Nuclear Magnetic Resonance - (1H NMR and 13C NMR)

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Nuclear Magnetic Resonance - (1H NMR and 13C NMR)
Nuclear Magnetic Resonance
 (1H NMR and 13C NMR)
Nuclear Magnetic Resonance - (1H NMR and 13C NMR)
Magnetic field is created by a spinning
charge. The resultant magnetic dipoles of
nuclei (I =1/2) are aligned with the external
magnetic field Bo as shown
Nuclear Magnetic Resonance - (1H NMR and 13C NMR)
Splitting of energy levels for a nucleus with I = ½,
 such as hydrogen, in an external magnetic field
Nuclear Magnetic Resonance - (1H NMR and 13C NMR)
A diagram of a continuous wave NMR (CW-
NMR) instrument. The sweep coils are used to
modulate the strength of the external magnetic
field
Nuclear Magnetic Resonance - (1H NMR and 13C NMR)
The NMR tube

            the NMR tube

              Solvents must not contain protons
                               CCl4        CDCl3
                                        O
20 cm
                                  D3C S CD3
        5 mm diameter          dimethyl sulfoxide-d6
                                  (DMSO)
                                             CH3
                                         H3C Si CH3
            the solution (0.7 ml)
                                             CH3
                           tetramethylsilane (reference)
                                    (TMS)
The shielding effect
In an applied magnetic field, magnetic nuclei like
proton precess at a frequency ν, which is
proportional to the strength Bx of the applied
field: ν = γBx/2π
                                 precession orbit

                                 magnetic dipole created
                                 by proton spin

                    H0

            external
           magnetic field
δ = (νmol – νTMS)/ν x 106
Proton chemical shift ranges for samples in CDCl3
solution. The δ scale is relative to TMS at δ = 0
If electron density is withdrawn from around
the hydrogen nucleus toward a more
electronegative atom, the lower electron
density around this hydrogen atom will
produce a smaller magnetic field (opposite to
the magnetic field of the spectrometer) and, as
a result, this proton will be deshielded and will
resonate at a position farther downfield
(farther to the left in the spectrum). For
example:
             CH3-CH3         δ 0.26
             CH3-Cl          δ 3.06
             CH3-OCH3        δ 3.24
Integration of the NMR spectra
The effect of the H – D exchange on
         the NMR spectra
       R-O-H + D2O   R-O-D + D-O-H
The hydroxyl proton can resonate over a large range of
chemical shifts but hydrogen bonding results in the
resonance at a lower magnetic field or higher
frequency. Because of their favored hydrogen-bonded
dimeric association, the hydroxyl proton of carboxylic
acids displays a resonance signal significantly down-
field of other functions
Magnetic anisotropy at the benzene ring
The spectra with and without a coupling pattern
Typical coupling patters
If an atom under examination is
perturbed or influenced by a nearby
magnetic field caused by a nuclear spin
(or set of spins), the observed nucleus
responds to such influences, and its
response is manifested in its resonance
signal. This spin-coupling is transmitted
through the connecting bonds, and it
functions in both directions.
Spin – spin coupling for -CH2-CH3

    For a CH2 group adjacent to a methyl group, there will be four peaks, created by the spin
    orientations of the methyl protons shown below

1             2            2            2            3             3           3           4
A quartet for –CH2-CH3
Four signals with the relative intensity of 1:3:3:1

                                    = quartet

        1      2            3   4

                   Energy
The “roof effect” for coupled protons
Pascal’s triangle (the intensity ratio)
The splitting pattern of a given nucleus (or set of equivalent nuclei) can be
predicted by the n+1 rule, where n is the number of neighboring spin-coupled
nuclei with the same (or very similar) Js. If there are 2 neighboring spin-
coupled nuclei, the observed signal is a triplet (2 + 1 = 3); if there are three
spin-coupled neighbors, the signal is a quartet (3 + 1 = 4 ). In all cases the
central line(s) of the splitting pattern are stronger than those on the
periphery (the “roof effect”).
                                      1
                                1           1

                          1            2          1

                     1          3            3            1
               1           4           6              4       1
Typical coupling patterns with a single coupling
                   constant J
Typical coupling patters with different coupling
                  constants Js
Typical values of coupling constants Js (in Hz)
13C   NMR spectroscopy
When significant portions of a molecule lack C-H bonds, little
information is forthcoming by 1H NMR.

 The following diagram depicts three
 pairs of isomers (A & B) which display
 similar proton NMR spectra.
13C   NMR spectroscopy
13Cisotope has a spin I = ½ (is magnetic)
1.1% of natural carbon is the 13C isotope

In 13C NMR spectroscopy, the sample is irradiated
with a relatively intense range of frequencies that
correspond to precessional frequencies of all protons
in the molecule. As a result, these protons become
saturated, no further absorption of the irradiation
energy is possible, and the protons are no longer
coupled to 13C nuclei.
Proton-decoupled 13C NMR and 1H NMR spectra
                of camphor
13C
    NMR chemical shifts for various classes of
compounds. The δ scale is relative to TMS at δ = 0
The isomeric pairs previously examined as giving very
similar proton NMR spectra can be distinguished by
carbon NMR spectroscopy.
Cyclohexane (A): a single signal at δ 27.1
Alkene (B): two signals at δ 20.4 and δ 123.5
Fulvene (A): five signals
ortho-Xylene (B): four signals
Quinone (A): four signals
Quinone (B): five signals
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