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Nuclear Magnetic Resonance

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Title: Nuclear Magnetic Resonance


1
Nuclear Magnetic Resonance
  • Chapter 13

2
Electromagnetic Radiation
  • Electromagnetic radiation light and other forms
    of radiant energy ??? c E h?
  • Wavelength (l) the distance between consecutive
    identical points on a wave
  • Frequency (n) the number of full cycles of a
    wave that pass a point in a second
  • Hertz (Hz) the unit in which radiation
    frequency is reported s-1 (read per second)

3
Electromagnetic Radiation
  • Wavelength

4
Molecular Spectroscopy
  • We study three types of molecular spectroscopy

5
A pictorial view of UV/Vis
UV/Vis radiation is measured in nm (wavelength)
6
IR Spectroscopy
  • IR radiation is measured in cm-1
  • This is actually a frequency. Remember that
    frequency and wavelength are inversely
    proportional.

7
NMR Spectroscopy
  • NMR uses radiowaves, measured in MHz

8
Nuclear Spin States
  • Any atomic nucleus that has an odd mass, an odd
    atomic number, or both has a spin and a resulting
    nuclear magnetic moment.
  • The allowed nuclear spin states are determined by
    the spin quantum number, I , of the nucleus.
  • A nucleus with spin quantum
    number I has 2I 1spin
    states. If I 1/2, there are
    two allowed spin states

9
Molecular Spectroscopy
  • Nuclear magnetic resonance (NMR) spectroscopy a
    spectroscopic technique that gives us information
    about the number and types of atoms in a
    molecule, for example, about the number and types
    of
  • hydrogens using 1H-NMR spectroscopy
  • carbons using 13C-NMR spectroscopy
  • phosphorus using 31P-NMR spectroscopy

10
Nuclear Spin States
  • Spin quantum numbers and allowed nuclear spin
    states for selected isotopes of elements common
    to organic compounds

11
Nuclear Spins in B0
  • Within a collection of 1H and 13C atoms, nuclear
    spins are completely random in orientation
  • When placed in a strong external magnetic field
    of strength B0, however, interaction between
    nuclear spins and the applied magnetic field are
    quartered, with the result that only certain
    orientations of nuclear magnetic moments are
    allowed

12
Nuclear Spins in B0
  • For 1H and 13C, only two orientations are allowed.

13
Nuclear Spins in B0
  • In an applied field strength of 7.05T, which is
    readily available with present-day
    superconducting electromagnets, the difference in
    energy between nuclear spin states for
  • 1H is approximately 0.0286 cal/mol, which
    corresponds to electromagnetic radiation of 300
    MHz (300,000,000 Hz)(300MHz)
  • 13C is approximately 0.00715 cal/mol, which
    corresponds to electromagnetic radiation of 75MHz
    (75,000,000 Hz)(75 MHz)

14
Population in high vs low
  • ?E 0.0286 cal/mol RT582cal/mol
  • If pop in high E state is 1,000,000 then pop in
    low energy state is 1,000,049

15
Nuclear Magnetic Resonance
  • If we were dealing with 1H nuclei isolated from
    all other atoms and electrons, any combination of
    applied field and radiation that produces a
    signal for one 1H would produce a signal for all
    1H. The same is true of 13C 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

16
NMR Spectroscopy
  • NMR uses radiowaves, measured in MHz
  • The energy transitions depend on the strength of
    the magnetic field which is different from
    machine to machine
  • We define the machine independent ppm as

17
Nuclear Magnetic Resonance
  • The circulation of electrons around a nucleus in
    an applied field is called diamagnetic current
    and the nuclear shielding resulting from it is
    called diamagnetic shielding
  • The difference in resonance frequencies among the
    various hydrogen nuclei within a molecule due to
    shielding/deshielding is generally very small

18
Nuclear Magnetic Resonance
  • The difference in resonance frequencies for
    hydrogens in CH3Cl compared to CH3F under an
    applied field of 7.05T is only 360 Hz, which is
    1.2 parts per million (ppm) compared with the
    irradiating frequency

