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NMR Theory

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NMR Theory There are 2 variables in NMR: an applied magnetic field B0, and the frequency ( ) of radiation required for resonance, measured in MHz. – PowerPoint PPT presentation

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Title: NMR Theory


1
NMR Theory
  • There are 2 variables in NMR an applied magnetic
    field B0, and the frequency (? ) of radiation
    required for resonance, measured in MHz.

http//vam.anest.ufl.edu/forensic/nmr.html
2
Effect of B0 on resonance frequency
  • NMR spectrometers are designated according to the
    frequency required to make protons resonate. The
    modern standard is 300 MHz. However,
    manufacturers are actively pursuing stronger
    magnets. 900 MHz is currently as high as it gets.

3
Schematic of an NMR
4
Resonance Frequency
  • Different nuclei resonate at greatly different ?
    on a 300 MHz instrument (1H 300 MHz) 13C
    resonates at 75 MHz.
  • The same type of nucleus also absorbs at slightly
    different ?, depending on its chemical
    environment.
  • Exact frequency of resonance chemical shift
  • The strength of the magnetic field actually felt
    by a nucleus (Beff) determines its resonance
    frequency.
  • Electron clouds shield the nucleus from the
    magnet
  • Circulation of electrons in p orbitals can
    generate local magnetic fields that influence
    Beff
  • Modern NMR spectrometers use a constant magnetic
    field strength B0, and pulse a broad range of
    frequencies to bring about the resonance of all
    nuclei at the same time.

5
Chemical Shift
  • Peaks on NMR spectrum resonances .
  • Chemical shift is measured in ppm
  • ppm ? in Hz relative to ref peak/instrument ?
    in MHz.
  • Protons absorb between 0-10 ppm. C-13 nuclei
    absorb between 0-250 ppm.
  • Reference peak 0 ppm (CH)4Si
    tetramethylsilane (TMS). TMS is an inert compound
    that gives a single peak at higher frequency than
    most typical NMR peaks.

6
Electronic Shielding
7
Shielding in Spectrum
8
1H NMR Interpretation
  1. Number of Resonances
  2. Chemical Shifts
  3. Integrations
  4. Splitting Patterns
  5. Exchangeable Protons

9
Number of Resonances
10
Stereochemistry
  • Watch out when you have rings and/or double
    bonds! To determine equivalent protons in
    cycloalkanes and alkenes, always draw all bonds
    to hydrogen.

11
Number of Signals in a Cyclic Compound
  • Proton equivalency in cycloalkanes can be
    determined similarly.

Types of NMR relationships 1. chemically
equivalent 2. coincidentally equivalent 3.
non-equivalent, enantiotopic 4. non-equivalent,
diastereopic 5. non-equivalent. Use substitution
criterion to decide.
12
Chemical Shift - Local Diamagnetic Shielding
13
Induced Anisotropic Shielding - Benzene
  • In a magnetic field, the six ? electrons in a
    benzene ring circulate around the ring creating a
    ring current.
  • The magnetic field induced by these moving
    electrons reinforces the applied magnetic field
    in the vicinity of the protons.
  • The protons feel a stronger magnetic field and
    thus are deshielded. A higher frequency is needed
    for resonance.

14
Induced Anisotropic Shielding - Alkenes
  • In a magnetic field, the loosely held ? electrons
    circulate creating a magnetic field that
    reinforces the applied field in the vicinity of
    the protons.
  • Since the protons now feel a stronger magnetic
    field, they require a higher frequency for
    resonance. Thus the protons are deshielded and
    the absorption is downfield.

15
Induced Anisotropic Shielding - Alkyne
  • In a magnetic field, the ? electrons of a
    carbon-carbon triple bond are induced to
    circulate, but in this case the induced magnetic
    field opposes the applied magnetic field (B0).
  • Thus, the proton feels a weaker magnetic field,
    so a lower frequency is needed for resonance. The
    nucleus is shielded and the absorption is upfield.

16
Summary of pi electron effects
17
Characteristic Shifts
18
Integrations
  • The integration of each resonance is proportional
    to the number of absorbing protons.
  • The integral ratios tell us the ratios of the
    protons causing the peak.
  • Strategy - find a peak that you can assign
    unambiguously and set its integral at the
    appropriate number of Hs.

19
Splitting Patterns
  • Consider the spectrum below

20
Theory of spin-spin splitting
  • Spin-spin splitting occurs only between
    nonequivalent protons on the same carbon or
    adjacent carbons.

Let us consider how the doublet due to the CH2
group on BrCH2CHBr2 occurs
21
Triplet
Let us now consider how a triplet arises
  • When placed in an applied magnetic field (B0),
    the adjacent protons Ha and Hb can each be
    aligned with (?) or against (?) B0.
  • Thus, the absorbing proton feels three slightly
    different magnetic fieldsone slightly larger
    than B0, one slightly smaller than B0, and one
    the same strength at B0.

22
Triplet
23
Peak ratios in a multiplet.
  • Doublet The two spin states of the proton
    causing splitting are nearly equally populated
    (because the energy difference is so small).
    Therefore a doublet is has a peak ratio of 11.
  • Triplet - Because there are two different ways
    to align one proton with B0, and one proton
    against B0that is, ?a?b and ?a?bthe middle peak
    of the triplet is twice as intense as the two
    outer peaks, making the ratio of the areas under
    the three peaks 121.
  • Higher use Pascals triangle

24
Multiplet names
25
Rules for predicting splitting patterns
  1. Equivalent protons do not split each others
    signals.
  2. A set of n nonequivalent protons splits the
    signal of a nearby proton into n 1 peaks.
  3. Splitting is observed for nonequivalent protons
    on the same carbon or adjacent carbons.

If Ha and Hb are not equivalent, splitting is
observed when
26
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27
Nuclear Magnetic Resonance Spectroscopy
1H NMRSpin-Spin Splitting
Whenever two (or three) different sets of
adjacent protons are equivalent to each other,
use the n 1 rule to determine the splitting
pattern.
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