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Temperature shift characteristics, time

Time-Temperature Shift Characteristics. Temperature is a major environmental influence on viscoelastic pavement response. The VESYS IIM program can handle material properties as a function of temperature variations. The computer input command BETA relates the time-temperature shift factor, au to the temperature variable for the pavement materials. This relationship is given by ... [Pg.208]

Fig. 4.9 Temperature dependence of the characteristic time of the a-relaxation in PIB as measured by dielectric spectroscopy (defined as (2nf ) ) (empty diamond) and of the shift factor obtained from the NSE spectra at Qmax=l-0 (filled square). The different lines show the temperature laws proposed by Tormala [135] from spectroscopic data (dashed-dotted), by Ferry [34] from compliance data (solid) and by Dejean de la Batie et al. from NMR data (dotted) [136]. (Reprinted with permission from [125]. Copyright 1998 American Chemical Society)... Fig. 4.9 Temperature dependence of the characteristic time of the a-relaxation in PIB as measured by dielectric spectroscopy (defined as (2nf ) ) (empty diamond) and of the shift factor obtained from the NSE spectra at Qmax=l-0 (filled square). The different lines show the temperature laws proposed by Tormala [135] from spectroscopic data (dashed-dotted), by Ferry [34] from compliance data (solid) and by Dejean de la Batie et al. from NMR data (dotted) [136]. (Reprinted with permission from [125]. Copyright 1998 American Chemical Society)...
Fig. 4.14 Results on fully protonated PIB by means of NSE [147]. a Time evolution of the self-correlation function at the Q-values indicated and 390 K. Lines are the resulting KWW fit curves (Eq. 4.9). b Momentum transfer dependence of the characteristic time of the KWW functions describing Sseif(Q,t) at 335 K (circles), 365 K (squares) and 390 K (triangles). In the scaling representation (lower part) the 335 K and 390 K data have been shifted to the reference temperature 365 K applying a shift factor corresponding to an activation energy of 0.43 eV. Solid (dotted) lines through the points represent (q-2 power laws. Full... Fig. 4.14 Results on fully protonated PIB by means of NSE [147]. a Time evolution of the self-correlation function at the Q-values indicated and 390 K. Lines are the resulting KWW fit curves (Eq. 4.9). b Momentum transfer dependence of the characteristic time of the KWW functions describing Sseif(Q,t) at 335 K (circles), 365 K (squares) and 390 K (triangles). In the scaling representation (lower part) the 335 K and 390 K data have been shifted to the reference temperature 365 K applying a shift factor corresponding to an activation energy of 0.43 eV. Solid (dotted) lines through the points represent (q-2 power laws. Full...
Fig. 5.16 Q-dependence of the characteristic times of the KWW functions describing the PIB dynamic structure factor at 335 K filled circle), 365 K empty square) and 390 K filled triangle), a Shows the values obtained for each temperature. Taking 365 K as reference temperature, the application of the rheological shift factor to the times gives b and a shift factor corresponding to an activation energy of 0.43 eV delivers c. The arrows in a show the interpolated mechanical susceptibility relaxation times at the temperatures indicated. (Reprinted with permission from [147]. Copyright 2002 The American Physical Society)... Fig. 5.16 Q-dependence of the characteristic times of the KWW functions describing the PIB dynamic structure factor at 335 K filled circle), 365 K empty square) and 390 K filled triangle), a Shows the values obtained for each temperature. Taking 365 K as reference temperature, the application of the rheological shift factor to the times gives b and a shift factor corresponding to an activation energy of 0.43 eV delivers c. The arrows in a show the interpolated mechanical susceptibility relaxation times at the temperatures indicated. (Reprinted with permission from [147]. Copyright 2002 The American Physical Society)...
An additional piece of information can be obtained by studying a synthetic compound derived from the GFP chromophore (1-28) fluorescing at room temperature. In Fig. 3a we show the chemical structure of the compound that we studied in dioxan solution by pump-probe spectroscopy. If we look at the differential transmission spectra displayed in Fig. 3b, we observed two important features a stimulated emission centered at 508 nm and a huge and broad induced absorption band (580-700 nm). Both contributions appear within our temporal resolution and display a linear behavior as a function of the pump intensity in the low fluences limit (<1 mJ/cm2). We note that the stimulated emission red shifts with two characteristic time-scales (500 fs and 10 ps) as expected in the case of solvation dynamics. We conclude that in the absence of ESPT this chromophore has the same qualitative dynamical behavior that we attribute to the relaxed anionic form. [Pg.440]

