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Nuclear Magnetic Resonance

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Electromagnetic radiation: light and other forms of radiant energy = c & E = h ... the chemical shift of the hydroxyl hydrogen is variable. ... – PowerPoint PPT presentation

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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
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

16
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

17
Electrons Shield
What causes differences? Electrons shield.
Remove electrons they de-shield.
18
Electron Withdrawing groups deshield by removing
electron density
I suck
19
Electron density can be added or removed through
the p or s systems
20
Field currents in benzene
21
Ring currents usually deshield
22
acetylene
23
Alkenes
24
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

25
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)

26
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

27
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

28
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

29
Chemical Shift - 1H-NMR
30
Chemical Shift - 1H-NMR
31
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

32
Chemical Shift
  • Hybridization of adjacent atoms

33
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

34
Methyl Acetate
35
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

36
Signal Splitting (n 1)
  • Problem predict the number of 1H-NMR signals
    and the splitting pattern of each

37
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

38
Origins of Signal Splitting
39
Origins of Signal Splitting
  • Table 13.8 Observed signal splitting patterns
    for an H with 0, 1, 2, and 3 equivalent
    neighboring hydrogens

40
Origins of Signal Splitting
  • Table 13.8 (contd.)

41
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

42
Ethyl acetate
43
Isopropyl alcohol
44
13C-NMR Spectroscopy
  • Each nonequivalent 13C gives a different signal
  • A 13C is split by the 1H bonded to it according
    to the (n 1) rule
  • Coupling constants of 100-250 Hz are common,
    which means that there is often significant
    overlap between signals, and splitting patterns
    can be very difficult to determine
  • The most common mode of operation of a 13C-NMR
    spectrometer is a hydrogen-decoupled mode

45
13C-NMR Spectroscopy
  • In a hydrogen-decoupled mode, a sample is
    irradiated with two different radio frequencies
  • one to excite all 13C nuclei
  • a second is a broad spectrum of frequencies that
    causes all hydrogens in the molecule to undergo
    rapid transitions between their nuclear spin
    states
  • On the time scale of a 13C-NMR spectrum, each
    hydrogen is in an average or effectively constant
    nuclear spin state, with the result that 1H-13C
    spin-spin interactions are not observed they are
    decoupled

46
Chemical Shift - 13C-NMR
47
C8H10
48
C7H12O4
49
C7H14O
50
Interpreting NMR spectra
  • Alkanes all 1H-NMR signals fall in the narrow
    range of d 0.8-1.7. 13C signals fall in the
    considerably wider range of d 0-60
  • Alkenes vinylic hydrogens typically fall in the
    range d 4.6-5.7
  • coupling constants are generally larger for trans
    vinylic hydrogens (J 11-18 Hz) compared with
    cis vinylic hydrogens (J 5-10 Hz)
  • the sp2 hybridized carbons of alkenes give
    13C-NMR signals in the range d 100-150, which is
    downfield from the signals of sp3 hybridized
    carbons

51
Interpreting NMR spectra
  • Alcohols
  • the chemical shift of the hydroxyl hydrogen is
    variable. It normally falls in the range d
    3.0-4.5, but may be as low as d 0.5.
  • hydrogens on an sp3 hybridized carbon adjacent to
    the -OH group are deshielded by the
    electron-withdawing inductive effect of the
    oxygen and their signals appear in the range d
    3.4-4.3.
  • Ethers a distinctive feature in the 1H-MNR
    spectra of ethers is the chemical shift, d
    3.3-4.0, of hydrogens on carbon attached to the
    ether oxygen.

52
Index of H Deficiency
  • Index of hydrogen deficiency (IHD) the sum of
    the number of rings and pi bonds in a molecule
  • To determine IHD, compare the number of hydrogens
    in an unknown compound with the number in a
    reference hydrocarbon of the same number of
    carbons and with no rings or pi bonds
  • the molecular formula of the reference
    hydrocarbon is CnH2n2

53
Index of H Deficiency
  • For each atom of a Group VII element (F, Cl, Br,
    I) added to the reference hydrocarbon, subtract
    one H
  • No correction is necessary for the addition of
    atoms of Group VI elements (O,S) to the reference
    hydrocarbon
  • For each atom of a Group V element (N, P) added
    to the reference hydrocarbon, add one hydrogen

54
  • Nuclear
  • Magnetic Resonance
  • End Chapter 13
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