromagnetic Radiation. Chapter 12: Phenomena. Chapter 12: Quantum Mechanics and Atomic Theory. Quantum Theory. Electromagnetic Radiation

Q1 and Q2 Review large CHEMISTRY

Photochemical principles

Honors Ch3 and Ch4. Atomic History and the Atom

Infrared Spectroscopy

Chapter 5 Light and Matter: Reading Messages from the Cosmos. What is light? Properties of Waves. Waves. The Electromagnetic Spectrum

Inorganic Spectroscopic and Structural Methods

Transcription:

Lecture 3 NMR Spectroscopy January 26, 2016

Please see me after class Enrollment issue Hugo Nicolas Eichner Nurbol Kaliyev

E = hn Energy per photon Frequency Wave Length

Electromagnetic Radiation Important relationships: nl = c Where C = 3.00 x 10 8 m/s E hn = hc l = Where h = 9.537 x 10-14 kcal sec/mol See examples of calculations in sections 12.1 &12.2

Absorbance promotes atom or molecule to higher energy state

Molecular Spectroscopy We study three types of molecular spectroscopy Region of the Spectrum radio frequency infrared ultraviolet-visible Absorption of Radiation Results in Transition Between: nuclear spin energy levels vibrational energy levels electronic energy levels

Absorption of electromagnetic radiation Described by quantum mechanical theories Only discrete (unique) energy states are allowed (accessible) Therefore only discrete (unique) amounts of radiation can be absorbed (or emitted) How many potential energy states are available to the ball??

Summary Molecular Spectroscopy Concept... Discrete transitions in energy levels Transitions with varying energy (areas of spectrum) Nmr : nuclear spin, radio frequency region IR : vibration, infrared region UV-Vis : electronic transitions, UV to visible Please know relationships between frequency, wave length and energy. Know length scale conversions micron, millimeter, nanometer, angstrom...

NMR Spectroscopy

Spin States Electrons have a spin quantum number of 1/2 with allowed values of +1/2 and -1/2 One can consider this as spinning charge that creates an associated magnetic field Electrons therefore behave like tiny bar magnets Remember the Pauli exclusion principle? Spin up and spin down

Nuclear Spin States Nuclei with an odd mass, an odd atomic number, or both also have a net spin and a resulting nuclear magnetic moment. The allowed nuclear spin states are determined by the spin quantum number, I, of the nucleus. For each I there are 2I + 1 spin states If I = 1/2, there are two allowed spin states

Nuclear Spins The shell model for the nucleus tells us that nucleons, just like electrons, fill orbitals. When the number of protons or neutrons equals 2, 8, 20, 28, 50, 82, and 126, orbitals are filled. Because nucleons have spin, just like electrons do, their spin can pair up when the orbitals are being filled and cancel out.

Nuclear Spins 1. If the number of neutrons and the number of protons are both even, then the nucleus has NO spin. He, for example has no spin 2. If the number of neutrons plus the number of protons is odd, then the nucleus has a half-integer spin (i.e. 1/2, 3/2, 5/2) (H and 13 C for example are both 1/2) 3. If the number of neutrons and the number of protons are both odd, then the nucleus has an integer spin (i.e. 1, 2, 3) (Deuterium or N for example)

Nuclear Spins in a Magnetic Field Within a collection of 1 H or 13 C atoms, nuclear spins are random in orientation When placed in a strong external magnetic field the interaction between nuclear spins and the applied magnetic field is quantized, with the result that only certain orientations of the nuclear magnetic moments are allowed

Nuclear Spins in a Magnetic Field E=hn or n = E/h

Nuclear Magnetic Resonance If the nucleus is irradiated with radiation having energy (E=h ) that is exactly the same as the difference between the nuclear spin states, energy is absorbed, and the nuclear spin is flipped from spin state +1/2 (with the applied field) to -1/2 (against the applied field)

Nuclear Spin States Spin quantum numbers and allowed nuclear spin states for selected isotopes of elements common to organic compounds Element 1 H 2 H 12 C 13 C 14 N 16 O 31 P 32 S nuclear spin quantum number ( I ) 1/2 1 0 1/2 1 0 1/2 0 number of spin states 2 3 1 2 3 1 2 1

