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Proton nuclei

The important experiments for our purposes are the correlation experiments, where both axes are chemical shift axes. Certainly the most useful of these is the proton-proton correlation experiment, initially known as COSY (for Correlated SpectroscopY) and now, to make things more precise, as H,H COSY. This experiment is important, as it provides direct information on which proton nuclei couple with which. [Pg.37]

H longitudinal and transverse relaxation constants are the most measured parameters in investigating small molecules/polymer interactions, as the high natural abundance of the proton nuclei ensures a rapid measurement and excellent signal to noise. [Pg.187]

In the case of pharmaceutical solids that are dominated by carbon and proton nuclei, the dipole-dipole interactions may be simplified. The carbon and proton nuclei may be perceived as dilute and abundant based upon then-isotopic natural abundance, respectively (Table 1). Homonuclear 13C—13C dipolar interactions essentially do not exist because of the low concentration of 13C nuclei (natural abundance of 1.1%). On the other hand, H—13C dipolar interactions contribute significantly to the broad resonances, but this heteronuclear interaction may be removed through simple high-power proton decoupling fields, similar to solution-phase techniques. [Pg.98]

NOESY NMR spectroscopy is a homonuclear two-dimensional experiment that identifies proton nuclei that are close to each other in space. If one has already identified proton resonances in one-dimensional NMR spectroscopy or by other methods, it is then possible to determine three dimensional structure through NOESY. For instance, it is possible to determine how large molecules such as proteins fold themselves in three-dimensional space using the NOESY technique. The solution structures thus determined can be compared with solid-state information on the same protein obtained from X-ray crystallographic studies. The pulse sequence for a simple NOESY experiment is shown in Figure 3.23 as adapted from Figure 8.12 of reference 19. [Pg.110]

Consequently, the splitting observed is due to the fact that TRIMEB induces nonequivalence in the proton nuclei of the two enantiomers of the allenes, thus enabling one to determine the enantiomeric purities by using a chiral solvating agent. In all cases examined the extent of the nonequivalence, i.e. the difference of the proton chemical shifts of the two enantiomers in the presence of TRIMEB, can be increased by increasing the... [Pg.174]

The carbon nuclei are to be identified with I, the proton nuclei with S, and the carbon-proton internuclear distance with r. The spectral density is the Fourier transform of a correlation function which is usually based on a probabilistic description of the motion modulating the dipole-dipole interactions. The spin-spin relaxation time, T2, is usually written directly as a function of spectral densities ( ). [Pg.272]

Protons, nuclei and electrons in cosmic rays would appear to inherit their energy spectrum from this mechanism, associated with shock waves. A non-thermal component in X-ray emissions from the recently discovered remnant of the 1006 supernova provides direct confirmation. [Pg.119]

The HMBC correlates proton nuclei with carbon nuclei that are separated by more than one bond (Figure 2.2). The experiment is normally optimized for Vch and VcH couplings however, the intensity of the crosspeaks generated by this experiment... [Pg.44]

The hyperfine interactions of proton nuclei with the unpaired electron in a radical splits the proton signals into doublets with large coupling constants (up to 100 MHz) in comparison to the J values of 10 Hz observed in NMR spectroscopy. For the small magnetic field employed in an ESR spectrometer, all uncoupled protons absorb at effectively the same rf. The ENDOR spectmm appears as a series of doublets with lines spaced equally upheld and downfield from the expected absorbance of an uncoupled proton. [Pg.131]

This means that the electron goes from naphthalene A with a particular set of +V2, —V2 proton nuclei to naphthalene B with a different set. The result is that the lines broaden and, if the exchange is very fast, the splitting vanishes. Because the splittings are about 5 gauss (14 MHz), the mean lifetime before exchange has to be about 10-8 sec or less to obscure the splitting (see Sections 27-1 and 27-2). [Pg.1368]

Carbon resonances arising from both nonprotonated and proto-nated aromatic carbons may appear at the same frequency under proton decoupling. Yet these two resonances could possess very different relaxation behavior and in a solid could evolve very differently due to local proton dipolar fields which attenuate with the carbon-proton distances as 1/rcH When the spin locking pulse for proton nuclei is turned off, carbons with directly bound protons such as methines and methylenes rapidly dephase in the local proton fields and their spectral response is rapidly diminished. The rapid internal motion of CH3 groups greatly decreases the effectiveness of methyl protons. Nonprotonated carbons are only dephased by remote and therefore... [Pg.89]