19
Nuclear Magnetic Resonance
  • It is customary to measure the resonance
    frequency (signal) of individual nuclei relative
    to the resonance frequency (signal) of a
    reference compound
  • The reference compound now universally accepted
    is tetramethylsilane (TMS)

20
Nuclear Magnetic Resonance
  • For a 1H-NMR spectrum, signals are reported by
    their shift from the 12 H signal in TMS
  • For a 13C-NMR spectrum, signals are reported by
    their shift from the 4 C signal in TMS
  • Chemical shift (d) the shift in ppm of an NMR
    signal from the signal of TMS

21
NMR Spectrometer
  • Essentials of an NMR spectrometer are a powerful
    magnet, a radio-frequency generator, and a
    radio-frequency detector
  • The sample is dissolved in a solvent, most
    commonly CDCl3 or D2O, and placed in a sample
    tube which is then suspended in the magnetic
    field and set spinning
  • Using a Fourier transform NMR (FT-NMR)
    spectrometer, a spectrum can be recorded in about
    2 seconds

22
NMR Spectrum
  • Downfield the shift of an NMR signal to the left
    on the chart paper
  • Upfield the shift of an NMR signal to the right
    on the chart paper

23
Equivalent Hydrogens
  • Equivalent hydrogens have the same chemical
    environment (Section 2.3C)
  • Molecules with
  • 1 set of equivalent hydrogens give 1 NMR signal
  • 2 or more sets of equivalent hydrogens give a
    different NMR signal for each set

24
Signal Areas
  • Relative areas of signals are proportional to the
    number of hydrogens giving rise to each signal
  • All modern NMR spectrometers electronically
    integrate and record the area of each signal

25
Chemical Shift - 1H-NMR
26
Chemical Shift - 1H-NMR
27
Chemical Shift
  • Depends on (1) electronegativity of nearby atoms,
    (2) the hybridization of adjacent atoms, and (3)
    magnetic induction within an adjacent pi bond
  • Electronegativity

28
Chemical Shift
  • Hybridization of adjacent atoms

29
Chemical Shift
  • Magnetic induction in pi bonds of a
  • a carbon-carbon triple bond shields an acetylenic
    hydrogen and shifts its signal upfield (to the
    right) to a smaller d value
  • carbon-carbon double bond deshields vinylic a
    hydrogens and shifts their signal downfield (to
    the left) to a larger d value

30
Field currents in benzene
31
acetylene
32
Alkenes
33
Methyl Acetate
34
Signal Splitting (n 1)
  • Peak the units into which an NMR signal is
    split doublet, triplet, quartet, etc.
  • Signal splitting splitting of an NMR signal
    into a set of peaks by the influence of
    neighboring nonequivalent hydrogens
  • (n 1) rule the 1H-NMR signal of a hydrogen or
    set of equivalent hydrogens is split into (n 1)
    peaks by a nonequivalent set of n equivalent
    neighboring hydrogens

35
Signal Splitting (n 1)
  • Problem predict the number of 1H-NMR signals
    and the splitting pattern of each

36
Origins of Signal Splitting
  • When the chemical shift of one nucleus is
    influenced by the spin of another, the two are
    said to be coupled
  • Consider nonequivalent hydrogens Ha and Hb on
    adjacent carbons
  • the chemical shift of Ha is influenced by whether
    the spin of Hb is aligned with or against the
    applied field

37
Origins of Signal Splitting
38
Origins of Signal Splitting
  • Table 13.8 Observed signal splitting patterns
    for an H with 0, 1, 2, and 3 equivalent
    neighboring hydrogens

39
Origins of Signal Splitting
  • Table 13.8 (contd.)

40
Coupling Constants
  • Coupling constant (J) the distance between
    peaks in an NMR multiplet, expressed in hertz
  • J is a quantitative measure of the magnetic
    interaction of nuclei whose spins are coupled

41
Ethyl acetate
42
Isopropyl alcohol
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