1. To here!
Nuclear Magnetic Resonance (NMR) Spectroscopy
From here
O
Dr.R.Srinivasan
Dean & Professor
Dept of Pharmaceutical Chemistry & Analysis
Faculty of Pharmacy
Bharath Institute of Higher Education & Research
2. The Nobel Prize in Physics 1952
"for their development of new methods for nuclear magnetic
precision measurements and discoveries in connection
therewith "
Felix Bloch Edward Mills Purcell
3. Magnetic nuclei are in resonance with external magnetic field if they absorb
energy and spin-flip from low energy state (parallel orientation) to high energy
state (antiparallel orientation).
4. 4
atomic nuclei in absence
of magnetic field
atomic nuclei in presence
of external magnetic field
atomic nuclei can either align parallel
(lower E) or antiparallel (higher E)
5. Magnetic nuclei are in resonance with external magnetic field if they absorb
energy and spin-flip from low energy state (parallel orientation) to high energy
state (antiparallel orientation).
6. Dependence of the difference in energy between lower and
higher nuclear spin levels of the hydrogen atom
7. Dependence of the difference in energy between lower and
higher nuclear spin levels of the hydrogen atom
Nuclei in different environments (i.e. with different amounts of electron
density around them) will require different amounts of energy to flip to
higher energy different spin state
8. 8
Magnetic:
oAll nuclei with odd number of
protons
oAll nuclei with odd number of
neutrons
Nonmagnetic:
oNuclei with even number of
both protons and neutrons
14. The Nobel Prize in Chemistry 1991
"for his contributions to the development of the
methodology of high resolution nuclear magnetic
resonance (NMR) spectroscopy"
Richard R. Ernst
15. 900 MHz NMR spectrometer
Center for Biomolecular NMR, Heinrich-Heine-Universit辰t D端sseldorf
State-of-the-art
18. Fig. 13-6, p. 447
13
C NMR spectrum
1-pentanol : 1 scan
19. Fig. 13-6, p. 447
13
C NMR spectrum
1-pentanol : 1 scan
13
C NMR spectrum
1-pentanol : 200 scans
20. The Nature of NMR Absorptions
1
H NMR spectrum
13
C NMR spectrum
21. The Nobel Prize in Chemistry 2002
"for his development of nuclear magnetic resonance
spectroscopy for determining the three-dimensional structure
of biological macromolecules in solution"
Kurt W端thrich
22. The Nobel Prize in Medicine 2003
"for their discoveries concerning magnetic resonance imaging "
Paul C. Lauterbur Sir Peter Mansfield
23. More energy to flip nucleus Less energy to flip nucleus
, ppm
chemical shift
=
observed from standard
spectrometer in MHz
H0
2
= gyromagnetic ratio (differs for each nucleus)
=
(obs) - (TMS)
spectrometer in MHz
38. Fig. 11-13, p. 424
Spin Spin Splitting
Absorption of a proton can split into multiple peaks (multiplet)
Tiny magnetic field produced by one nucleus affects magnetic field
felt by neighboring nuclei
#3: Since a nucleus is a charged particle in motion, it will develop a magnetic field. 1H and 13C have nuclear spins of 1/2 and so they behave in a similar fashion to a simple, tiny bar magnet. In the absence of a magnetic field, these are randomly oriented but when a field is applied they line up parallel to the applied field, either spin aligned or spin opposed. The more highly populated state is the lower energy spin state spin aligned situation. Two schematic representations of these arrangements are shown above.
#5: Since a nucleus is a charged particle in motion, it will develop a magnetic field. 1H and 13C have nuclear spins of 1/2 and so they behave in a similar fashion to a simple, tiny bar magnet. In the absence of a magnetic field, these are randomly oriented but when a field is applied they line up parallel to the applied field, either spin aligned or spin opposed. The more highly populated state is the lower energy spin state spin aligned situation. Two schematic representations of these arrangements are shown above.
#9: Figure 13.4: Schematic operation of an NMR spectrometer. A thin glass tube containing the sample solution is placed between the poles of a strong magnet and irradiated with rf energy.
#18: Figure 13.6: Carbon-13 NMR spectra of 1-pentanol, CH3CH2CH2CH2CH2OH. Spectrum (a) is a single run, showing the large amount of background noise. Spectrum (b) is an average of 200 runs.
#19: Figure 13.6: Carbon-13 NMR spectra of 1-pentanol, CH3CH2CH2CH2CH2OH. Spectrum (a) is a single run, showing the large amount of background noise. Spectrum (b) is an average of 200 runs.
#26: Figure 13.7: Chemical shift correlations for 13C NMR.
#27: Figure 13.7: Chemical shift correlations for 13C NMR.
#28: List of shifts based on functional groups. Divide spectrum in half (sp2 vs sp3).
EN atoms cause shift downfield (left). EN atoms attract electrons so more deshielded and come into resonance at a lower field.
#31: Figure 13.10: DEPTNMR spectra for 6-methyl-5-hepten-2-ol.
Part (a) is an ordinary broadband-decoupled spectrum, which shows signals for all eight carbons.
#36: 2 kinds of equivalent protons. Different height peaks. Can measure yourself if get step as show. Get 1:3 ratio but there are 12 Hs so 3:9 which correlates to structure.
#38: Figure 11.13
The 1H NMR spectrum of bromoethane, CH3CH2Br. The CH2Br protons appear as a quartet at 3.42 隆, and the CH3 protons appear as a triplet at 1.68 隆. Go to this books student companion site at www.cengage.com/chemistry/mcmurry to explore an interactive version of this figure.
#39: Figure 13.13: The 1H NMR spectrum of bromoethane, CH3CH2Br. The CH2Br protons appear as a quartet at 3.42隆, and the CH3 protons appear as a triplet at 1.68隆.
#40: Figure 13.13: The 1H NMR spectrum of bromoethane, CH3CH2Br. The CH2Br protons appear as a quartet at 3.42隆, and the CH3 protons appear as a triplet at 1.68隆.
#42: Figure 11.15
The 1H NMR spectrum of 2-bromopropane. The CH3 proton signal at 1.71 隆 is split into a doublet, and the CHBr proton signal at 4.28 隆 is split into a septet. Note that the distance between peaksthe coupling constantis the same in both multiplets. Note also that the outer two peaks of the septet are so small as to be nearly lost.
#43: Figure 11.15
The 1H NMR spectrum of 2-bromopropane. The CH3 proton signal at 1.71 隆 is split into a doublet, and the CHBr proton signal at 4.28 隆 is split into a septet. Note that the distance between peaksthe coupling constantis the same in both multiplets. Note also that the outer two peaks of the septet are so small as to be nearly lost.
#44: Figure 11.16
The 1H NMR spectrum of p-methoxypropiophenone.
#46: Figure 13.19: The 1H NMR spectrum of trans-cinnamaldehyde. The signal of the proton at C2 (blue) is split into four peaksa doublet of doubletsby the two nonequivalent neighboring protons.
#47: Figure 13.19: The 1H NMR spectrum of trans-cinnamaldehyde. The signal of the proton at C2 (blue) is split into four peaksa doublet of doubletsby the two nonequivalent neighboring protons.