Here, yH, yc and Wh, o>c are the gyromagnetic ratios and Larmor frequencies of the carbon and proton nuclei, respectively h (=/i/27r) is Planck s constant rc.H is the C—H bond length noted earlier and N is the number of protons directly attached to the carbon atom under consideration. The n.O.e. value in Eq. 14 depends neither on the number of protons nor on the C—H distance, in contrast to the other two parameters. This means that the T, and T2 values of the carbon nuclei are affected by neighboring intramolecular protons. The shortest distances (1.08-1.09 A) involve directly attached protons, making them the main contributors to the relaxation of a carbon nucleus. [Pg.69]

The behavior of the trimethylsilyl-substituted cyclopentadienylthallium(I) compound Llllk in solution differs from that of the so far described thallium complexes. The air-stable species LHIk is fairly soluble even in aromatic solvents and behaves as a covalent monomer. Furthermore, spin-spin coupling between the 205T1 nucleus and the ring proton nuclei and the13C and H nuclei of the trimethylsilyl groups has been observed (175). A halfsandwich structure in solution and in the gas phase has been suggested for this 7i complex. [Pg.255]

The proton nuclei have spins m = Vi, indicated as + and or as t and j.. The occurrence of the different proton spins of CH2 are (H)/ (Tl and equivalent, ) and (H). The three protons of the CH3 group feel the different magnetic fields of these proton spins and the PNMR spectrum exhibits a CH3 peak which is composed of three peaks with relative intensities 1 2 1. On the other hand the occurrence of the different proton spins of CH3 are (TTT)/ (Hi/ Tit/ and ITT)/ (Hi/ Hi and j T) and (HI)- The two protons of the CH2 group feel the different magnetic fields of these proton spins and the PNMR spectrum exhibits a CH2 peak which is composed of four peaks with relative intensities 1 3 3 1. [Pg.371]

Proton nuclei located at different positions within the small molecules and amino adds that were investigated exhibit similar degrees of spin-probe accessibility as shown by the similar values of slope d(l/Ti)/dC for these protons in the presence of the neutral spin-probe IV. This experimental observation is consistent with the theoretical estimation of spin-probe accessibility as studied by computer-assisted molecular modeling of the various amino acid/spin-probe encounter complexes in our study. [Pg.154]

For the molecular case, the essential conclusion is that the orbital must have some s (or cr) character for the impaired electron to interact with a magnetic nucleus. Consider however the case of the benzene radical anion, in which the electron is usually described as being in a tt orbital with a node in the molecular plane. As a consequence no coupling with the proton nuclei is expected, a prediction clearly in conflict with the hyperfme splitting of 3.75 gauss seen in the ESR spectrum of this species as shown in Fig. 2. Flow, then, does the unpaired tt electron density appear at the Ft nucleus ... [Pg.458]

In a continuing study(20), these experiments were applied to five fulvic and humic samples. In addition, the DEPT pulse sequence was used. This technique allows for a further discrimination between singly and doubly protonated nuclei. They found that all five samples react in the same manner. Reaction products of hydroxylamine with esters were observed. Other resonances discovered were attributable to the tautomeric forms of the nitrosophenol and monooxime derivatives of quinones. Thus, this study provides indirect evidence for the presence of quinones in humic material and also suggests the possible presence of cyclic... [Pg.72]

Atoms consist of very small, very dense nuclei surrounded by clouds of electrons at relatively great distances from the nuclei. All nuclei contain protons nuclei of all atoms except the common form of hydrogen also contain neutrons. [Pg.184]


See other pages where Proton nuclei is mentioned: [Pg.175]    [Pg.902]    [Pg.159]    [Pg.22]    [Pg.9]    [Pg.249]    [Pg.262]    [Pg.286]    [Pg.130]    [Pg.195]    [Pg.46]    [Pg.564]    [Pg.199]    [Pg.320]    [Pg.323]    [Pg.444]    [Pg.10]    [Pg.16]    [Pg.237]    [Pg.511]    [Pg.320]    [Pg.323]    [Pg.370]    [Pg.518]    [Pg.155]    [Pg.518]    [Pg.345]    [Pg.72]    [Pg.275]   
See also in sourсe #XX -- [ Pg.70 ]




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Between Protons and Other Nuclei

Coupling of Protons to Other Important Nuclei

Light proton-rich nuclei

NMR Spectroscopy of Nuclei Other Than Protons

Nuclei other than the proton

Nuclei proton signals

Nucleus neutron-proton ratios

Nucleus proton-rich

Proton A positively charged particle atomic nucleus

Protonated heteroaromatic nucleus

Reactions of protons with light nuclei

THE ATOMIC NUCLEUS IS MADE OF PROTONS AND NEUTRONS

The Stability of a Nucleus Is Determined Primarily by Its Neutron-to-Proton Ratio

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