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Relaxation a and

Fig. 5.1. The semiclassical description of angular momentum distribution relaxation (a) and rotational energy relaxation at Ea — 0 (6). Fig. 5.1. The semiclassical description of angular momentum distribution relaxation (a) and rotational energy relaxation at Ea — 0 (6).
The properties of zeolitic water and the behavior of the exchangeable cations can be studied simultaneously by dielectric measurements (5, 6). In X-type zeolites Schirmer et al. (7) interpreted the dielectric relaxation as a jump of cations from sites II to III or from sites II to II. Jansen and Schoonheydt found only relaxations of cations on sites III in the dehydrated zeolites (8) as well as in the hydrated samples (9). Matron et al. (10) found three relaxations, a, (, and 7, in partially hydrated and hydrated NaX. They ascribed them respectively to cations on sites I and II, on sites III, and to water molecules. [Pg.103]

CSA cross-correlated relaxation, a and torsional angles in nucleotides Measurement of differential DQ-ZQ 33... [Pg.307]

Fig. 12.8. Schematic representation of a sarcomere in the relaxed (a) and contracted (b) state (according to Gault, 1992). 1 I band, 2 A band, 3 Z line, 4 M line, 5 thin filament, 6 thick filament, 7 H zone. Cross section I thin filaments near the Z line, II overlapping thick and thin filaments. III thick filaments, IV M line... Fig. 12.8. Schematic representation of a sarcomere in the relaxed (a) and contracted (b) state (according to Gault, 1992). 1 I band, 2 A band, 3 Z line, 4 M line, 5 thin filament, 6 thick filament, 7 H zone. Cross section I thin filaments near the Z line, II overlapping thick and thin filaments. III thick filaments, IV M line...
Cooperative diffusion of transient polymer networks, heterogeneity mode related to polymer self-diffusion in diblock copolymers, entanglement mode, chain reptation, viscoelastic relaxation, diffusion of clusters Viscoelastic relaxation, a- and 3-relaxation... [Pg.178]

It is important to recognize the approximations made here the electric field is supposed to be sulficiently small so that the equilibrium distribution of velocities of the ions is essentially undisturbed. We are also assuming that the we can use the relaxation approximation, and that the relaxation time r is independent of the ionic concentration and velocity. We shall see below that these approximations break down at higher ionic concentrations a primary reason for this is that ion-ion interactions begin to affect both x and F, as we shall see in more detail below. However, in very dilute solutions, the ion scattering will be dominated by solvent molecules, and in this limiting region A2.4.31 will be an adequate description. [Pg.571]

L is Avagadro s constant and k is defined above. It can be seen that there are indeed two corrections to the conductivity at infinite dilution tire first corresponds to the relaxation effect, and is correct in (A2.4.72) only under the assumption of a zero ionic radius. For a finite ionic radius, a, the first tenn needs to be modified Falkenliagen [8] originally showed that simply dividing by a temr (1 -t kiTq) gives a first-order correction, and more complex corrections have been reviewed by Pitts etal [14], who show that, to a second order, the relaxation temr in (A2.4.72) should be divided by (1 + KOfiH I + KUn, . The electrophoretic effect should also... [Pg.585]

Mullin A S and Schatz G C (eds) 1997 Highly Excited Molecules Relaxation, Reaction and Structure (ACS Symp. Ser. 678) (Washington, DC American Chemical Society)... [Pg.1003]

Tabor M, Levine R D, Ben-Shaul A and Steinfeld J I 1979 Microscopic and macroscopic analysis of non-linear master equations vibrational relaxation of diatomic molecules Mol. Phys. 37 141-58... [Pg.1085]

Tjandra N, Szabo A and Bax A 1996 Protein backbone dynamics and N-15 chemical shift anisotropy from quantitative measurement of relaxation interference effected. Am. Chem. Soc. 118 6986-91... [Pg.1518]

Figure Bl.14.6. J -maps of a sandstone reservoir eore whieh was soaked in brine, (a), (b) and (e), (d) represent two different positions in the eore. For J -eontrast a saturation pulse train was applied before a standard spin-eeho imaging pulse sequenee. A full -relaxation reeovery eiirve for eaeh voxel was obtained by inerementing the delay between pulse train and imaging sequenee. M - ((a) and (e)) and r -maps ((b) and (d)) were ealeulated from stretehed exponentials whieh are fitted to the magnetization reeovery eurves. The maps show the layered stnieture of the sample. Presumably -relaxation varies spatially due to inliomogeneous size distribution as well as surfaee relaxivity of the pores. (From [21].)... Figure Bl.14.6. J -maps of a sandstone reservoir eore whieh was soaked in brine, (a), (b) and (e), (d) represent two different positions in the eore. For J -eontrast a saturation pulse train was applied before a standard spin-eeho imaging pulse sequenee. A full -relaxation reeovery eiirve for eaeh voxel was obtained by inerementing the delay between pulse train and imaging sequenee. M - ((a) and (e)) and r -maps ((b) and (d)) were ealeulated from stretehed exponentials whieh are fitted to the magnetization reeovery eurves. The maps show the layered stnieture of the sample. Presumably -relaxation varies spatially due to inliomogeneous size distribution as well as surfaee relaxivity of the pores. (From [21].)...
Attard J J, Doran S J, Flerrod N J, Carpenter T A and Flail L D 1992 Quantitative NMR spin-lattice-relaxation imaging of brine in sandstone reservoir cores J. Magn. Reson. 96 514-25... [Pg.1545]

