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Chain structure concentration

For the second method the threshold concentration of the filler in a composite material amounts to about 5 volume %, i.e. below the percolation threshold for statistical mixtures. It is bound up with the fact that carbon black particles are capable (in terms of energy) of being used to form conducting chain structures, because of the availability of functional groups on their surfaces. This relatively sparing method of composite material manufacture like film moulding by solvent evaporation facilitates the forming of chain structures. [Pg.132]

Besides synthesis, current basic research on conducting polymers is concentrated on structural analysis. Structural parameters — e.g. regularity and homogeneity of chain structures, but also chain length — play an important role in our understanding of the properties of such materials. Research on electropolymerized polymers has concentrated on polypyrrole and polythiophene in particular and, more recently, on polyaniline as well, while of the chemically produced materials polyacetylene stih attracts greatest interest. Spectroscopic methods have proved particularly suitable for characterizing structural properties These comprise surface techniques such as XPS, AES or ATR, on the one hand, and the usual methods of structural analysis, such as NMR, ESR and X-ray diffraction techniques, on the other hand. [Pg.16]

The properties of a polymer network depend not only on the molar masses, functionalities, chain structures, and proportions of reactants used to prepare the network but also on the conditions (concentration and temperature) of preparation. In the Gaussian sense, the perfect network can never be obtained in practice, but, through random or condensation polymerisations(T) of polyfunctional monomers and prepolymers, networks with imperfections which are to some extent quantifiable can be prepared, and the importance of such imperfections on network properties can be ascertained. In this context, the use of well-characterised random polymerisations for network preparation may be contrasted with the more traditional method of cross-linking polymer chains. With the latter, uncertainties can exist with regard to the... [Pg.377]

In general, the factor by which G is reduced depends on Me, f, chain stiffness, and the initial concentrations of reactive groups obtainable in bulk, in a manner which still needs to be resolved in detail. However, for bulk reaction mixtures, the moduli of networks with relatively flexible chain structures can be reduced by a factor of five below those expected for network formation in the absence of pre-gel intramolecular reaction. [Pg.395]

The D. pulchra furanone compounds generally consist of a furan ring structure with a substituted alkyl chain at the C-3 position and a bromine substitution at the C-4 position (Fig. 5). The substituent at the C-5 position may vary in terms of side chain structure. The natural furanones are halogenated at various positions by bromine, iodine, or chlorine [128]. D. pulchra produces at least 30 different halogenated furanones which are stored in specialized vesicles and are released at the surface of the thallus at concentrations ranging from 1 to 100 ng/cm2 [132]. Field experiments have demonstrated that the surface concentration of furanones is inversely correlated with the degree of colonization by marine bacteria [133]. [Pg.320]

Recently many subtle effects of the ligand structure, concentrations of alkene, and conditions on the polymerisation have been reported to have significant effects on molecular weight, regioselectivity, branching, stereoselectivity or enantioselectivity, incorporation of other monomers, chain transfer, etc. Often these subtle effects can be understood from the mechanism, or they contribute to the understanding of the detailed processes going on. [Pg.214]

To a first approximation, which neglects changes in average chain structure, the loss in elastically active junction point concentration may be translated directly into loss in concentration of elastically active chains and increase in the value of M, . For a perfect network in the dry state, the concentration of elastically active chains is given by the equations... [Pg.32]

Figure 5. Effect of organolithium concentration on polyisoprene chain structure undiluted ( ) 0.5M in n-hexane (A) 0.5M in benzene (O ... Figure 5. Effect of organolithium concentration on polyisoprene chain structure undiluted ( ) 0.5M in n-hexane (A) 0.5M in benzene (O ...
The Eyring analysis does not explicity take chain structures into account, so its molecular picture is not obviously applicable to polymer systems. It also does not appear to predict normal stress differences in shear flow. Consequently, the mechanism of shear-rate dependence and the physical interpretation of the characteristic time t0 are unclear, as are their relationships to molecular structure and to cooperative configurational relaxation as reflected by the linear viscoelastic behavior. At the present time it is uncertain whether the agreement with experiment is simply fortuitous, or whether it signifies some kind of underlying unity in the shear rate dependence of concentrated systems of identical particles, regardless of their structure and the mechanism of interaction. [Pg.144]

Here D is the translational diffusion coefficient of the solute molecule at C —> 0 with C the mass concentration of the solute, kd the diffusion second virial coefficient, f a dimensionless parameter depending on polymer chain structure and solvent, and the mean square radius of gyration of the polymer chain. Hence, for C and q small enough, Eq. (2.3) may be approximated by... [Pg.110]

The luminescent binuclear gold dithiophosphate complexes [Au2 S2P-(OR)2h] (R = Me, Et) were found to possess comparable intra- and intermolecular aurophilic contacts and afforded one-dimensional Au - Au chain structures [60]. At 77 K, solid samples of [Au2 S2P(OMe)2 2] displayed multiple emission bands, with the two concentration-dependent higher energy bands at 415 nm (r = 20 ns) and 456 nm (r = 2.16 is) assigned to XMC and 3MC emission, respectively, while the lower energy band at 560 nm was attributed to a LMCT excited state. [Au2 S2P(OR)2 2] was further shown to exhibit intense luminescence of different colors and striking thermochromism of the emission in frozen glasses of different solvents. [Pg.283]

The single-chain structure factors calculated in the previous sections correspond to the infinite dilution limit. This limit also corresponds to zero scattering intensity and is not useful so that concentration effects have to be included in the modeling of polymer solutions. First, Zimm s single-contact approximation [5] is reviewed for dilute polymer solutions then, a slight extension of that formula which applies to semidilute solutions, is discussed. [Pg.103]

Effects due to macromolecular shape changes during single-contact interactions can, within the Benoit-Benmouna theory, be included in an ad-hoc fashion by renormalizing the single-chain structure factor to make it concentration dependent. This approach is often used to describe polymer solutions up to the concentrated region. [Pg.107]

It should be taken into account that only part of the particles collect into chain structure and others remain separated. Both types of particles are in thermal equilibrium. Using EMR spectra it is possible to calculate the fraction of particles, which belong to aggregate by spectra separation procedure. The fraction of magnetite involved in aggregates increases with concentration (Figure2). [Pg.51]

Percolation theory is helpful for analyzing disorder-induced M-NM transitions (recall the classical percolation model that was used to describe grain-boundary transport phenomena in Chapter 2). In this model, the M-NM transition corresponds to the percolation threshold. Perhaps the most important result comes from the very influential work by Abrahams (Abrahams et al., 1979), based on scaling arguments from quantum percolation theory. This is the prediction that no percolation occurs in a one-dimensional or two-dimensional system with nonzero disorder concentration at 0 K in the absence of a magnetic field. It has been confirmed in a mathematically rigorous way that all states will be localized in the case of disordered one-dimensional transport systems (i.e. chain structures). [Pg.298]


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See also in sourсe #XX -- [ Pg.287 ]




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