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Relaxation activation energies and

Okazaki I, Wunderlich B (1996) Modulated Differential Scanning Calorimetry in the Glass Transition Region, V. Activation Energies and Relaxation Times of Poly(ethylaie terephthalate)s. J Polymer Sci Part B Polymer Phys 34 2941-2952. [Pg.704]

The aim of this work is to analyze the changes in the relevant thermal behavior of the crosslinked EVA encapsulant material due to outdoor exposure in Mediterranean climate by TSC and DSC thermal analysis. The changes in thermal properties should be discussed and special interest will be focused on the specific TSC relaxation parameters like activation energy and relaxation frequency determination by using the initial rise method. [Pg.194]

Details of relaxation processes such as activation energies and relaxation spectra are obtainable from DMTA. The inset in Figure 7.16 shows an Arrhenius plot for the epoxy composite. The Arrhenius relation ... [Pg.202]

In Equation 1, t is a thermal vibration frequency, U and P are, respectively activation energy and volume whereas c is a local stress. The physical significance and values for these parameters are discussed in Reference 1. Processes (a)-(c) are performed with the help of a Monte-Carlo procedure which, at regular short time intervals, also relaxes the entanglement network to its minimum energy configuration (for more details, see Reference 1). [Pg.117]

In general, intramolecular isomerization in coordinatively unsaturated species would be expected to occur much faster than bimolecular processes. Some isomerizations, like those occurring with W(CO)4CS (47) are anticipated to be very fast, because they are associated with electronic relaxation. Assuming reasonable values for activation energies and A-factors, one predicts that, in solution, many isomerizations will have half-lives at room temperature in the range 10 7 to 10 6 seconds. The principal means of identifying transients in uv-visible flash photolysis is decay kinetics and their variation with reaction conditions. Such identification will be difficult if not impossible with unimolecular isomerization, particularly since uv-visible absorptions are not very sensitive to structural changes (see Section I,B). These restrictions do not apply to time-resolved IR measurements, which should have wide applications in this area. [Pg.285]

Work in groups of three. The shift factor, or, in the WLF Equation [Eq. (5.76)], is actually a ratio of stress relaxation times, f , in the polymer at an elevated temperature, T, relative to some reference temperature. To, and can be related via an Arrhenius-type expression to the activation energy for relaxation, Erei as... [Pg.458]

The position of absorption B on the temperature scale depends on the nature and on the number of exchangeable cations. We conclude that absorption B is a cationic relaxation process. The activation energy of absorption B for NaF86.5 agrees with that reported by Matron (10) for their -relaxation process. It is in line with the increase of activation energy for relaxation after adsorption of water on dehydrated Na+-zeolites. Thus, absorption B is caused by the local migration of site III cations over two neighboring sites III, as observed on dehydrated X-type zeolites (8) and on partially hydrated NaX (10). [Pg.111]

Table 6 Activation energies and entropies determined for y and /S relaxations of different copolyamides (from [57])... Table 6 Activation energies and entropies determined for y and /S relaxations of different copolyamides (from [57])...
It is evident that the dipolar interaction increases the activation energy and slows the relaxation time of moment reversal. To explain the dependence quantitatively a simple model was proposed [26], inspired by the references contained in [22], where the relaxation time considered is for independent clusters and the dipolar interaction modifies Ueff. In the model, a test cluster of uniaxial anisotropy is surrounded by clusters with their anisotropy axis randomly oriented. The susceptibility is dominated by the largest particles in a sample since it is proportional... [Pg.19]

Figure 55. Ajump within the true potential (lattice potential (top) plus defect potential (center)) requires the surmounting of a relatively high activation energy and a subsequent relaxation of the environment, before the site B takes on the original potential surroundings of A (see text). From Ref.217. (Reprinted from K. Funke, Ion transport in fast ion conductors—spectra and models , Solid State Ionics. 94, 27-33. Copyright 1997 with permission from Elsevier.)... Figure 55. Ajump within the true potential (lattice potential (top) plus defect potential (center)) requires the surmounting of a relatively high activation energy and a subsequent relaxation of the environment, before the site B takes on the original potential surroundings of A (see text). From Ref.217. (Reprinted from K. Funke, Ion transport in fast ion conductors—spectra and models , Solid State Ionics. 94, 27-33. Copyright 1997 with permission from Elsevier.)...
Detailed examination of the relaxations requires isothermal scans of relative permittivity and dielectric loss factor as a function of frequency/ so that effective dipole movements and activation energies of relaxation times may be obtained. A typical pair of plots of d and e" values against log/is shown in Fig. 3.7. Graphs of dielectric data of this kind are sometimes called, rather... [Pg.72]


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