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Temperature variation, normalised

Table 1.4 Equations for the calculation of the normalised temperature variation Si, the dimensionless transfer capability Ni and the mean temperature difference in counter and cocurrent heat exchangers... Table 1.4 Equations for the calculation of the normalised temperature variation Si, the dimensionless transfer capability Ni and the mean temperature difference in counter and cocurrent heat exchangers...
We will now compare the two flow configurations. For C = 0 the normalised temperature variation in Table 1.4 is... [Pg.53]

The pattern can be obtained from the polymer temperature or concentration variations in addition to the change of G°N. The relaxation function may be too complicated a mathematical expression ever to be calculated, nonetheless, it obeys a property of invariance which allows the superposition of all normalised relaxation curves to one another by adjusting a suitable factor to the time scale of each curve. The time shift factor is found to obey the equation... [Pg.312]

Where Cf is a structural parameter that counts available reactive carbon sites and c, is a coefficient that account for distribution of reactive carbon sites types and catalytic effects and thus a variation in c, may change kinetic parameters. The gas composition vector (F) in J X) may beside the CO2 partial pressure also include such gas partial pressures as KOH since the likelihood that a catalytic site is activated is a function of the partial pressure of the catalyst, the site-catalyst attraction forces and the temperature. Since from Eq. (2) the structural profile invariance SPI assumption is by no means obvious we suggest that a temperature and partial pressure range are always given for the validity of the structural profile invariance assumption. Only if the invariant structural profile assumption is approximately valid a reference profile (/ /) can be used to eliminate the structural profile to form a normalised reactivity (R ) and to determine kinetics up to a constant... [Pg.63]

This new technique has been developed at Lure by A. Fontaine and E. Dartyge Figure 8 a shows the evolution of the Pt L3 edge of a dried catalyst which has been reduced, the rate of increase of temperature under a hydrogen flux being 6°/min the decrease of the amplitude of the white line is complete after one hour. Figure 8 b shows the variation of the area of this white line, normalised to that of the elemental metal. Two points are worth mentioning here ... [Pg.78]

In order to effectively assess the variation of the directionally dependent elastic modulus, the results were normalised relative to elastic modulus along Y direction, i.e. = Ej/E2 (i=l, 2 and 3), as shown in Figure 11. The comparison and difference can be more readily seen with normalised average values added. The degree of anisotropy (DA) is thus be calculated and plotted for each sintering temperature DA=l-smallest normalised modulus, with DA=0 when fliUy isotropic and DA=1, fully anisotropic. [Pg.123]

The equation states that variations in heat capacity, Cp, are normalised between unity for the liquid or imrestricted state (with heat capacity Cpi), and zero for a frozen glassy state (with heat capacity Cpg). The evolution of this factor should mirror the reduction of mobility due to vitrification only, and not the changes in heat capacity due to changes in temperature or to the chemical changes themselves. Therefore, the influence of both temperature and conversion on the reference states, Cpi and Cpg, needs to be taken into account to obtain quantitative results. [Pg.124]

Evaluation of dynamic fracture characteristics of 9Cr-lMo ferritic steel was carried out for normalised tempered (N T), aged (at 1013 K for 1-2 h) and welded conditions (with PWHT). The drop-weight nil-ductility transition temperatures (Tj ) were 248 K, 248 K and 268 K respectively for N T, aged and welded conditions. Despite the difficulties in crack-profile measurement and the uncertainties in fracture loads due to microstructural variation in HAZ of the drop-weight specimens, the particular procedure developed enabled determination of conservative estimates of at/below T. j. from instrumented drop-weight tests which are... [Pg.127]

Fig. 7.37 Variation of integrated intensities with reaction temperature. In (a) the totai intensity of the magnetite pattern (decreasing) and of the iron pattern (increasing) are composed. The straight lines indicate the discrepancy of the sum of the total diffracted intensity from the expected constant value. In (b) the evolutions of the iron (110) and (211) intensities are composed. The expectation value for the (211) reflection is calculated from the suitable scanned structure factor normalised to the (110) intensity 0 ... Fig. 7.37 Variation of integrated intensities with reaction temperature. In (a) the totai intensity of the magnetite pattern (decreasing) and of the iron pattern (increasing) are composed. The straight lines indicate the discrepancy of the sum of the total diffracted intensity from the expected constant value. In (b) the evolutions of the iron (110) and (211) intensities are composed. The expectation value for the (211) reflection is calculated from the suitable scanned structure factor normalised to the (110) intensity 0 ...

See other pages where Temperature variation, normalised is mentioned: [Pg.52]    [Pg.960]    [Pg.107]    [Pg.451]    [Pg.255]    [Pg.127]    [Pg.607]    [Pg.387]    [Pg.294]    [Pg.222]    [Pg.31]    [Pg.328]    [Pg.72]    [Pg.156]   
See also in sourсe #XX -- [ Pg.50 ]




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