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Equation experimental applications

Although Gibbs published his monumental treatise on heterogeneous equilibrium in 187S, his work was not generally appreciated until the turn of the century, and it was not until many years later that the field of surface chemistry developed to the point that experimental applications of the Gibbs equation became important. [Pg.79]

The most convenient form of the BET equation for application to experimental data is that already given in Equation (2.13), viz... [Pg.49]

Equations (4-5) and (4-7) are alternative expressions for the estimation of the diffusion-limited rate constant, but these equations are not equivalent, because Eq. (4-7) includes the assumption that the Stokes-Einstein equation is applicable. Olea and Thomas" measured the kinetics of quenching of pyrene fluorescence in several solvents and also measured diffusion coefficients. The diffusion coefficients did not vary as t) [as predicted by Eq. (4-6)], but roughly as Tf. Thus Eq. (4-7) is not valid, in this system, whereas Eq. (4-5), used with the experimentally measured diffusion coefficients, gave reasonable agreement with measured rate constants. [Pg.136]

This chapter has provided a brief overview of the application of optimal control theory to the control of molecular processes. It has addressed only the theoretical aspects and approaches to the topic and has not covered the many successful experimental applications [33, 37, 164-183], arising especially from the closed-loop approach of Rabitz [32]. The basic formulae have been presented and carefully derived in Section II and Appendix A, respectively. The theory required for application to photodissociation and unimolecular dissociation processes is also discussed in Section II, while the new equations needed in this connection are derived in Appendix B. An exciting related area of coherent control which has not been treated in this review is that of the control of bimolecular chemical reactions, in which both initial and final states are continuum scattering states [7, 14, 27-29, 184-188]. [Pg.73]

The authors have verified Eq. (43) for an orifice diameter of 0.192 cm. The results, given in Table IV, show good agreement between the theoretical and the experimental values. The data for the range of 2.5 cm3/sec to 14 cm3/sec are not reported by the authors and it is not known which of the equations is applicable. [Pg.292]

Miller s recommended equation actually had a higher constant (0.029) substituted for the value of 0.023 shown in Eq. (37). This was found necessary to enable correlation of his data on both water and aqueous suspensions, i.e., he was able to conclude that the same correlating equation is applicable to pure liquids and suspensions alike, although the coefficients were high for both. For the former, Eq. (37) is usually suitable hence it may be concluded that the consistently high coefficients reported by Miller were probably due to unusual experimental factors and are not of general interest. [Pg.127]

This equation is particularly useful if v = v (i.e if v is constant). Having determined v in advance by means of labeled atoms or any other method or having assumed a certain value of v as a hypothesis, we pass over from experimental r values to r+ values that dep6nd in a simpler way on partial pressures (or concentrations) of substances. This facilitates the determination of a kinetic equation. For instance, often the following form of equation is applicable ... [Pg.207]

A detailed examination of the mass transport effects of the HMRDE has been made. At low rotation speeds and for small amplitude modulations (as defined in Section 10.3.6.2) the response of the current is found to agree exactly with that predicted by the steady-state Levich theory (equations (10.15)-(10.17)) [27, 36, 37]. Theoretical and experimental application of the HMRDE, under these conditions, to cases where the electrode reaction rate constant was comparable to the mass-transfer coefficient has also been made [36]. At higher rotation speeds and/or larger amplitude modulations, the observed current response deviated from the expected Levich behaviour. [Pg.396]

Disadvantage of this equation is false identification of inoculum volume with volume of tumor. Moreover, limited relative volume of tumor more than in three exceeds the maximum relative volume observing experimentally. Application of catalysis equation [11] of the form ... [Pg.91]

Approximate Methods for Bases.—The procedures described for determining the dissociation constants of acids can also be applied, in principle, to bases analogous equations are applicable except that hydroxyl ions replace hydrogen ions, and vice versa, in all the expressions. Since the value of the product of an and ooir is known to have a definite value at every temperature (cf. Table LXI), it is possible to derive ooh" from obtained experimentally. [Pg.329]

The most reliable data are from studies of hydrogen evolution on mercury cathodes in acid solutions. This reaction has been studied most extensively over the years. The use of a renewable surface (a dropping mercury electrode, in which a new surface is formed every few seconds), our ability to purify the electrode by distillation, the long range of overpotentials over which the Tafel equation is applicable and the relatively simple mechanism of the reaction in this system all combine to give high credence to the conclusion that p = 0.5. This value has been used in almost all mechanistic studies in electrode kinetics and has led to consistent interpretations of the experimental behavior. It... [Pg.386]

