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Solvent scattering

Table 13. Refractive index and refractive index increments for light scattering solvents... Table 13. Refractive index and refractive index increments for light scattering solvents...
Filters or monochromators are generally used for the selection of either excitation and/or emission. Other, undesired sources of radiation (Raman scattering, Rayleigh scattering, solvent impurity emission) must not reach the photomultiplicator. [Pg.37]

For solution scattering, solvent densities can be calculated from standard tables of buffer densities and compositions. This procedure will allow for the non-ideality of concentrated buffer solutions that are used in some X-ray scattering studies (Table 2). Macromolecular partial specific volumes v can be experimentally determined by densitometry, usually with a Paar digital density meter, to measure the density of the buffer p uff the solutions p ,p over a concentration range ... [Pg.152]

Micellar structure has been a subject of much discussion [104]. Early proposals for spherical [159] and lamellar [160] micelles may both have merit. A schematic of a spherical micelle and a unilamellar vesicle is shown in Fig. Xni-11. In addition to the most common spherical micelles, scattering and microscopy experiments have shown the existence of rodlike [161, 162], disklike [163], threadlike [132] and even quadmple-helix [164] structures. Lattice models (see Fig. XIII-12) by Leermakers and Scheutjens have confirmed and characterized the properties of spherical and membrane like micelles [165]. Similar analyses exist for micelles formed by diblock copolymers in a selective solvent [166]. Other shapes proposed include ellipsoidal [167] and a sphere-to-cylinder transition [168]. Fluorescence depolarization and NMR studies both point to a rather fluid micellar core consistent with the disorder implied by Fig. Xm-12. [Pg.481]

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]

If the scattering particles are in a dielectric solvent medium with solvent refractive index Uq, we can define the excess... [Pg.1389]

Two of the most important functions in the application of neutron scattering are the use of deuterium labelling for the study of molecular confomiation in the bulk state and the use of deuterium solvent in polymer solutions. In the following, we will consider several different applications of die general fomuda to deuteration. [Pg.1412]

Let us take two polymers (one deuterated and one hydrogenated) and dissolve them in a solvent (or another polymer) having a scattering length b. The coherent scattered intensity can be derived from (B 1.9.117), which gives... [Pg.1413]

Fox and Floryf used experimental molecular weights, intrinsic viscosities, and rms end-to-end distances from light scattering to evaluate the constant in Eq. (9.55). For polystyrene in the solvents and at the temperatures noted, the following results were assembled ... [Pg.653]

Next let us consider the light scattered by liquids of low molecular weight compounds. We are actually not directly interested in this quantity per se, but in scattering by solutions-polymer solutions eventually, but for now solutions of small solute molecules. The solvent in such a solution does scatter, but, in practice, the intensity of light scattered by pure solvent is measured and subtracted as a blank correction from the scattering by the solution. [Pg.678]

The molecular weight and its distribution have been determined by laser light scattering, employing a new apparatus for ETFE dissolution and solution clarification at high temperature diisobutyl adipate is the solvent at 240°C. The molecular weight of molten ETEE is determined by high temperature rheometry (21). [Pg.366]


See other pages where Solvent scattering is mentioned: [Pg.21]    [Pg.197]    [Pg.83]    [Pg.164]    [Pg.150]    [Pg.1407]    [Pg.1408]    [Pg.209]    [Pg.241]    [Pg.21]    [Pg.197]    [Pg.83]    [Pg.164]    [Pg.150]    [Pg.1407]    [Pg.1408]    [Pg.209]    [Pg.241]    [Pg.403]    [Pg.1121]    [Pg.1179]    [Pg.1414]    [Pg.1415]    [Pg.1416]    [Pg.2419]    [Pg.2489]    [Pg.2519]    [Pg.2589]    [Pg.2962]    [Pg.164]    [Pg.276]    [Pg.328]    [Pg.350]    [Pg.259]    [Pg.360]    [Pg.360]    [Pg.411]    [Pg.431]    [Pg.32]    [Pg.378]    [Pg.3]    [Pg.60]    [Pg.237]    [Pg.433]    [Pg.497]    [Pg.343]    [Pg.343]    [Pg.354]    [Pg.534]   
See also in sourсe #XX -- [ Pg.239 ]




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