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
15NMR 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
16Nuclear 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
17Electrons Shield
What causes differences? Electrons shield.
Remove electrons they de-shield.
18Electron Withdrawing groups deshield by removing
electron density
I suck
19Electron density can be added or removed through
the p or s systems
20Field currents in benzene
21Ring currents usually deshield
22acetylene
23Alkenes
24NMR 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
25Nuclear 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)
26Nuclear 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
27Equivalent 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
28Signal 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
29Chemical Shift - 1H-NMR
30Chemical Shift - 1H-NMR
31Chemical Shift
- Depends on (1) electronegativity of nearby atoms,
(2) the hybridization of adjacent atoms, and (3)
magnetic induction within an adjacent pi bond - Electronegativity
32Chemical Shift
- Hybridization of adjacent atoms
33Chemical 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
34Methyl Acetate
35Signal 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
36Signal Splitting (n 1)
- Problem predict the number of 1H-NMR signals
and the splitting pattern of each
37Origins 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
38Origins of Signal Splitting
39Origins of Signal Splitting
- Table 13.8 Observed signal splitting patterns
for an H with 0, 1, 2, and 3 equivalent
neighboring hydrogens
40Origins of Signal Splitting
41Coupling 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
42Ethyl acetate
43Isopropyl alcohol
4413C-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
4513C-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
46Chemical Shift - 13C-NMR
47C8H10
48C7H12O4
49C7H14O
50Interpreting 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
51Interpreting 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.
52Index 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
53Index 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