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Capacity measurement

Fig. V-12. Variation of the integral capacity of the double layer with potential for 1 N sodium sulfate , from differential capacity measurements 0, from the electrocapillary curves O, from direct measurements. (From Ref. 113.)... Fig. V-12. Variation of the integral capacity of the double layer with potential for 1 N sodium sulfate , from differential capacity measurements 0, from the electrocapillary curves O, from direct measurements. (From Ref. 113.)...
Hence, it is necessary to correct the temperature change observed to the value it would have been if there was no leak. This is achieved by measuring the temperature of the calorimeter for a time period both before and after the process and applying Newton s law of cooling. This correction can be reduced by using the teclmique of adiabatic calorimetry, where the temperature of the jacket is kept at the same temperature as the calorimeter as a temperature change occurs. This teclmique requires more elaborate temperature control and it is prunarily used in accurate heat capacity measurements at low temperatures. [Pg.1901]

The temperature dependence of the open circuit voltage has been accurately determined (22) from heat capacity measurements (23). The temperature coefficients are given in Table 2. The accuracy of these temperature coefficients does not depend on the accuracy of the open circuit voltages at 25°C shown in Table 1. Using the data in Tables 1 and 2, the open circuit voltage can be calculated from 0 to 60°C at concentrations of sulfuric acid from 0.1 to 13.877 m. [Pg.573]

Potassium Pentaborate Tetrahydrate. Potassium pentaborate tetrahydrate, KB Og 4H2O or K2O -5B202 8H20 formula wt, 293.20 orthorhombic prisms sp gr, 1.74 heat capacity, 329.0 J/(mol-K) [78.6 cal/(mol-K)] at 296.6 K is much less soluble than sodium pentaborate (Tables 9 and 10). Heat capacity measurements on the soHd have been made over a broad temperature range (85). [Pg.206]

With liquids, the refractive index at a specified temperature and wavelength is a sensitive test of purity. Note however that this is sensitive to dissolved gases such as O2, N2 or CO2. Under favourable conditions, freezing curve studies are sensitive to impurity levels of as little as 0.(X)1 moles per cent. Analogous fusion curves or heat capacity measurements can be up to ten times as sensitive as this. With these exceptions, most of the above methods are rather insensitive, especially if the impurities and the substances in which they occur are chemically similar. In some cases, even an impurity comprising many parts per million of a sample may escape detection. [Pg.2]

Measurements of the adsorption of inhibitors on corroding metals are best carried out using the direct methods of radio-tracer detection and solution depletion measurements . These methods provide unambiguous information on uptake, whereas the corrosion reactions may interfere with the indirect methods of adsorption determination, such as double layer capacity measurements", coulometry", ellipsometry and reflectivity Nevertheless, double layer capacity measurements have been widely used for the determination of inhibitor adsorption on corroding metals, with apparently consistent results, though the interpretation may not be straightforward in some cases. [Pg.806]

Equation (4.2) requires that the total area above 0 Kelvin be obtained, but heat capacity measurements cannot be made to the absolute zero of temperature. The lowest practical limit is usually in the range from 5 K to 10 K, and heat capacity below this temperature must be obtained by extrapolation. In the limit of low temperatures, Cp for most substances follows the Debye low-temperature heat capacity relationship11 given by equation (4.4)... [Pg.157]

This result is in excellent agreement with the value of Sm.o = 18.1 JKr moI-1 obtained from the heat capacity measurements.10... [Pg.176]

Catalysts such as charcoal can be used to maintain the equilibrium ratio of ortho-hydrogen to para-hydrogen with decreasing temperature.1 When this happens, heat capacity measurements give the equilibrium value for the entropy of hydrogen. [Pg.176]

J. Boerio-Goates, "Heat-Capacity Measurements and Thermodynamic Functions of Crystalline a-D-Glucose at Temperatures from 0 K to 350 K.". J. Chem. Thermodyn.. 23, 403-409 (1991). [Pg.201]

In Chapter 5 we saw how to determine Cp, 2 from heat capacity measurements. 07 is easily obtained from these same measurements using equation (7.106), after the value of C° 2 is obtained by extrapolation of Cp. 2 to infinite dilution. [Pg.366]

The obtained value AHf(PUF3,c) = - 1585.7 + 2.9 kJ.mol-1 cannot be considered as entirely satisfactory as the reliability of the adopted value for the enthalpy of dehydration is not demonstrated. The only experimentally known enthalpies of formation for the actinide trifluorides are AHf(PuF3,c) and AHf(UF3,c) accuracy is therefore essential if these two data are used to estimate the enthalpies of formation of the other trifluorides. The low temperature heat capacity measurements of Osborne et al. (22) using 242PuF3(c) yield S°(PuF3,c 126.11+0.38 J.K"l.mol"i. [Pg.81]

Maurer et al. [57] determined the foaming power of octadecyl sulfuric acid and several of its salts, such as sodium, triethylamine, triethanolamine, and some amino acids. Foam capacity, measured by the Ross-Miles test [150] at 60°C, was in the range of 180-210 mm showing comparatively few differences. [Pg.268]

