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General Spectroscopy
“Spectroscopy is the study of the nature of energy levels of
matter, and the transitions induced between the by EM
radiation.”
•Energy levels quantised ie have descrete values (electron/nuclear,
nuclear/electron magnetic moments, vibrational, rotational etc).
•Interaction with Electromagnetic (EM) radiation.
•Emmision, Absorption, scattering or resonant.
•Selection rules
MRI, NMR
(energy levels of nuclear
magnetic moments)
Electron Spin Resonance (ESR, EPR)
IR (atomic bond vibrations)
Ultra Violet/visible (electron
transitions)
Xray Cystallography (scattering)
Types of Spectroscopy
Certain nuclei possess a nuclear magnetic moment (eg 1H, 13C, 19F,…)
Nucleus
Where is the signal from?
Patient Molecules 1H Atom 1H Nucleus Compass Needle
“Nuclear Magnetic
moment ”Electron
“spin angular
Momentum”
N
S
Polarisation using Strong Magnet
At atomic level quantum mechanics applies to nuclear magnetic moments (“spins”).
It says only TWO eigenstates are possible, the “spin up” and “spin down” state.
Ener
gy
No net Magnetisation M
M= N↑ - N↓ = 0
Compass Needle
N
S
No magnetic field
Polarisation using Strong Magnet
At atomic level quantum mechanics applies to nuclear magnetic moments (“spins”).
It says only TWO states are possible, the “spin up” and “spin down” state.
Ener
gy
magnetic
field, B S
N
Low energy
High energy
polarisation creates a Net Magnetisation M
This is the origin of MRI signal
M
M= N↑ - N↓ ≈ 6 per million
Compass Needle
N
S
Polarisation using Strong Magnet
At atomic level quantum mechanics applies to nuclear magnetic moments (“spins”).
It says only TWO states are possible, the “spin up” and “spin down” state.
Ener
gy
Compass Needle
N
S
∆E = hν
Frequency, ν
RF radiation of the precise frequency can drive transitions,
1. leading to an adsorption of energy.
2. Creation of transverse magnetisation
Signal Detection• Following pulse of RF radiation, Magnetisation M now precessing in xy plane
• Induces an electric current in the receiver coil. (Analogous to electric generator)
• Frequency of signal same as frequency of precession of M.
MRI Signal
y
x
B0
z
Φ
M
Receiver coil
Time (s)
∝precession
frequency, ωmagnetic field
strength B0
0Bγω =
High Resolution Liquid State Nuclear Magnetic Resonance
1. Chemical Shift
2. J coupling
3. Assigning spectra
4. Examples of metabolites
Chemical Shift
The resonant frequency depends on the main magnetic field B0
BUT, electrons can slightly alter the effective magnetic field
“seen” by a nucleus.
0Bγω =
Within a molecule 1H nuclei have,
• Different “electron environments”
• experience effective magnetic field, Beff
• Resonate at different frequencies
CH3—CH2 — OH
Chemical Shift
Nucleus experiences lower effective magnetic field
Beff = B0 - σB0 = (1- σ)B0
ω = γ(1-σ)B0
Magnetic
field
Electrons
induced to
circulate
Generating a small
additional magnetic
field opposing the
main field.
σ Chemical shift sheilding constant
C C
HA O
F HB
O strongly “electronegative”, ie
pulls electron density towards it.
Nucleus is Well shielded,
resonates at lower frequency
Nucleus is less Well shielded,
resonates at higher frequency
Chemical shift depends on “Function groups”
Example
Fourier
transform
freq
Intensity
C C
HA O
CH3HB
O is electronegative, ie pulls
electron density towards it.
Nucleus is Well shielded,
resonates at lower frequency
Nucleus is less Well shielded,
resonates at higher frequency
Example
ν0δ =
ν - ν0
Chemical Shift- the “ppm scale”
Resonance frequencies vary with magnetic field.
Therefore, Chemical Shift present with δ scale , unit ppm (parts per million)
This allows comparision between measurements made at
different magnetic fields (eg 1.5T and 3T).
Reference Standards
Organic Chemistry - Tetramethylsilane (TMS) define 0 ppm
In-vivo - internal reference e.g. N-acetyl aspartate to define 2.2ppm
CH3
Si
CH3
CH3
CH3
Chemical shift δ (ppm)
Chemical Shift
Effect of neighbouring functional groups
H nucleus become less shielded
Resonant at higher frequency
Chemical shift δ (ppm)
Chemical Shift
Effect of neighbouring functional groups
CSi
C
C
CH
H
H
H
HHH
HH
H
HH
H nuclei are well shielded
Resonant at lower frequency
TMS
C O
H
Chemical shift δ (ppm)
Chemical Shift
Effect of neighbouring functional groups
H nuclei LESS shielded
Resonant at higher frequencyCarbonyl group
Chemical shift δ (ppm)
Chemical Shift
Effect of neighbouring functional groups
C
H
H
For CH2 wide range
of ppm
Methylene group? ?
