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NMR SPECTROSCOPY. JM Franconi. MR SPECTROCOPY. Principle of FT NMR spectroscopy. In a spectrum, each signal represent the resonance frequency of a nucleus in a specific environment. Bo is fixed a RF pulse irradiate a broad range of frequency. RF. irradiation. sampling. FT. t.
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NMR SPECTROSCOPY JM Franconi
MR SPECTROCOPY Principle of FT NMR spectroscopy In a spectrum, each signal represent the resonance frequency of a nucleus in a specific environment Bo is fixed a RF pulse irradiate a broad range of frequency RF irradiation sampling FT t spectrum f FID
MR SPECTROCOPY Non selective RF pulse In spectroscopy the RF pulse used is < 100 microsecond RF sinc rectangular g.B1 > 2pF F frequency range
MR SPECTROCOPY RF pulse Magnetisation evolution During RF pulse M rotate Around x direction with an angle: Bo z Q = g. t . B1 q Mz M y O Mxy x
MR SPECTROCOPY spectrum parameter chemical shift f f1 f2 f3 f4 A same nucleus can have different resonance frequency
MR SPECTROCOPY chemical shift phenomenon Bo Bo Bo1 H2 Bo2 H1 O C Bo2 Bo1
MR SPECTROCOPY chemical shift measurement u i u ref reference f paramagnetic low field high electronégativity Diamagnetic High field Low electronégativity
MR SPECTROCOPY J coupling J coupling is an interaction between close nuclei This interaction is independant of Bo field It does not exit on one isolated molecule JAB fA fB f
MR SPECTROCOPY J scalar coupling H1 H1 is influenced by the 2 H2 sites Jcoupling is transported by chemical bond C C 50%(+1/2) H2 50%(-1/2) f1+dBH2 f1 f1- dBH2
MR SPECTROCOPY J dipolar coupling Coupling is also possible directly through space r H1 H2 1/r6
MR SPECTROCOPY J coupling The Nuclei magneticaly equivalent have the same chemical shift. They do not show any coupling effect Ha C fHa = fHb = fHc C Hb Hc
MR SPECTROCOPY J coupling Rules for multiplicity determination A I nucleus coupled to n spin S give a signal with: 2.n.S + 1 componants The componants relative intensity are given by a binomial Distribution.
MR SPECTROCOPY Signal area NMR spectroscopy is a quantitative method f
MR SPECTROCOPY spectrum quality DR Concept of digital resolution AT = N.DW DW t f At R = 1/AT Digital resolution FT Frequency domain Time domain T2* TR=1/pT2* f t True NMR resolution CONDITION: TR > DR
MR SPECTROCOPY Sampling rules Application of Nquist theorem DW f1 f2 f1 f2 f2 F=1/Dw 2. F. Aq = N
MR SPECTROCOPY Sensitivity • The gyromagnetic ratio and the natural isotopic abundance • determine the NMR signal available - the nucleus sensitivity is proportional to Bo2 and g3
MR SPECTROCOPY concept of population and coherence Mz Mz MR signal E2 RF E2 E1 E1 Cohérence=transition population
MR SPECTROCOPY Polarisation transfer (NOE) C +1/2 -1/2-1/2 Transition C13 C -1/2+1/2 +1/2 Long distance +1/2 H Transition H1 Niveau C13 +1/2-1/2 -1/2 +1/2+1/2 H Niveau H1 2 independant level of energy system of 4 levels of energy NO COUPLING COUPLING
MR SPECTROCOPY Polarisation transfer (NOE) dH = 4.dC f f +5 -dH-dC +dH-dC C13 transition -dH+dC H1 transition dH-dC -dH-dC -3 -dH+dC dH+dC POLARISATION H1 TRANSITION SATURATION
180° te/2 90° SEQUENCE SPIN ECHO SEQUENCE
SEQUENCE DEMI TOUR!
SEQUENCE ECHO = coherence recovery
o o 90 180 Mxy T2 T2* t FID ECHO DE SPIN SEQUENCE SPIN ECHO
SPIN ECHO SEQUENCE 180° 90° TR TE RF GS GP DAC on GR CONCEPT OF PULSE SEQUENCE
NMR SPECTROSCOPY APPLICATION • Chemical structure determination (protein, ADN,…) • Quantitative measurement • (isotopic enhancement determination) • food and beverage quality control • Spectroscopy in vivo (metabolism caracterisation)