Temperatures of vitrification, Tv, and melting, Tm, for some compounds the diffusion coefficients D and the characteristic times rD at 77 K of the shift at distances of the order of the atomic size for particles with radius Ru - 3 A... [Pg.139]

The second in situ technique is NMR. An autoclave fitting with the NMR cavity was designed by Gerardin et al. [59] and allows to follow the evolution of many parameters of the synthesis via the NMR characteristics of the different nuclei versus temperature and reaction time. The first measurement that can be reached now is the absolute value of the pH in hydrothermal conditions and the quantitative evolution of the concentration of protons in the bomb with the parameters of the synthesis [60], They proved that 14N NMR chemical shifts of well chosen amine compounds (imidazole and DABCO which possess complementary pKas) are precise pH indicators in aqueous solutions from room temperature to 475 K. Use of both amines permit to cover a wide range of about 9 pH units, with a precision of 0.1 pH unit. [Pg.223]

Another very significant characteristic of multiple mechanism relaxation is the pronounced change of the shape of the spectrum of relaxation times with temperature with increasing temperature the relaxation spectrum not only shifts to shorter time values, but a dip appears and deepens indicating increased separation with temperature of those parts of the spectrum due to the different mechanisms. (This is shown in Fig. 21.) The high temperature or long-time part of the spectrum consists,... [Pg.98]

T represents the desired function, providing the information about the stability constant Ks. AH is the enthalpy of reaction, R the gas constant and T the (absolute) temperature. The chemical shift expressed by ccomplex has to be recorded instantaneously as a relaxation signal, since only then does it reflect exclusively the chemical response (proceeding with its characteristic time constant), and can clearly be separated from other - physical — changes, brought about by the rapid temperature alternation. In Figs. 6 and 7 the quantity T, to be determined by such experiments is plotted as a function of the total standard concentration (at fixed sample concentration). These relaxational titration plots are to be seen in comparison with the well-known classical titration curves and with the derivatives (Figs. 8 and 9), which contain more detailed information about complex stabilities. [Pg.104]

Figures 2.27(b) shows the spectral dependence of the long-time photoluminescence integrated over 30-90 ns after excitation as a function of temperature. At these times the initial exciton population has completely decayed and all the remaining emission originates from the long-lived exciplex states. At low temperatures, we see the red-shifted emission characteristic of the exciplex. For higher temperatures, however, the emission spectrum increasingly acquires excitonic... Figures 2.27(b) shows the spectral dependence of the long-time photoluminescence integrated over 30-90 ns after excitation as a function of temperature. At these times the initial exciton population has completely decayed and all the remaining emission originates from the long-lived exciplex states. At low temperatures, we see the red-shifted emission characteristic of the exciplex. For higher temperatures, however, the emission spectrum increasingly acquires excitonic...
Fig. 6. Comparison of the frequency dependence of the total longitudinal proton relaxation time Ti and the dipolar proton relaxation time Tjo in the selectively methyl-deuterated high-temperature nematic liquid crystal PAA-d (upper diagram). The characteristic features are qualitatively similar to the results of Fig. S. However, because of the higher temperature both relaxation times are longer and the local field is smaller therefore the limit Bq < Bix is shifted to lower v values and the regime with T IT DS i is not fully seen (lower diagram) for experimental reasons. Fig. 6. Comparison of the frequency dependence of the total longitudinal proton relaxation time Ti and the dipolar proton relaxation time Tjo in the selectively methyl-deuterated high-temperature nematic liquid crystal PAA-d (upper diagram). The characteristic features are qualitatively similar to the results of Fig. S. However, because of the higher temperature both relaxation times are longer and the local field is smaller therefore the limit Bq < Bix is shifted to lower v values and the regime with T IT DS i is not fully seen (lower diagram) for experimental reasons.
The fourth step is to plot the shift factors Aj against temperature (Figure 2.15c). This representation of the time-temperature superposition characteristic of viscoelastic materials has been extensively analysed with the well-known Williams-Landel-Ferry (WLF) relationship, at temperatures above T ... [Pg.33]

The specific productivity of chemical processes can be increased considerably by working under unconventional reaction conditions in the so-called novel process windows [5]. Novel process windows allow highly intensified processing at high temperatures and high concentrations, preferably solvent free. As the intrinsic reaction rate increases exponentially with the temperature, the characteristic reaction times are shifted to very low values. Typical characteristic reaction times, as defined in Eq. (11.1), are indicated in Figure 11.1 together with characteristic times... [Pg.333]


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Characteristic temperature

Shifted temperature

Shifting time

Time characteristic times

Time-temperature

Time-temperature shift

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