1 / 14

Introduction to NMR in Chemistry: Understanding the Basics |

NMR, nuclei, spin, magnetic, resonance, spectroscopy, chemical shift

jrosalyn
Download Presentation

Introduction to NMR in Chemistry: Understanding the Basics |

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Intro to NMRfor CHEM 645we also visited the website:The Basics of NMR by Joseph P. Hornak, Ph.D.http://www.cis.rit.edu/htbooks/nmr/ Brian Bahnson Department of Chemistry & Biochemistry University of Delaware

  2. Nuclei Unpaired Protons Unpaired Neutrons Net Spin (MHz/T) 1H 1 0 1/2 42.6 2H 1 1 1 6.5 31P 1 0 1/2 + 17.3 23Na 1 2 3/2 11.3 15N 0 1 1/2 4.3 13C 0 1 1/2 10.7 Tesla Natural abundance 19F 1 0 1/2 40.1 99.98 0.36 1.11 A Spinning Nucleus Gives a Magnetic Moment gyromagnetic ratio  =  unpaired electron spin Spinning nucleus photo frequency applied magnetic field

  3. The energy gap between states is small and corresponds to radio frequency waves E = h  Planck’s constant For I = ½ nuclei have two spin states M = -1/2 M = +1/2

  4. The energy gap gives rise to a slight excess of the +1/2 state -1/2 E +1/2 Boltzmann Distribution Nupper-/Nlower+ = e-E/kT DE = h  N direction of applied static magnetic field - + S

  5. The Net Magnetization Vector N S A 90º pulse places the net vector along the y-axis

  6. The spin-lattice relaxation time – T1 For a clearer description click:The Basics of NMR and follow the links – spin physics – T1 processes The return to equilibrium along the z-axis is the T1

  7. The de-phasing of this precession is mediated by the spin-spin relaxation T2 The spin-spin relaxation time – T2 For a clearer description click:The Basics of NMR and follow the links – spin physics – T2 processes Following a 90º pulse

  8. What is actually measured in NMR experiment? But due to the T1 relaxation: FT

  9. Definition of Chemical Shift d = (n - nREF) x106 / nREF units of ppm

  10. CA CB CA CB Spin-Spin Coupling is Through Bonds a.k.a. scalar-coupling or J-coupling HA HB B0 CA CB +1/2 -1/2 +1/2 -1/2 Looking at only HA JA-B shielded d (ppm) deshielded If HB not there

  11. NOE Effects are Through Space C C C C C C NOEs are highly distant dependent, seen from 2-5Å NOE  1/r6.f (tc) Correlation time is a combination of rotational motions, molecule size + shape dependent, and intra-molecular motions

  12. A Protein’s 1H-NMR Spectra is Complex To assign peaks of proteins, this needs to be spread into a 2nd or 3rd dimension.

  13. 2-D and 3-D Separates Out Spectra

  14. Two Papers to Read for next Thursday’s Class Wuthrich, (1989) “Protein Structure Determination in Solution by Nuclear Magnetic Resonance Spectroscopy” Science 243, 45-50. Ikura et al., (1989) “A Novel Approach for Sequential Assignment of 1H, 13C, and 15N Spectra of Larger Proteins: Heteronuclear Triple-Resonance Three-Dimensional NMR Spectroscopy. Application to Calmodulin” Biochemistry 29, 4659-4667.

More Related