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Energy - temperature curves

Figure 5.2 The modification of the electron energy distribution curve by the presence of diffraction limits in a crystal. The lower filled band is separated from upper unoccupied states in a semiconductor by a small energy difference, so that some electrons can be promoted to conduction by an increase in temperature... Figure 5.2 The modification of the electron energy distribution curve by the presence of diffraction limits in a crystal. The lower filled band is separated from upper unoccupied states in a semiconductor by a small energy difference, so that some electrons can be promoted to conduction by an increase in temperature...
Fig. 9. Stored energy release curves for CSF graphite irradiated at 30°C in the Hanford K reactor cooled test hole [64], Note, the rate (with temperature) of stored energy release (J/Kg-K) exceeds the specific heat and thus under adiabatic conditions self sustained heating will occur. Fig. 9. Stored energy release curves for CSF graphite irradiated at 30°C in the Hanford K reactor cooled test hole [64], Note, the rate (with temperature) of stored energy release (J/Kg-K) exceeds the specific heat and thus under adiabatic conditions self sustained heating will occur.
Consider a distribution system that consists of a gaseous mobile phase and a liquid stationary phase. As the temperature is raised the energy distribution curve in the gas moves to embrace a higher range of energies. Thus, if the column temperature is increased, an increasing number of the solute molecules in the stationary phase will randomly acquire sufficient energy (Ea) to leave the stationary phase and enter the... [Pg.12]

In a series of reactions for which an acceUrative decrease in the activation energy is accompanied by a decelerative decrease in the entropy of activation (Compensation Law ), or the two increase together, there wiU be an isokinetic temperature (between 0-200° C for three-fourths of the 79 reactions tabulated by Leffler ). The rate vs. temperature curves for all the reactions in the series pass through this single point. Comparisons are affected since the isokinetic temperature is a point of inversion of relative reactivity in the series. [Pg.267]

Figure 9-17. Photoinduced absorption in s-LPPP al 0.26 eV versus temperature (filled squares). Full lines represent the model results (lower curve for two activation energies, higher curve for one). The doited lines represent the decay rates for the 0.12eV (a) and 0.37 eV (b) activated processes the dash-dolled horizontal line represents the temperature-independent part E. Figure 9-17. Photoinduced absorption in s-LPPP al 0.26 eV versus temperature (filled squares). Full lines represent the model results (lower curve for two activation energies, higher curve for one). The doited lines represent the decay rates for the 0.12eV (a) and 0.37 eV (b) activated processes the dash-dolled horizontal line represents the temperature-independent part E.
Experiments measuring the energy density at a high rate of extension over a range of temperatures showed that the abrasion-temperature function for tread compounds had a similar shape as the inverse of the energy density at break temperature curve. This is also shown in Figure 26.51... [Pg.727]

However, the characteristics of point b with regard to temperature fluctuations are quite different. At this point the slope of the energy release curve is greater than the slope of the energy loss curve. If a small positive temperature fluctuation were to occur, one would be in a... [Pg.372]

If the temperature intercept of the energy loss curve lies between those corresponding to the... [Pg.374]

With this information it is now possible to derive values of h and ki from the appropriate slope and intercept in Fig. 13 with the aid of Eq. (43). All these constants are listed in Table XXIII, together with the other constants derived above. In Table XXIII data are also given for the polymerization process at 40°C but is probably less accurate since fewer measurements of Pn and Q were obtained at this temperature. The values for the energy of activation obtained for the termination constants therefore can only be considered approximate. It is evident from these, however, that because kt increases more rapidly with temperature than kiKi or kiK2 that both D ] and Pn will decrease with increasing temperature. This is not clear from the experimental data because the temperature difference is too small although the trend is discernible. It also follows from Eq. (40) that since R is the product of two terms, fc2 which increases with temperature and 5° [E ] which decreases with increasing temperature, the rate versus temperature curve will have a maximum. [Pg.321]

Figure 1. Activation energy of electron-transfer process as a function of electronic energy gap of a reaction. Er = Eg + Ec is the total reorganization energy where Es is the classical solvent reorganization energy and Ec is the reorganization energy of an intramolecular mode, l Figure 1. Activation energy of electron-transfer process as a function of electronic energy gap of a reaction. Er = Eg + Ec is the total reorganization energy where Es is the classical solvent reorganization energy and Ec is the reorganization energy of an intramolecular mode, l<oc = 2kBT, at room temperature. Curve 1 (Ec = 0) represents a classical case curve 3 (Ea = 0) represents quantum effects at room temperature and curve 2 (Eg = Ec = EJ2) represents the interference of the...
Mossbauer spectra were then taken of the small iron particles after various pretreatments, with the catalyst under reaction conditions (765). For increased sensitivity the velocity-offset mode was used (Section II, B, 1), and the magnetically split spectral area versus temperature curves after the various pretreatments are shown in Fig. 30. It is therein seen that the ammonia treatment, which increases the catalytic activity, decreases the magnetically split spectral area at a given temperature this is the result of a decrease in the magnetosurface anisotropy energy barrier. While the effects of these pretreatments are in themselves interesting, the important point for surface... [Pg.205]

White (1955) believes that differential thermal analysis curves obtained by him on heating drawn fibers of 6, 6-6 and 6-10 nylons as well as polyethylene terephthalate, indicate that at first crystallites disorient and then melt. He found two peaks in what would correspond to a specific heat-temperature curve. However, it is difficult to understand why the disorientation of oriented crystals would involve the absorption of energy. [Pg.243]


See other pages where Energy - temperature curves is mentioned: [Pg.81]    [Pg.81]    [Pg.108]    [Pg.306]    [Pg.512]    [Pg.199]    [Pg.507]    [Pg.873]    [Pg.132]    [Pg.383]    [Pg.227]    [Pg.61]    [Pg.18]    [Pg.90]    [Pg.372]    [Pg.373]    [Pg.373]    [Pg.291]    [Pg.123]    [Pg.89]    [Pg.164]    [Pg.223]    [Pg.228]    [Pg.49]    [Pg.532]    [Pg.277]    [Pg.199]    [Pg.391]    [Pg.22]    [Pg.243]    [Pg.306]    [Pg.512]    [Pg.115]    [Pg.12]    [Pg.65]    [Pg.25]   
See also in sourсe #XX -- [ Pg.21 , Pg.30 ]




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Energy temperatures

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