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Observing Diffusion

Ruiter A G T, Veerman J A, Garoia-Para]o M F and van Huist N F 1997 Singie moieouie rotationai and transiationai diffusion observed by near-fieid soanning optioai miorosoopy J. Chem. Phys. A 101 7318-23... [Pg.2509]

Emphasis Aims principally to eliminate influence diffusion, observe intcrfacial happenings. Prefers Tafcl region Aims principally to reduce influence interfacial happenings, observe diffusion monitor entities in solution. Prefers reversible region... [Pg.704]

Fasten the tube in an inclined position in a clamp of a stand and heat the layer of ammonium chloride below the stopper. What explains the change in the colour of the litmus paper What law does the rate of gas diffusion observe Which of the gases obtained as a result of the thermal dissociation of ammonium chloride diffuses more rapidly, and how many times Write the equation of thermal dissociation of ammonium chloride. [Pg.129]

Add a drop of food coloring to each glass. The drop will sink to the bottom and then begin to diffuse. Observe how long it takes until the water is uniformly colored. [Pg.495]

The experimental evidences for these conclusions derive mainly from low-temperature spectra of isolated molecules in rigid matrices.62,63 The diffuseness observed ranges from a few tenths of a cm-1 to thousands of cm-1. In the case of a relatively simple molecule like naphthalene that has two nearby states (S at 31,680 cm-1, and S2 at 34,420 cm-1) a careful study of the second state shows many relatively sharp lines emerging from a diffuse background.64,65 It appears that these sharp transitions can be associated with vibrational levels of the lower electronic state, and that the intensity is borrowed from the second state by the mixing of vibronic states having different electronic parentage in the Born-Oppenheimer representation. [Pg.175]

Theory for the self- and tracer-diffusion of a diblock copolymer in a weakly ordered lamellar phase was developed by Fredrickson and Milner (1990). They modelled the interactions between the matrix chains and a labelled tracer molecule as a static, sinusoidal, chemical potential field and considered the Brownian dynamics of the tracer for small-amplitude fields. For a macroscopically-oriented lamellar phase, they were able to account for the anisotropy of the tracer diffusion observed experimentally. The diffusion parallel and perpendicular to the lamellae was found to be sensitive to the mechanism assumed for the Brownian dynamics of the tracer. If the tracer has sufficiently low molecular weight to be unentangled with the matrix, then its motion can be described by a Rouse model, with an added term representing the periodic potential (Fredrickson and Bates 1996) (see Fig. 2.50). In this case, motion parallel to the lamellae does not change the potential on the chains, and Dy is unaffected by... [Pg.99]

For finite 8, the effective diffusion observation time A in equation (17) takes the reduced value Ar = A-8/3 [35],... [Pg.130]

Investigation of the microscopic origin of these TLSs has demonstrated the feasibility of modulating resonance shifts in a single molecule by interrogation of neighboring solvent molecules coupled to the system.1158 In poly(methyl methacrylate) doped with free base phthalocyanine and small amounts of water, it has been shown that reorientation of nearby water molecules is the source of spectral diffusion observed in the phthalocyanine. [Pg.6]

The orientational diffusion observed by intermolecular Raman techniques is not the diffusion of single molecules, but rather arises from collective effects. For symmetric tops, the collective orientational correlation time rcon is related to the single-molecule orientational correlation time rsm via... [Pg.493]

Figure 6.4 Observed diffusivity in a canopy normalized by the mean velocity and stem diameter. Vertical bars indicate one standard deviation among cases conducted at the same canopy density ad, but different velocity, a) Red > 100. Vertical (solid) and lateral (open) diffusivity observed in the lab (triangle) and in the field (circle) from Nepf et al. [460], Tarrel [602], and Lightbody [371]. b) Red < 100, only mechanical diffusion is present closed symbol from Nepf et al. [460], open symbol from Sena et al., [570],... Figure 6.4 Observed diffusivity in a canopy normalized by the mean velocity and stem diameter. Vertical bars indicate one standard deviation among cases conducted at the same canopy density ad, but different velocity, a) Red > 100. Vertical (solid) and lateral (open) diffusivity observed in the lab (triangle) and in the field (circle) from Nepf et al. [460], Tarrel [602], and Lightbody [371]. b) Red < 100, only mechanical diffusion is present closed symbol from Nepf et al. [460], open symbol from Sena et al., [570],...
Where D is the diffusivity observed under the same conditions in a straight cylindrical pore. [Pg.251]

