Title: Nuclear Magnetic Resonance
1Nuclear Magnetic Resonance
2Electromagnetic 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)
3Electromagnetic Radiation
4Molecular Spectroscopy
- We study three types of molecular spectroscopy
5A pictorial view of UV/Vis
UV/Vis radiation is measured in nm (wavelength)
6IR Spectroscopy
- IR radiation is measured in cm-1
- This is actually a frequency. Remember that
frequency and wavelength are inversely
proportional.
7NMR Spectroscopy
- NMR uses radiowaves, measured in MHz
8Nuclear 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
9Molecular 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
10Nuclear Spin States
- Spin quantum numbers and allowed nuclear spin
states for selected isotopes of elements common
to organic compounds
11Nuclear 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
12Nuclear Spins in B0
- For 1H and 13C, only two orientations are allowed.
13Nuclear 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)
14Population 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
15Nuclear 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
16NMR 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
17Nuclear 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
18Nuclear 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
19Nuclear 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)
20Nuclear 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
21NMR 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
22NMR 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
23Equivalent 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
24Signal 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
25Chemical Shift - 1H-NMR
26Chemical Shift - 1H-NMR
27Chemical Shift
- Depends on (1) electronegativity of nearby atoms,
(2) the hybridization of adjacent atoms, and (3)
magnetic induction within an adjacent pi bond - Electronegativity
28Chemical Shift
- Hybridization of adjacent atoms
29Chemical 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
30Field currents in benzene
31acetylene
32Alkenes
33Methyl Acetate
34Signal 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
35Signal Splitting (n 1)
- Problem predict the number of 1H-NMR signals
and the splitting pattern of each
36Origins 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
37Origins of Signal Splitting
38Origins of Signal Splitting
- Table 13.8 Observed signal splitting patterns
for an H with 0, 1, 2, and 3 equivalent
neighboring hydrogens
39Origins of Signal Splitting
40Coupling 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
41Ethyl acetate
42Isopropyl alcohol