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Temperature values display

For both cluster ions, the ZTRID rates for Equations (24) and (25) at room temperature (Table 6) were analyzed by the master equation method, the ab initio calculated IR intensities being used, to give the fitted values of Eq displayed in the Table. In addition, the temperature dependence of Equation (25) was fitted to the master equation simulation (the E approach), to give an independent value of Ef (0.31 eV) in excellent agreement with the value from the approach (0.32 eV). These values were corrected to 298 K by use of Equations (3) and (4) to give the BDE values displayed as AH (ZTRID). [Pg.111]

The temperature dependence of the ratio ( 1/2)0/( 1/2) where ( 1/2)0 refers to the room temperature value, measured for the CHOH - CH2 - O and CH2 -N carbons in HMDA, HMDA/AP10 and HMDA/AP19 systems, is displayed in Fig. 102a and b, respectively. Over the temperature range investi-... [Pg.149]

In Fig. 7 the dependence x(T) is shown for 16 different liquids with extremely different yo values. At room temperature they display i values which cover five decades. [Pg.49]

Auxiliary power +12—r30V DC Power consumption max. 700 mW Measured value display LCD Ambient temperature range -10°C—r55°C ... [Pg.348]

The chemical compositions of both the target and deposited films were analyzed by x-ray photoelectron spectroscopy (XPS) and Fourier-transform infrared (FTIR) spectroscopy. The typical XPS Cl s level spectra for the films deposited at different target temperatures are displayed in Fig. 26, and compared with that of the target (bottom trace) [58]. Besides the CF2 peak centered at 292 eV, a small shoulder due to CF3 was detected at 295 eV for the SR-deposited films (top and middle traces) but not for the target (bottom trace). Correspondingly, the ratio of F to C values (measuring errors... [Pg.314]

Fig. 30. In (a) the 10-kHz capacitance versus temperature is displayed for the 2 densities of states shown in Fig. 20 as well as a constant g(E) = lO cm eV [as indicated by the dashed and dotted (as in Fig. 20) and dash-dotted lines, respectively] at which now the bulk Fermi level E% is assumed to lie 0.6 eV below E. In (b) the ratio C [dCldT] is plotted versus temperature. As explained in the text, the slope and curvature of these curves are directly related to the value and slope, respectively, oig(E) at FJ. Fig. 30. In (a) the 10-kHz capacitance versus temperature is displayed for the 2 densities of states shown in Fig. 20 as well as a constant g(E) = lO cm eV [as indicated by the dashed and dotted (as in Fig. 20) and dash-dotted lines, respectively] at which now the bulk Fermi level E% is assumed to lie 0.6 eV below E. In (b) the ratio C [dCldT] is plotted versus temperature. As explained in the text, the slope and curvature of these curves are directly related to the value and slope, respectively, oig(E) at FJ.
In the top segment of Table 11.2 we display data for peaks 2, 3, and IS 6 from the standard curve mns, and for three unknown peaks (A, B, C) in a separate chromatographic run eluting with similar RT, plus D, which is the IS 6 peak in that mn. In both runs we use IS 6 as a retention internal standard to calculate RRT values displayed in the third column of the table. If we only compared RTs (i.e., t ), we might say A is 2 and B is 3. We note, however, that IS D elutes 0.2 min later than it did in the standard mns. Something has caused a shift in retention between the mns, perhaps the flow has slowed a little, or the GC oven temperature dropped a bit. If we compare RRTs we see that B and C are better matches to 2 and 3, respectively. [Pg.745]

Fig. 18 A series of growth morphologies for different temperatures is displayed. The en-tropic barrier is set to ps = 0.6, a value which allows for considerable reorganization processes, as they are observed also in experiments. Increasing the temperature leads not only to thicker lamellae but also to much wider finger structures. The interplay between the internal ordering (chain stretching) and morphology changes represents the key for the understanding of structure formation in polymer crystals... Fig. 18 A series of growth morphologies for different temperatures is displayed. The en-tropic barrier is set to ps = 0.6, a value which allows for considerable reorganization processes, as they are observed also in experiments. Increasing the temperature leads not only to thicker lamellae but also to much wider finger structures. The interplay between the internal ordering (chain stretching) and morphology changes represents the key for the understanding of structure formation in polymer crystals...
HBA. The T p values display minima, coincident with the temperatures of the y and p relaxations previously observed by dielectric and dynamic mechanical analysis. The Tjp - temperature data have been fitted to the Cole-Davidson distribution function, which indicates a broad distribution of correlation times. The activation energies obtained from the fitting are higher than from dielectric data, but, in a qualitative sense support the contention that the y relaxation is associated with the motion of HBA units, and the p relaxation with the motion of HNA units. [Pg.249]

Situation 3. We need to display temperature value in centigrade degrees. It is recommended to turn the variable into operand of the prefix-operator type with invisible name in the left part of operator =. That is, if we multiply displayed value by the constant °C equal to 1 (the third object named °C) we will get illusion that temperature is represented on relative scale t2 = 132°C. [Pg.249]


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Temperature displays

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