Quite similar equations can be formulated for AG and AH by use of the partition function f of the activated complex. It follows from equations (6) and (7) that AEp can only be evaluated if the partition functions and AEz are available from spectroscopic data or heat capacity measurements. However, if AG = AH, the entropy change AS equals zero, and if AEz also equal to zero, either AG or AH can then be identified with the potential energy change. If... [Pg.415]

Frequently it has been observed with n-type as well as with p-type electrodes in aqueous solutions that the onset potential of the pure photocurrent differs considerably from the flatband potential. The latter can be determined by capacity measurements in the dark as illustrated by the dashed line in the ij — Ub curve in Fig. 8 a. This effect is usually explained by recombination and trapping of minority carriers created by light excitation at the surface. It is obvious that these effects have a negative effect... [Pg.95]

E (A4>). This relation can be used to plot y (E ) from Fig. 5.7 as a function of the electrode potential, y [E (A(j))], for different electrolytes and concentrations, depending on which experimental capacity measurements have been used for the integration. Since these measurements were performed with an SCE, we have added a corresponding subscript to the electrode potential. [Pg.147]

An automated procedure to measure peak widths for peak capacity measurements has been proposed.35 Since peak width varies through the separation, the peak capacity as conventionally measured depends on the sampling procedure. The integral of reciprocal base peak width vs. retention time provides a peak capacity independent of retention time, but requires an accurate calculation of peak width. Peak overlap complicates automation of calculation. Use of the second derivative in the magnitude-concavity method gives an accurate value of the standard deviation of the peak, from which the base peak width can be calculated. [Pg.62]

B28. Bladon, P. T., Rowlands, T. E., Whittaker, J. A., and Oakey, R. E., Serum cortisol binding capacity measured with concanavalin A-Sepharose in patients with a recent inflammatory response. Clin. Chim. Acta 253,9-20 (1996). [Pg.109]

Equipment Material of construction Capacity measure Base size Qb Base cost CB ( ) Size range Cost exponent M... [Pg.18]

CSLF A taskforce for review and development of standards with regards to storage capacity measurment 2005. [Pg.168]

Bradshaw J., Bachu S., et al. Discussion paper on C02 storage capacity estimation (Phase 1) A taskforce for review and development of standards with regards to storage capacity measurment. 2005 CSLF-T 15. [Pg.168]

Heat capacity measurements at the glass transition temperature, Tg, are based on the same differential concept. The weight fraction of amorphous phase is calculated as the ratio of changes of heat capacity of the semi-crystalline sample ACp(S) over the change in heat capacity of the melt (ACp(m)) at the glass transition. For a two-phase system, the degree of crystallinity is given as ... [Pg.272]

Figure 1 presents the plot of the BET specific surface area vs the irreversible capacity measured for graphite samples milled in different atmospheres and sometimes post-treated by pyrolytic carbon deposition. The experimental values are quite scarce and, contrarily to several claims [7-9], there is not any linear dependence between these two parameters. It seems that the linearity would exist only for samples from the same family with comparable microtextures. [Pg.251]

The cycling improvement for the Cu-metallized graphite over the pristine graphite was also observed by K. Guo et al. [15] in their study of electroless Cu deposited on graphite cycled in a lithium cell with a 20% PC blend electrolyte. Also, they recorded a rate capability improvement in their Cu graphite material as well. At a current density of 1.4 mA/cm2, the cell achieved about 60% ( 200 mAh/g) of the charge capacity measured at 0.14 mA/cm2, compared to about 30% ( 100 mAh/g) for the non-treated pristine natural graphite cell [15]. [Pg.381]

Heat capacity measurements can also be used to extract A7 ad in addition to Sm(T) (Equations 9.3a and 9.3b), where CM is the heat capacity of magnetization for a more complete analysis fHt... [Pg.296]

Fig. 3.1. Debye temperature versus temperature for some materials. The values of Debye temperatures are obtained by heat capacity measurements [10,11]. Fig. 3.1. Debye temperature versus temperature for some materials. The values of Debye temperatures are obtained by heat capacity measurements [10,11].
Let us examine in Fig. 12.1 a schematics of a set up for heat capacity measurement a support (Sp) of heat capacity CSp is thermally linked to the thermal bath through a thermal resistance RG = l/G. [Pg.283]

Fig. 12.2. Thermal equivalent circuit for the heat capacity measurement. Fig. 12.2. Thermal equivalent circuit for the heat capacity measurement.

See other pages where Capacity measurement is mentioned: [Pg.1905]    [Pg.2559]    [Pg.2560]    [Pg.2749]    [Pg.433]    [Pg.25]    [Pg.149]    [Pg.216]    [Pg.81]    [Pg.120]    [Pg.795]    [Pg.800]    [Pg.105]    [Pg.190]    [Pg.226]    [Pg.282]    [Pg.371]    [Pg.616]    [Pg.85]    [Pg.146]    [Pg.218]    [Pg.105]    [Pg.283]   
See also in sourсe #XX -- [ Pg.133 ]




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