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Nuclei magnetic

A second type of relaxation mechanism, the spin-spm relaxation, will cause a decay of the phase coherence of the spin motion introduced by the coherent excitation of tire spins by the MW radiation. The mechanism involves slight perturbations of the Lannor frequency by stochastically fluctuating magnetic dipoles, for example those arising from nearby magnetic nuclei. Due to the randomization of spin directions and the concomitant loss of phase coherence, the spin system approaches a state of maximum entropy. The spin-spin relaxation disturbing the phase coherence is characterized by T. ... [Pg.1552]

The couplings of other magnetic nuclei to nitrogen have been studied the reader should refer to Axenrod s chapter in the monograph of Witanowski and Webb for details bond coupling in quaternized heterocycles... [Pg.17]

If the oriented nuclei are now irradiated with electromagnetic radiation of the proper frequency, energy absorption occurs and the lower-energy state "spin-flips" to the higher-energy state. When this spin-flip occurs, the magnetic nuclei are said to be in resonance with the applied radiation—hence the name nuclear magnetic resonance. [Pg.441]

FT-NMR (Section 13.4) Fourier-transform NMR a rapid technique for recording XMR spectra in wrhich all magnetic nuclei absorb at the same time. [Pg.1242]

Multiplet (Section 13.11) A pattern of peaks in an NMR spectrum that arises by spin-spin splitting of a single absorption because of coupling between neighboring magnetic nuclei. [Pg.1246]

Van Vleck 8) has shown how the second moment and fourth moment interactions between the magnetic nuclei. [Pg.93]

The fine structure of the spectrum is the splitting of the resonance into sharp peaks. Note that the methyl resonance in ethanol at 8 = 1 consists of three peaks with intensities in the ratio 1 2 1. The fine structure arises from the presence of other magnetic nuclei close to the protons undergoing resonance. The fine structure of the methyl group in ethanol, for instance, arises from the presence of the protons in the neighboring methylene group. [Pg.905]

The process of spin-lattice relaxation involves the transfer of magnetization between the magnetic nuclei (spins) and their environment (the lattice). The rate at which this transfer of energy occurs is the spin-lattice relaxation-rate (/ , in s ). The inverse of this quantity is the spin-lattice relaxation-time (Ti, in s), which is the experimentally determinable parameter. In principle, this energy interchange can be mediated by several different mechanisms, including dipole-dipole interactions, chemical-shift anisotropy, and spin-rotation interactions. For protons, as will be seen later, the dominant relaxation-mechanism for energy transfer is usually the intramolecular dipole-dipole interaction. [Pg.128]

Nuclear Overhauser effects (NOEs) cause changes in the intensity of NMR signals by through-space dipole iipole interactions [36]. The magnitude of an observed NOE between two magnetic nuclei gives useful information on the distances between them. The observed NOE is also related to Brownian... [Pg.17]

The elimination of the need to use paramagnetic doping of the catalyst will facilitate future spectroscopic studies both in a catalyst bed and in single catalyst pellets. For spatially resolved spectroscopy, it could also be advantageous to use magnetic nuclei with a wider spread of chemical shifts as compared with H. Extension to other classes of reactors and reactions is feasible and will be addressed. [Pg.587]

The most important magnetic property by far is the chemical shift of NMR spectroscopy. While proton H) and 13C shieldings hold a prominent place in organic chemistry, other magnetic nuclei such as 15N, 29Si, or 31P but also heavier nuclei such as transition-metals are increasingly important in many areas of chemistry. Obviously, all these nuclei are equally... [Pg.216]

All the magnetic nuclei present in the molecule CH, 13C, 31P, 170, 35C1) are included in the NMR measurements, and the necessary theory is discussed very briefly the reader is referred to suitable texts which he or she can consult in order to learn more about the theoretical aspects. [Pg.221]

When one or more magnetic nuclei interact with the unpaired electron, we have another perturbation of the electron energy, i.e., another term in the spin Hamiltonian ... [Pg.5]

A) If the radical was produced by a chemically straightforward procedure, you usually have some idea of the identity of the radical. How many and what kinds of magnetic nuclei, i.e. nuclei with spins, should be present if your guess is correct ... [Pg.33]

Table A 1.3 Some properties of stable magnetic nuclei... Table A 1.3 Some properties of stable magnetic nuclei...
The information that can be obtained from an epr spectrum can be divided into three forms (i) the 0-factor, (ii) the hyperfine splitting of the spectra due to the interaction of the spin with magnetic nuclei in the radical and (iii) the shape of the observed bands. [Pg.193]

