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NMR-spectroscopy Kjernemagnetisk resonans
History Physical requirements Principles Theory Interpretation of spectra
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History 1946: NMR discovered 1949: Chemical shift
1953: First commercial high resolution instrument 1960: Structure determination of organic molecules 1970: FT-NMR 1971 – 75 : 2D-NMR 1973: MR-tomography
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An example
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Schematic diagram of NMR
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Physical requirements
1.Nuclear spin (12C and 16O are NMR silent) Magnetic moment 2. Magnetic field Number of spin states in the presence of a magnetic field = 2I +1 1H and 13C # spin states = 2 2H # spin states = 3
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ν = frequency, B0 = applied magnetic field, γ = magnetogyric ratio
ΔE = hν ν = γB0/2π ν = frequency, B0 = applied magnetic field, γ = magnetogyric ratio
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N1 = number of nuclei in the α state
N1/N2 is given by Boltzmann’s distribution: At 60 MHz: excess in α state is 9 nuclei in a population of 2 million. The N1/N2 ratio increases with increasing B0.
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Net magnetisation
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Net magnetisation vector
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FT-NMR
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Magnetic field data
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Properties
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Sample preparation
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Chemical shift
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Electron density
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δ-scale Tetramethylsilane, Si(Me)4 is used as reference in both 1H and 13C TMS: - The nuclei are strongly shielded and appear to the right H and 4 13C nuclei - One singel peak - Chemically inert - Non toxic
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Carbon 13 and proton
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Integration
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Integration CW(1H): The area is proportional to the number of nuclei in the peak FT(1H): Same as CW given that the relaxtion time is long enough (2-3 s) FT(13C): Not commonly used due to slow relaxtion and large difference in relaxtion rates for different 13C nuclei.
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