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Nuclear Magnetic Resonance (NMR) Spectroscopy

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Nuclear Magnetic Resonance (NMR) Spectroscopy Part 1 Carbon 13 NMR Theory of NMR The positively charged nuclei of certain elements (e.g., 13C and 1H) behave as tiny ... – PowerPoint PPT presentation

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Title: Nuclear Magnetic Resonance (NMR) Spectroscopy


1
Nuclear Magnetic Resonance (NMR) Spectroscopy
  • Part 1
  • Carbon 13 NMR

2
Theory of NMR
  • The positively charged nuclei of certain elements
    (e.g., 13C and 1H) behave as tiny magnets.
  • In the presence of a strong external magnetic
    field (Bo), these nuclear magnets align either
    with ( ) the applied field or opposed to ( )
    the applied field.
  • The latter (opposed) is slightly higher in energy
    than aligned with the field.

DE is very small
3
Theory of NMR
  • The small energy difference between the two
    alignments of magnetic spin corresponds to the
    energy of radio waves according to Einsteins
    equation Ehn.
  • Application of just the right radiofrequency (n)
    causes the nucleus to flip to the higher energy
    spin state
  • Not all nuclei require the same amount of energy
    for the quantized spin flip to take place.
  • The exact amount of energy required depends on
    the chemical identity (H, C, or other element)
    and the chemical environment of the particular
    nucleus.

4
Theory of NMR
  • Our departments NMR spectrometer (in Dobo 245)
    has a superconducting magnet with a field
    strength of 9.4 Tesla. On this
    instrument, 1H nuclei absorb (resonate) near a
    radiofrequency of 400 MHz
    13C nuclei absorb around 100 MHz.
  • Nuclei are surrounded by electrons.
    The strong applied magnetic field
    (Bo) induces the
    electrons to circulate
    around the nucleus (left hand rule).

(9.4 T)
5
Theory of NMR
  • The induced circulation of electrons sets up a
    secondary (induced) magnetic field (Bi) that
    opposes the applied field (Bo) at the nucleus
    (right hand rule).
  • We say that nuclei are shielded from the full
    applied magnetic field by the surrounding
    electrons because the secondary field diminishes
    the field at the nuclei.

6
Theory of NMR
  • The electron density surrounding a given nucleus
    depends on the electronegativity of the attached
    atoms.
  • The more electronegative the attached atoms, the
    less the electron density around the nucleus in
    question.
  • We say that that nucleus is less shielded, or is
    deshielded by the electronegative atoms.
  • Deshielding effects are generally additive. That
    is, two highly electronegative atoms (2 Cl atoms,
    for example) would cause more deshielding than
    only 1 Cl atom.

C and H are deshielded C and H are more
deshielded
7
Chemical Shift
  • We call the relative position of absorption in
    the NMR spectrum (which is related to the amount
    of deshielding) the chemical shift. It is a
    unitless number (actually a ratio, in which the
    units cancel), but we assign units of ppm or d
    (Greek letter delta) units.
  • For 1H, the usual scale of NMR spectra is 0 to 10
    (or 12) ppm (or d).
  • The usual 13C scale goes from 0 to about 220
    ppm.
  • The zero point is defined as the position of
    absorption of a standard, tetramethylsilane
    (TMS)
  • This standard has only one type
    of C and only one
    type of H.

8
Chemical Shifts
9
Chemical Shifts
  • Both 1H and 13C Chemical shifts are related to
    three major factors
  • The hybridization (of carbon)
  • Presence of electronegative atoms or electron
    attracting groups
  • The degree of substitution (1º, 2º or 3º).
    These latter effects are most important in 13C
    NMR, and in that context are usually called
    steric effects.
  • First well focus on Carbon NMR spectra
  • (they are simpler)

10
CMR Spectra
  • Each unique C in a structure gives a single peak
    in the spectrum there is rarely any overlap.
  • The carbon spectrum spans over 200 ppm chemical
    shifts only 0.001 ppm apart can be distinguished
    this allows for over 2x105 possible chemical
    shifts for carbon.
  • The intensity (size) of each peak is NOT directly
    related to the number of that type of carbon.
    Other factors contribute to the size of a peak
  • Peaks from carbon atoms that have attached
    hydrogen atoms are bigger than those that dont
    have hydrogens attached.
  • Carbon chemical shifts are usually reported as
    downfield from the carbon signal of
    tetramethylsilane (TMS).

11
13C Chemical Shifts
12
Predicting 13C Spectra
  • Problem 13.6 Predict the number of carbon
    resonance lines in the 13C spectra of the
    following ( unique Cs)

  • 4 lines
  • plane of symmetry

13
Predicting 13C Spectra
  • Predicte the number of carbon resonance lines in
    the 13C spectra of the major product of the
    following reaction

  • 7 lines
  • 5 lines
  • plane of symmetry

14
Predicting 13C Spectra
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C6H12O2
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