T (Tesla) = W (Weber) m 2 Nikola Tesla Serbian-American inventor, electrical engineer and scientist Born, 1856 in Smiljan, Lika (Austria-Hungary) Died 1943 in New York City, New York (USA) Inventions: a telephone repeater, rotating magnetic field principle, polyphase alternating-current system, induction motor, alternating-current power transmission, Tesla coil transformer, wireless communication, radio, fluorescent lights, and more than 700 other patents.

http://www.teslasociety.com/index.html Famous and Controversial picture of Tesla

if constructed, would result in: "An inexpensive Wardenclyffe instrument, Towernot bigger than a watch, will enable its bearer to hear anywhere, on sea or land, music or song, the speech of a political leader, the address of an eminent man of science, or the sermon of an eloquent clergyman, delivered in some other place, however distant. In the same manner any picture, character, drawing, or print can be transferred from one to another place." Tesla ray gun The ray was described as the most important of all Tesla s inventions so far. It was said that IT COULD SEND CONSECRATED BEAMS OF PARTICLES THROUGH FREE AIR, and could cause armies of millions to drop dead in their tracks.

At B=1.0T, E 42. = 42.58MHz E = hn = f ( B 0 )

Nuclear Spins in B 0 In an applied field strength of 7.05T (BIG!) E between nuclear spin states for 1 H is approximately 0.0286 cal/mol, which corresponds to electromagnetic radiation of 300 MHz (300,000,000 Hz) 13 C is approximately 0.00715 cal/mol, which corresponds to electromagnetic radiation of 75MHz (75,000,000 Hz) This E is quite small low frequency radiation induces flip (resonance)

Resonance The transition from the lower state to the higher occurs at unique combinations of magnetic field and frequency of electromagnetic radiation. When placed in a magnetic field of strength B, a particle with a net spin can absorb a photon, of frequency n. The frequency, n depends on the gyromagnetic ratio, of the particle. n = B For hydrogen, = 42.58 MHz / Tesla Allows you to calculate spectrometer frequency for 1 H!! This is the frequency at which naked 1 H resonates in that machine

Some Proportionality Constants Gyromagnetic Ratio n = B For 1 H = 42.58 MHz/T Planck s Constant E = h n Speed of light n = c / l or c = n l Chemical Shift d(ppm) = n Spectrometer frequency

NMR Spectrometer

In principle, we could hold field constant and scan frequency looking for resonance, but it is equally effective to scan field strength and hold frequency constant

500MHz 1 H-nmr Spectrometer Magnet

http://www.jeolusa.com/resources/analyticalinstruments/nmrmagnetdestruction/tabid/390/default.aspx

800 The first MHz Avancemachine 1000 system was at UH delivered to the new Centre de RMN à Très Hauts Champs in Lyon, France. 1020 MHz nmr June 2015 Weight 15 tons Highest Frequency in 2013

The 100MHz nmr Chart 90 80 CH 3 0.00 70 60 H 3 C Si CH 3 50 40 CH 3 30 20 10 0 1000 900 800 700 600 500 400 300 200 100 0 Frequency field The TMS resonance is defined as having 0 frequency

100MHz Spectrum 20 C H 3 Cl 20 304.00 15 15 10 10 5 5 0 325 320 315 310 305 300 295 290 285 280 0 450 400 350 300 250 200 150 100 50 0 304 Hz Hz

100MHz nmr Spectrum 20 268.50 20 15 15 10 C H 3 Br 5 10 0 275 270 265 260 255 5 0 450 400 350 300 250 200 150 100 50 0 268.5Hz Hz

Nuclear Magnetic Resonance If we were dealing with 1 H nuclei isolated from all other atoms and electrons, any combination of applied field and radiation that produces a signal for one 1 H would produce a signal for all 1 H. The same for 13 C nuclei But.hydrogens in organic molecules are not isolated from all other atoms; they are surrounded by electrons, which are caused to circulate by the presence of the applied field

Nuclear Magnetic Resonance The circulation of electrons around a nucleus in an applied field is called diamagnetic current. This current generates a field that opposes the applied field...diamagnetic nuclear shielding results. Lenz s Law?? The difference in resonance frequencies between the various hydrogen nuclei within a molecule is due to shielding/deshielding is very small but very important

Lenz s Law Heinrich Lenz 1804-1865

Conditions for Resonance It is the frequency of the radiation and the NET field at the nucleus that matters. The NET field is the sum of all incident magnetic fields including those from: The Giant Magnet (applied field) Diamagnetic Shielding field (electrons) Coupling (spin fields of adjacent nuclei) credit card strips, earth s field, etc..