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Relaxation exchange

An application of dynamic q-space imaging for parenchyma tissue of apple was reported where relaxation/exchange and permeable feature of bio-membrane was considered [53]. [Pg.134]

To complete the two-temperature approximation we should introduce vibrational kinetic relation controlling rates of e ( W -, and VT-relaxation processes and chemical reactions (Potapkin, Rusanov, Fridman, 1984a,b, 1987). They have to be considered as functions of the average number of vibrational quanta in CO2 symmetric valence mode ( i, quantum ftco ), CO2 symmetric deformation mode ( 2. quantum >2), CO2 asynunetric mode ( 3, quantum tws), and in CO vibrations (0(4, quantum <04). Rates of W -relaxation exchange between CO and CO2 molecules (rate coefficient k, ) and between asymmetric and symmetric modes of CO2 molecules in collisions with ar r i components of the mixture (rate... [Pg.277]

NOESY exchange cross-peaks of same sign as the cross-relaxation peaks ROESY exchange cross-peaks of opposite sign as the cross-relaxation peaks Mixed cross-relaxation/exchange pathways may contribute to cross-peaks. [Pg.277]

Spin-spin relaxation (transverse relaxation) Exchange of energy of excited nuclei with other precessing nuclei. It is characterized by the exponential time constant T2. Also, it determines the envelope of the free induction decay in a perfectly uniform magnetic field and the amplitude of the spin echo. [Pg.523]

Treanor C E, Rich J W and Rehm R G 1968 Vibrational relaxation of anharmonic oscillators with exchange-dominated collisions J. Chem. Phys. 48 1798-807... [Pg.1085]

Scalar coupling 0 Relaxation of the coupled spin or exchange Can be Important for T2 Further reading... [Pg.1506]

Woessner D E 1996 Relaxation effects of chemical exchange Encyclopedia of Nuclear Magnetic Resonance ed D M Grant and R K Harris (Chichester Wiley) pp 4018-28... [Pg.1516]

From SCRP spectra one can always identify the sign of the exchange or dipolar interaction by direct exammation of the phase of the polarization. Often it is possible to quantify the absolute magnitude of D or J by computer simulation. The shape of SCRP spectra are very sensitive to dynamics, so temperature and viscosity dependencies are infonnative when knowledge of relaxation rates of competition between RPM and SCRP mechanisms is desired. Much use of SCRP theory has been made in the field of photosynthesis, where stnicture/fiinction relationships in reaction centres have been connected to their spin physics in considerable detail [, Mj. [Pg.1617]

Relaxation or chemical exchange can be easily added in Liouville space, by including a Redfield matrix, R, for relaxation, or a kinetic matrix, K, to describe exchange. The equation of motion for a general spin system becomes equation (B2.4.28). [Pg.2099]

The tenn slow in this case means that the exchange rate is much smaller than the frequency differences in the spectrum, so the lines in the spectrum are not significantly broadened. Flowever, the exchange rate is still comparable with the spin-lattice relaxation times in the system. Exchange, which has many mathematical similarities to dipolar relaxation, can be observed in a NOESY-type experiment (sometimes called EXSY). The rates are measured from a series of EXSY spectra, or by perfonning modified spin-lattice relaxation experiments, such as those pioneered by Floflfman and Eorsen [20]. [Pg.2107]

In the absence of exchange (and ignoring dipolar relaxation), each z magnetization will relax back to equilibrium at a rate governed by its own T, as in (B2.4.44). [Pg.2107]

If the two sites exchange with rate k during the relaxation, tiien a spin can relax either tlirough nonnal spin-lattice relaxation processes, or by exchanging witli the other site, equation (B2.4.45) becomes (B2.4.46). [Pg.2107]

Figure B2.4.8. Relaxation of two of tlie exchanging methyl groups in the TEMPO derivative in figure B2.4.7. The dotted lines show the relaxation of the two methyl signals after a non-selective inversion pulse (a typical experunent). The heavy solid line shows the recovery after the selective inversion of one of the methyl signals. The inverted signal (circles) recovers more quickly, under the combined influence of relaxation and exchange with the non-inverted peak. The signal that was not inverted (squares) shows a characteristic transient. The lines represent a non-linear least-squares fit to the data. Figure B2.4.8. Relaxation of two of tlie exchanging methyl groups in the TEMPO derivative in figure B2.4.7. The dotted lines show the relaxation of the two methyl signals after a non-selective inversion pulse (a typical experunent). The heavy solid line shows the recovery after the selective inversion of one of the methyl signals. The inverted signal (circles) recovers more quickly, under the combined influence of relaxation and exchange with the non-inverted peak. The signal that was not inverted (squares) shows a characteristic transient. The lines represent a non-linear least-squares fit to the data.
For constant temperature dynamics where the constant temperature check box in the Molecular Dynamics Options dialog box is checked, the energy will not remain constant but will fluctuate as energy is exchanged with the bath. The temperature, depending on the value set for the relaxation constant, will approach con-stan cy. [Pg.321]


See other pages where Relaxation exchange is mentioned: [Pg.2107]    [Pg.132]    [Pg.181]    [Pg.2107]    [Pg.277]    [Pg.552]    [Pg.203]    [Pg.205]    [Pg.2107]    [Pg.132]    [Pg.181]    [Pg.2107]    [Pg.277]    [Pg.552]    [Pg.203]    [Pg.205]    [Pg.390]    [Pg.1143]    [Pg.1453]    [Pg.1500]    [Pg.1506]    [Pg.1572]    [Pg.1610]    [Pg.2091]    [Pg.2092]    [Pg.2096]    [Pg.2097]    [Pg.2101]    [Pg.2105]    [Pg.2108]    [Pg.2108]    [Pg.2108]    [Pg.2110]    [Pg.2111]    [Pg.2111]    [Pg.2111]    [Pg.2112]    [Pg.2112]    [Pg.2208]    [Pg.2209]    [Pg.7]    [Pg.321]    [Pg.396]   
See also in sourсe #XX -- [ Pg.407 ]




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