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Differentiability double integral

Double integration with respect to EA yields the surface excess rB+ however, the calculation requires that the value of this excess be known, along with the value of the first differential 3TB+/3EA for a definite potential. This value can be found, for example, by measuring the interfacial tension, especially at the potential of the electrocapillary maximum. The surface excess is often found for solutions of the alkali metals on the basis of the assumption that, at potentials sufficiently more negative than the zero-charge potential, the electrode double layer has a diffuse character without specific adsorption of any component of the electrolyte. The theory of diffuse electrical double layer is then used to determine TB+ and dTB+/3EA (see Section 4.3.1). [Pg.222]

It should be noted that if a differential mass, energy and electron balance approach were followed to describe the reactor s behavior one would obtain a set of non-linear, partial, integro-differential equations. However, since the reactor is simulated by a two-dimensional array of mixing cells, a large number of algebraic equations result in which there are no differentials and in which double integrals are replaced by double summations. [Pg.182]

We can now understand that these measurements are largely equivalent to electrocapillary information. The capacitances can be obtained from the electrocapillary curves by double differentiation, whereas the electrocapillary curves can be constructed from differential capacitances by double integration (11, 12) ... [Pg.541]

Palenzola and Cirafici [1975PAL/CIR] have measured the enthalpies of formation of ThSn3(cr) by dynamic differential calorimetry (integration of DTA curves) from an appropriate mixture of the elements, held in a molybdennm container. As discussed in Appendix A, the DTA peak reached its maximnm at 793 K. Palenzola and Cirafici [1975PAL/CIR] report the valne of Af//° (ThSns, cr) = -(162 + 16) kJ-mof to be that at 298.15 K, but make no mention of any corrections applied to the experimental valne. We have therefore assumed the value to be that at the maximum in the DTA peak, 793 K and have doubled the uncertainty stated by the anthors. However, in view of the nncertainties in the processing of the data from both these studies, these values are quoted for information only. [Pg.380]

Area, constant, optical absorption Activity, absorption coefficient Debye length Cyclic voltammogram Capacitance / j,F Double layer capacity / 0.F Differential double layer capacity Integral double layer capacity Concentration / M Surface concentration Bulk concentration / M Diffusion coefficient / cm s ... [Pg.2]

Elementary links are used to represent the properties of the energy container through an operator. In a canonical Formal (jraph, two kinds of links are possible those belonging to the system itself, such as capacitance, inductance, and conductance, and those supported by the space-time, such as the evolution property represented by the time operator or the spatial distribution represented by a spatial operator. When the operator is a purely differential one (integration or derivation), a double line is used, otherwise (space-time velocity, coupling frequency, mass transfer operator, etc.) a simple but thicker line is used. In a Differential Formal Graph, only partial derivatives with respect to a variable are allowed. [Pg.762]

It follows from Eq. (9.9) that at the maximum of the electrocapillary curve, qM = 0. In other words, the potential of zero charge, p2Cf coincides with the potential of the electrocapillary maximum. The double-layer capacitance can be obtained by double differentiation of the surface tension with respect to potential, and the surface tension can be obtained by double integration of the dependence of Cdi on E. The situation is not entirely symmetrical, however. For double differentiation, all one needs is very accurate data of y versus For double integration, one also needs two constants of integration. These are the coordinates of the electrocapillary maximum, namely Epzc and For liquid electrodes (e.g., mercury and... [Pg.131]

Electrochemical techniques such as chronocoulometry, integrated cyclic voltammetry curves, or differentiating double-layer capacity measurements as a function of bulk concentrations can be used to estimate FA however, these types of determinations may still be in error since they measure the total number of surface species, while the number of molecules at active sites which exhibit both the EM and CT effects may be much smaller. Thus, the estimates of Gsers 10 to 10 found at pretreated Ag, for example, may err on the low side if special active sites are involved in SERS. It has been estimated that only 3% of the surface sites are SERS active. " ... [Pg.319]

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.)...
If qM is evaluated experimentally, e.g. from the integration of differential capacity curves, A02 can be calculated using eqn. (44) of the diffuse double layer theory. Figure 3 shows the variation of A02 with... [Pg.35]

We have seen that the instantaneous faradaic current at an electrode is related to surface concentrations and charge transfer rate constants, and exponentially to the difference of the electrode potential from the E° of the electrochemical couple. This is represented in Figure 5.1c by Zf. With very few exceptions, this leads to intractable nonlinear differential equations. These systems have no closed form solutions and are treatable only by numerical integrations or numerical simulations (e.g., cyclic voltammetry). In addition, the double-layer capacitance itself is also nonlinear with respect to potential. [Pg.144]

In order to elucidate how the total cross section for double photoionization, equ. (5.76), can be derived from the triple-differential cross section, equ. (4.84b), the necessary integration steps will be listed (for details see [HSW91]). Assuming for simplicity completely linearly polarized incident light with the electric field vector defining the reference axis, the triple-differential cross section from equ. (4.84b) including also a constant of proportionality can be reproduced here ... [Pg.260]

Thus for numerical solution, the equations are the (at) equations n. C. 9., the (x-at) equations n. C. 10., n. C. 11. andH. C. 12. for the p + 2 variables T, P, and pX1. With all quantities known at some starting point z = 0, a computing machine can be programmed to calculate the derivatives in equations n. C. 10-12. Various machine integration routines are then available to solve simultaneous, first order differential equations. Such routines should have a variable step-wise feature for automatically doubling or halving the internal to satisfy a chosen precision index. [Pg.69]

Cd differential capacity of double layer Cj integral capacity of double layer Cs capacity in RC series combination... [Pg.444]


See other pages where Differentiability double integral is mentioned: [Pg.350]    [Pg.386]    [Pg.438]    [Pg.187]    [Pg.210]    [Pg.210]    [Pg.329]    [Pg.252]    [Pg.299]    [Pg.299]    [Pg.557]    [Pg.115]    [Pg.210]    [Pg.210]    [Pg.353]    [Pg.550]    [Pg.331]    [Pg.319]    [Pg.315]    [Pg.342]    [Pg.349]    [Pg.923]    [Pg.166]    [Pg.353]    [Pg.125]    [Pg.156]    [Pg.531]    [Pg.161]    [Pg.434]    [Pg.392]    [Pg.164]    [Pg.161]   
See also in sourсe #XX -- [ Pg.210 ]

See also in sourсe #XX -- [ Pg.210 ]




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