Hyperfine splitting. As was discussed above, one consequence of placing a free electron onto a molecule is to alter its 0-value. Another is that the electron spin comes under the influence of any magnetic nuclei present in the radical, with the result that the spectrum is split into a number of lines centred on the position of the single resonance expected for the simple /transition discussed above. This hyperfine structure is the most useful characteristic ofepr spectra in the identification of an unknown radical species. [Pg.194]

When there are several magnetic nuclei present in the radical, the extension of the argument is straightforward. Each nucleus contributes to the splitting of the spectrum and the a and / levels of the unpaired electron are accordingly split by all the nuclei, with the energies of the resultant levels given by ... [Pg.195]

At this point, some mention of the intensity of the lines observed in epr spectra should be made. In the case of a radical having no magnetic nuclei the difference in the energy of the a and 0 levels is of the order of 0.3 cm . At room temperature, kT is c. 200cm and the Boltzmann equation thus gives the ratio of the number of radicals in the lower state to those in the upper, Np/Na, as 1.0015. The absorption intensity is proportional to this difference and as a consequence epr absorptions are very weak. The phase-sensitive detection employed in epr spectrometers is thus a necessity if these weak... [Pg.195]

The introduction of additional techniques such as Pulsed Fourier Transform NMR spectroscopy (PFT-NMR) has considerably increased the sensitivity of the method, allowing many magnetic nuclei which may be in low abundance, including 13C, to be studied. The additional data available from these methods allow information on polymer structure, conformation and relaxation behaviour to be obtained (1.18.20). [Pg.41]

The pre-eminent advantage of C-nitroso-compounds as spin traps is that in the spin adduct the scavenged radical is directly attached to the nitroxide nitrogen. Consequently, the esr spectrum of the spin adduct is likely to reveal splittings from magnetic nuclei in the trapped radical, and these will greatly facilitate its identification. A simple example is presented in Fig. 2, which shows the spectrum of the spin adduct of the methyl radical with 2-methyl-2-nitroso-... [Pg.12]


See other pages where Nuclei magnetic is mentioned: [Pg.1547]    [Pg.1567]    [Pg.582]    [Pg.441]    [Pg.460]    [Pg.469]    [Pg.469]    [Pg.1251]    [Pg.94]    [Pg.194]    [Pg.64]    [Pg.227]    [Pg.16]    [Pg.17]    [Pg.217]    [Pg.327]    [Pg.308]    [Pg.17]    [Pg.14]    [Pg.19]    [Pg.250]    [Pg.93]    [Pg.120]    [Pg.40]    [Pg.41]    [Pg.89]    [Pg.41]    [Pg.8]    [Pg.16]   
See also in sourсe #XX -- [ Pg.190 ]

See also in sourсe #XX -- [ Pg.190 ]

See also in sourсe #XX -- [ Pg.10 , Pg.17 , Pg.88 , Pg.135 , Pg.141 ]




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A Properties of Magnetically Active Nuclei

Atomic nucleus magnetism

Electric and magnetic fields generated by the nucleus

Electrons and nuclei in magnetic fields

Finite nucleus magnetic interactions

Magnetic Equivalence of Nuclei

Magnetic dipole moment of a nucleus

Magnetic electron-nucleus double

Magnetic field at the nucleus

Magnetic field, nucleus

Magnetic interactions between nuclei

Magnetic moments of nuclei

Magnetic nuclei hydrides

Magnetic nuclei natural abundance

Magnetic nuclei receptivity

Magnetic of nucleus

Magnetic properties of nuclei

Magnetic properties, nuclei

Magnetically equivalent nuclei

NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY PART TWO CARBON-13 SPECTRA, INCLUDING HETERONUCLEAR COUPLING WITH OTHER NUCLEI

Nuclear magnetic resonance active nuclei

Nuclear magnetic resonance electron-nucleus coupling

Nuclear magnetic resonance nuclei

Nuclear magnetic resonance nuclei characteristics

Nuclear magnetic resonance nuclei possibility

Nuclear magnetic resonance nuclei spin angular momentum

Nuclear magnetic resonance spectroscopy different nuclei

Nuclear magnetic resonance spectroscopy other nuclei

Nucleus magnetic moment

Nucleus magnetization, distribution

Point nucleus magnetic properties

Spinning Nuclei in Magnetic Fields

Systems magnetic resonance nuclei

The Nucleus in a Magnetic Field

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