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA HB
Cl R
HA
Chemical ShiftB
ν
Resonance of HA depends on state of HBElectron
density
(Probability)
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA HB
Cl R
HA
Chemical Shift
Chemical shift +
J coupling
Bα
ν
να
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA HB
Cl R
HA
Chemical Shift
Chemical shift +
J coupling
B βν
νβ
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA HB
Cl R
HA
Chemical Shift
Chemical shift +
J coupling
B βν
ναβ
Overall, molecules chance are 50:50
whether HB is up (α) or down (β), so
see both
Intensity ratio 1 : 1
Called a “Doublet”
α
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA HB
Cl R
HA
Chemical Shift
Chemical shift +
J coupling
J Coupling
Constant Hz
B βν
ναβ
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA H
Cl H
BHA
Chemical Shiftν
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA H
Cl H
Bα
α
HA
Chemical Shift
Chemical shift +
J coupling
ν
ναα
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA H
Cl H
Bβ
β
HA
Chemical Shift
Chemical shift +
J coupling
ν
νββ
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA H
Cl H
Bα
HA
Chemical Shift
Chemical shift +
J coupling
ν
νβ αβ
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA H
Cl H
Bβ
HA
Chemical Shift
Chemical shift +
J coupling
ν
να
βα
J Coupling (spin-spin Coupling)
The magnetic dipoles of 1H can interact via electrons.
C C
HA H
Cl H
Bβ
HA
Chemical Shift
Chemical shift +
J coupling
ν
να
Intensity ratio 1 : 2 : 1
Called a “Triplet”
ββ αββα
αα
J
0 1 1 Singlet
1 2 1 1 Doublet
2 3 1 2 1 Triplet
3 4 1 3 3 1 Quartet
J Coupling (spin-spin Coupling)
“n” magnetically equivalent neighbouring 1H, leads to “n+1” lines in multiplet.
nn+1
lines Intensities Name
C C
HA H
Cl H
H
Pascal’s Triangle
Simple rules for predicting NMR spectra
1. Divide hydrogens 1H into magnetically equivalent groups.
2. Look at functional group, estimate Chemical Shift.
Example Pentanone CH3—CH2 —C —CH2 —CH3
O
These are two magnetically equivalent groups of H
• The CH3 hydrogens (~1.7ppm)
• The CH2 hydrogens (~3.9ppm)
These will have different chemical shifts, hence expect two peaks.
CH2 CH3
0 ppm1.7 ppm3.9 ppm
3. Overall intensity of group proportional to number of
Hydrogens.
CH2
CH3
0 ppm1.7 ppm3.9 ppm
6 x CH3 hydrogens
4x CH2 hydrogens
Hence, ratio of peaks is 6:4
Example Pentanone CH3—CH2 —C —CH2 —CH3
O
Simple rules for predicting NMR spectra
4. J Splitting due to neighbouring 1H, ( n magnetically
equivalent), leads to n+1 lines in multiplet.
CH2
CH3
0 ppm1.7 ppm3.9 ppm
CH3 hydrogen has CH2 as neighbours (2 equivalent protons) .
This splits the CH3 peak into (2+1= 3) ie triplet
CH2 hydrogen has CH3 as neighbours (3 equivalent protons) .
This splits the CH3 peak into (3+1= 3) ie quartet
Example Pentanone CH3—CH2 —C —CH2 —CH3
O
Simple rules for predicting NMR spectra
5. Intensity within multiplet obeys Pascals Triangle
CH2
CH3
0 ppm1.7 ppm3.9 ppm
Example Pentanone CH3—CH2 —C —CH2 —CH3
O
1 Singlet
1 1 Doublet
1 2 1 Triplet
1 3 3 1 Quartet
Quartet 1 : 3 : 3 : 1 Triplet 1 : 2 : 1
Simple rules for predicting NMR spectra
Water suppression (Vapor,Chess) water signal >> metabolites, have to suppress
water signal
Outer volume suppression (see later)
Navigator echo is magnetic field drifts during scans, the navigator echo can be used
as reference. Prevents broadening of spectra.