This is the famous Lorentzian fimction which is very often found for spectra of radicals in solution. In order to detenuiue the relaxation times and T2, a series of EPR spectra is recorded with the MW power varying... [Pg.1553]

K, L, M,. ..), 5 is the energy shift caused by relaxation efiects and cp is the work fimction of tlie spectrometer. The 5 tenn accounts for the relaxation effect involved in the decay process, which leads to a final state consisting of a heavily excited, doubly ionized atom. [Pg.1858]

Floffman R A and Forsen S 1966 Transient and steady-state Overhauser experiments in the investigation of relaxation prooesses. Analogies between ohemioal exohange and relaxation J. Chem. Phys. 45 2049-60... [Pg.2113]

Sohaublin S, FIdhener A and Ernst R R 1974 Fourier speotrosoopy of non-equilibrium states. Applioation to CIDNP, Overhauser experiments and relaxation time measurements J. Magn. Reson. 13 196-216... [Pg.2113]

Averbukh I Sh, Blumenfeld L A, Kovarsky V A and Perelman N F 1986 A model of the mechanism of enzyme action in terms of protein conformational relaxation Blochim. Blophys. Acta. 873 290-6... [Pg.2848]

How does one monitor a chemical reaction tliat occurs on a time scale faster tlian milliseconds The two approaches introduced above, relaxation spectroscopy and flash photolysis, are typically used for fast kinetic studies. Relaxation metliods may be applied to reactions in which finite amounts of botli reactants and products are present at final equilibrium. The time course of relaxation is monitored after application of a rapid perturbation to tire equilibrium mixture. An important feature of relaxation approaches to kinetic studies is that tire changes are always observed as first order kinetics (as long as tire perturbation is relatively small). This linearization of tire observed kinetics means... [Pg.2950]

Figure C3.2.12. Experimentally observed electron transfer time in psec (squares) and theoretical electron transfer times (survival times, Tau a and Tau b) predicted by an extended Sumi-Marcus model. For fast solvents tire survival times are a strong Emction of tire characteristic solvent relaxation dynamics. For slower solvents tire electron transfer occurs tlirough tire motion of intramolecular degrees of freedom. From [451. Figure C3.2.12. Experimentally observed electron transfer time in psec (squares) and theoretical electron transfer times (survival times, Tau a and Tau b) predicted by an extended Sumi-Marcus model. For fast solvents tire survival times are a strong Emction of tire characteristic solvent relaxation dynamics. For slower solvents tire electron transfer occurs tlirough tire motion of intramolecular degrees of freedom. From [451.
Mullin A S, Miohaels C A and Flynn G W 1995 Moleoular superoollisions evidenoe for large energy transfer in the oollisional relaxation of highly vibrationally exoited pyrazine by COj J. Chem. Phys. 102 6032-45... [Pg.3014]

Flynn G W, Michaels C A, Tapalian C, Lin Z, Sevy E and Muyskens M A 1997 Infrared laser snapshots vibrational, rotational and translational energy probes of high energy collision dynamics Highly Excited Molecules Relaxation, Reaction, and Structure ed A Mullin and G Schatz (Washington, DC ACS)... [Pg.3015]

Wall M C, Stewart B A and Mullin A S 1998 State resolved oollisional relaxation of highly vibrationally exoited pyridine ( ii = 38,000 om ) and CO2 influenoe of a permanent dipole moment J. Chem. Rhys. 108 6185-96... [Pg.3016]

Voth G A and Hoohstrasser R M 1996 Transition state dynamios and relaxation prooesses in solutions a frontier of physioal ohemistry J. Phys. Chem. 100 13034-49... [Pg.3049]

Kenkre V M, Tokmakoff A and Payer M D 1994 Theory of vibrational relaxation of polyatomio moleoules in liquids J. Chem. Phys. 101 10618-29... [Pg.3050]

Nitzan A and Jortner J 1973 Vibrational relaxation of a moleoule in a dense medium Mol. Phys. 25 713-34... [Pg.3050]

Everitt K F, Egorov S A and Skinner J L 1998 Vibrational energy relaxation in liquid oxygen Chem. Phys. 235 115-22... [Pg.3051]

From a mathematical point of view, conformations are special subsets of phase space a) invariant sets of MD systems, which correspond to infinite durations of stay (or relaxation times) and contain all subsets associated with different conformations, b) almost invariant sets, which correspond to finite relaxation times and consist of conformational subsets. In order to characterize the dynamics of a system, these subsets are the interesting objects. As already mentioned above, invariant measures are fixed points of the Frobenius-Perron operator or, equivalently, eigenmodes of the Frobenius-Perron operator associated with eigenvalue exactly 1. In view of this property, almost invariant sets will be understood to be connected with eigenmodes associated with (real) eigenvalues close (but not equal) to 1 - an idea recently developed in [6]. [Pg.104]

Specinfo, from Chemical Concepts, is a factual database information system for spectroscopic data with more than 660000 digital spectra of 150000 associated structures [24], The database covers nuclear magnetic resonance spectra ( H-, C-, N-, O-, F-, P-NMR), infrared spectra (IR), and mass spectra (MS). In addition, experimental conditions (instrument, solvent, temperature), coupling constants, relaxation time, and bibliographic data are included. The data is cross-linked to CAS Registry, Beilstein, and NUMERIGUIDE. [Pg.258]

Bernstein, B., Kearslcy, E.A. and Zapaa, L., 1963. A study of stress relaxation with finite strain. Trans. Soc. Rheol. 7, 391-410. [Pg.15]


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See also in sourсe #XX -- [ Pg.224 ]




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A-Relaxation

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