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Network relaxation

Finally, interactions between neighbouring molecules and viscosity will alter the resolution in the spectrum via the spin/network relaxation time. [Pg.141]

In the benzene-methanol case, the first inertial component exhibits similar dependence on xp as in acetonitrile mixtures (see Fig. 2.b). The same is still true at intermediate times around 1-2 ps and a similar picture as in Fig. 3.a. can be observed at x/ >=0.2.. However, the addition of methanol to benzene gives rise to a very long decay time (see Fig. 2.b), which may be associated with the slow hydrogen bond network relaxation of methanol. It should be noted that no significant change of the hydrogen bond from methanol to the coumarin carbonyl group is observed between the S0 and S states. [Pg.248]

Alternatively, defects containing an oxygen vacancy (OV) can significantly deform the network, mainly due to mechanical distortions of the defect and its surrounding fragment. In order to simulate both network relaxation caused by the defect and its incorporation into the bulk in such systems, one needs to use larger model clusters that include at least one additional layer of bonds surrounding the defect. The atomic coordinates inside the model... [Pg.73]

It Is of Interest to note that subsequent cycling of the epoxy sample In Figure 6 results In a gradual Increase of the "stable" dry and wet state tan 6 values. This cumulative Increase In network mobility continues with moisture cycling because the sample Is never allowed a macroscopic network relaxation. Recovery of original dry state properties at least requires thermal excitation of the system to temperatures near the glass transition point (3). [Pg.106]

The results clearly sho that the network relaxation time can be varied continuously from 10 s to many seconds. This.means that it is possible that the frequency range in which detergent solutions show elastic properties can be shifted to a desired range. [Pg.65]

Early experiments with elastomers showed that the relaxation toward equilibrium was sharply dependent on crosslink density. It was found that tightly crosslinked networks relaxed very quickly, whereas networks with low crosslink density exhibited relaxation that covered an extremely broad time scale. These early experiments were correlated in terms of the expression for the tensile relaxation modulus E(t) ... [Pg.155]

Generally, a decrease in the thermodynamic affinity of the solvent (X-induced syneresis) during cooling would have to result in decreasing copolymer swelling. However, if much solvent has to be removed from the beads, it first separates as droplets inside the gel, because the network relaxation is fairly slow [266]. Excess solvent is then slowly pushed out of the beads having a rather flexible gel-type matrix that is homogeneous under equilibrium conditions. Consequently, the microsyneresis is a nonequilibrium state of the particular gel-type polymer-solvent system. [Pg.98]

During the preparation of macroporous materials by crosslinking copolymerization in the presence of precipitants, phase separation takes place within a relatively short period of time. This fast phase separation naturally results in the formation of microdroplets of the rejected porogen. Since the conversion of comonomers at that moment is very low, the rapidly growing polymeric network fixes in the gel the emerging liquid droplets. The nonequilibrium microsyneresis thus transforms into the stable form of phase separation within a heterogeneous system. Thus, the fast arrival at the unstable local polymer-solvent relationship, as compared with the slow rates of solvent macrosyneresis and of network relaxation, leads to the formation of gel-included microdroplets and, finally, to a permanent macroporous structure of copolymers. [Pg.98]

Methanol happens to be the 0-solvent for the examined hypercrosslinked sample, where its network relaxes completely. Solvents to the right from methanol cause additional swelling and stretching of the network. When filled with water and, especially, air, the network contracts significantly and acquires strong inner stresses. [Pg.237]

Fully silylated silica exhibits hydrophobic interactions between the PDMS-covered surface and the solvent as well as entanglement of the PDMS layers. Addition of UP or VE resins increases the polarity of the medium. As a result, the mismatch between the matrix and the PDMS layer is increased, which favors PDMS-PDMS interactions and therefore enhances the network stability and decreases the network relaxation time. [Pg.765]

Oscillatory shear rheology of EPDM plasticized with resol was used to determine an equilibrium shear modulus Ge), relaxation in compression and strain recovery. Ge was analysed with consideration of crosslink density and permanent entanglements, including evaluation of plasticizer and soluble polymer fraction. Relaxation data were modelled with the empirical Chasset-Thirion equation and it was proposed that longer relaxation times were associated with chains pendant from the network. Relaxation times increased with crosslink density. When the crosslink density was low and pendant chains were longer and more numerous, relaxation times were increased and elastic recovery diminished. ... [Pg.608]

Fig. 2. Stages of relaxation in diluted polymer gel a) Undeformed gel b) short times gel (black) and sol (green) polymers are stretched and aligned c) intermediate times sol polymers (in green) relax but gel network (black) is still deformed d) long times polymer in gel network relaxes but retains an equilibrium deformation. Fig. 2. Stages of relaxation in diluted polymer gel a) Undeformed gel b) short times gel (black) and sol (green) polymers are stretched and aligned c) intermediate times sol polymers (in green) relax but gel network (black) is still deformed d) long times polymer in gel network relaxes but retains an equilibrium deformation.
However, other rheological studies reported the existence of two relaxation processes. Reference 112 presented an interpretation of the results that is very different from that in References 105-108. The slow process, which is that discussed in References 105-108, is now attributed to the network relaxation while the faster of the two processes, not seen in these references, is attributed to the exit of a hydrophobe from a junction. One of the difficrdties with this interpretation is that the lifetime of a hydrophobe in a junction would increase with temperature. The authors state that nonionic surfactants show such a behavior. Unfortunately, the references cited to back this point do not really refer to dynamic studies of micelles of nonionic surfactants. Such studies have been performed and show that the residence time/lifetime of nonionic surfactants in micelles decreases as the temperature is increased,just as for ionic surfactants. Thus at the present time there appears to be no good evidence for the assignment of the fast relaxation observed in Reference 112 to the exit of a hydrophobe from a junction. In contrast, the available experimental results seem to indicate that it is the slow relaxation that is associated with this process. [Pg.218]


See other pages where Network relaxation is mentioned: [Pg.480]    [Pg.377]    [Pg.151]    [Pg.63]    [Pg.201]    [Pg.27]    [Pg.108]    [Pg.505]    [Pg.153]    [Pg.63]    [Pg.105]    [Pg.566]    [Pg.101]    [Pg.82]    [Pg.60]    [Pg.376]    [Pg.387]    [Pg.8]    [Pg.3]    [Pg.110]    [Pg.378]    [Pg.146]    [Pg.257]    [Pg.139]    [Pg.608]    [Pg.377]    [Pg.285]    [Pg.4764]    [Pg.299]    [Pg.205]    [Pg.209]    [Pg.270]    [Pg.374]    [Pg.265]    [Pg.733]    [Pg.26]   
See also in sourсe #XX -- [ Pg.92 , Pg.154 ]




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