Figure 33.3 Different results of motion picture with different video frame speeds for the identical trajectory of random walk. In contrast to the case of normal diffusion, observed mean square displacements (MSD) significantly depend on the frame speed in the case of anomalous diffusion. Figure 33.3 Different results of motion picture with different video frame speeds for the identical trajectory of random walk. In contrast to the case of normal diffusion, observed mean square displacements (MSD) significantly depend on the frame speed in the case of anomalous diffusion.
Experimental Example of Anomalous Diffusion Observed in a Model System for Extracellular Matrices... [Pg.374]

The fact that lower Q values were obtained for polycrystalline tungsten than for single crystals, especially for T < 0.77 , is due to a more or less significant contribution of grain boundary diffiision to the total bulk diffusion. Observed rates of volume diffusion. [Pg.32]

Fig. 6.1.9. 200 MHz spectra of H pertaining to spin diffusion experiments on a nylon 6,6 PBZT blend (VanderHart [46]). Left, magnetization gradient created by dipolar echo sequence with spacing 30 [xs, thus, initially favoring the PBZT portion of the blend. Right, results of spin diffusion observed using CRAMPS to obtain high resolution proton NMR of the blend, and observation of magnetization transfer between the phenyl protons of the PBZT, and the methylene protons of the nylon 6,6. Fig. 6.1.9. 200 MHz spectra of H pertaining to spin diffusion experiments on a nylon 6,6 PBZT blend (VanderHart [46]). Left, magnetization gradient created by dipolar echo sequence with spacing 30 [xs, thus, initially favoring the PBZT portion of the blend. Right, results of spin diffusion observed using CRAMPS to obtain high resolution proton NMR of the blend, and observation of magnetization transfer between the phenyl protons of the PBZT, and the methylene protons of the nylon 6,6.
In the case of non electrolytes, eg sucrose, the diffusion coefficient falls with increase m the concentration, so that the increase in diffusion observed by Arrhenius is connected with the presence of 10ns (cf Arrhenius, Theories of Chemistry, p 189 seq Cf. also Oholm s results quoted in Chap IX, Vol I)... [Pg.204]

Abstract Neutron scattering was first used to derive the self-diffusivities of hydrocarbons in zeolites, but transport diffusivities of deuterated molecules and of molecules which do not contain hydrogen atoms can now be measured. The technique allows one to probe diffusion over space scales ranging from a few A to hundreds of A. The mechanism of diffusion can, thus, be followed from the elementary jumps between adsorption sites to Lickian diffusion. The neutron spin-echo technique pushes down the lower limit of diffusion coefficients, traditionally accessible by neutron methods, by two orders of magnitude. The neutron scattering results indicate that the corrected diffusivity is rarely constant and that it follows neither the Darken approximation nor the lattice gas model. The clear minimum and maximum in diffusivity observed by neutron spin-echo for n-alkanes in 5A zeolite is reminiscent of the controversial window effect . [Pg.207]

Nonetheless, some clear patterns do emerge from these studies. Not only are the two processes of early wash-out and steady diffusion observed in all published studies, other features have been identified. Resin-modified glass-ionomers release more fluoride in acid media than neutral ones [49-53], and also release greater amounts in pure water than into solutions including aitificial saliva [53-55]. In these features, resin-modified glass-ionomers also resemble convenhonal glass-ionomers. [Pg.147]

Fig. 4 Diffusion fields observed at microelectrodes. (a) Linear diffusion observed at short times and (b) radial (convergent) diffusion observed at long times. Fig. 4 Diffusion fields observed at microelectrodes. (a) Linear diffusion observed at short times and (b) radial (convergent) diffusion observed at long times.
The solid line represents the correlation between the vibrational cooling rate and thermal diffusivity observed in molecular liquids, whereas the dotted portion indicates the extrapolated values. [Pg.249]

We attribute this to the existence of a non-equilibrium state of the TLS ensemble due to the fast cooling procedure The large amount of spectral diffusion observed after fast... [Pg.75]


See other pages where Observing Diffusion is mentioned: [Pg.493]    [Pg.393]    [Pg.143]    [Pg.177]    [Pg.129]    [Pg.96]    [Pg.18]    [Pg.180]    [Pg.201]    [Pg.155]    [Pg.295]    [Pg.287]    [Pg.151]    [Pg.366]    [Pg.85]    [Pg.161]    [Pg.307]    [Pg.174]    [Pg.32]   
See also in sourсe #XX -- [ Pg.57 ]




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Attempts to observe spin diffusion directly

Diffusion macroscopically observed diffusivities

Experiments for the Direct Observation of Proton Spin-Diffusion

Proton chemical shift spin-diffusion observation

Proton-spin diffusion observations

Qualitative observations of vacancy-induced surface diffusion

Single-file diffusion observation time

Spin diffusion direct observation

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