Experimental investigations on convective heat transfer in liquid flows in microchannels have been in the continuum regime. Hence, the conventional Navier-Stokes equations are applicable. [Pg.19]

In the experimental application of these equations, we must remember that c refers to the ionic concentration and not to the total concentration. AVe cannot therefore expect our equations to be in exact agreement with experiment as long as we are ignorant of the exact value of the degree of ionisation. Conversely, however, we may use an experimental determination of the e. m.f. to calculate the degree of ionisation or the transference number. The validity of the Nernst equations has been placed beyond doubt by the results of numerous measurements. [Pg.359]

Eq. (6.2) in terms of photon number n and quantization volume V, is not directly amenable to experimental application. Moreover, since the quantization volume is merely a theoretical artefact, it must invariably cancel out in any final rate equation. However the ratio of photon number and quantization volume is directly related to the mean irradiance I the relationship is as follows ... [Pg.60]

Stuve et al. [78STU/FER] also reported the results of a limited set of drop calorimetry experiments (402.9 to 1001.5 K). The authors fitted an equation to the experimental enthalpy differences such that the heat capacity values meshed smoothly with the value obtained tfom adiabatic calorimetry for 298.15 K. The authors indicated that their equation was applicable, within 0.6 per cent for temperatures between 298 and 1200 K. As discussed below, NiS04 decomposes towards the upper end of this temperature range, and extrapolation of the heat capacities to 1200 K does not seem justified. Conversion of the equation from calorie to joule units leads to ... [Pg.194]

The nonrandom, two-liquid (NRTL) equation developed by Renon and Prausnitz, as listed in Table 5.3, represents an accepted extension of Wilson s concept. The NRTL equation is applicable to multicomponent vapor-liquid, liquid-liquid, and vapor-liquid-liquid systems. For multicomponent vapor-liquid systems, only binary-pair constants from the corresponding binary-pair experimental data are required. [Pg.119]

It is an experimental fact that the Arrhenius equation is applicable to bioprocesses. A theoretical prerequisite for the Arrhenius equation is well known—that the velocities of, for example, gas particles follow a Boltzmann distribution. The distribution becomes narrower with increasing molecular weight, so that in the case of enzymes and cells it barely exists. Without the theoretical background, application of the Arrhenius equation to a microbiological processes must be considered a formal kinetic procedure with appropriate fitting parameters. [Pg.201]

One of the advantages of the Fox equation is that it does not contain adjustable parameters. An agreement of experimental data with the prediction supports the conclusion of the high miscibility. Data from different authors are consistent and show that up to 45 wt% of ATBC content in PLA, the Fox equation is applicable. At concentrations equal to or higher than 60 wt%, ATBC phase separation is evidenced in a miscible PLA/ATBC blend of stable composition and a pure ATBC phase. Consequently two Tg values can be measured, where the high temperature transition becomes independent... [Pg.145]

Here, [t)] is the shape-dependent intrinsic viscosity, viz. [t ] = 2.5 for spheres and is the maximum packing volume fraction. Owing to < )-dependent rotation and orientation of particles, the flow of suspensions with anisometric particles is more complex. Here also Simha s equation is applicable, but experimental values of the two parameters, [t ] and < ) should be used. [Pg.719]

The method is useful for materials in which there is no capillary condensation below p/pt 0.7-0.8. The equation is applicable up to at least p/p 0.3. A theoretical equation for the /-curve not requiring any adjustable constants was proposed by Ternan (46). Based on thermodynamics, and taking into account dispersion forces using the Lennard-Jones potential, the equation related relative pressure to Him thickness in reasonable agreement with experimental data. [Pg.470]

When electrolytes are added to a solvent, they dissociate to a certain degree. It would appear that the solution contains at least three components solvent, anions, and cations. If the solution is to remain neutral in charge at each point, assuming the absence of any applied electric potential field, the anions and cations diffuse effectively as a single component, as with molecular diffusion. The diffusion of the anionic and cationic species in the solvent can thus be treated as a binary mixture. The theory of dilute diffusion of salts is well developed and has been experimentally verified. For dilute solutions of a single salt, the Nernst-Haskell equation is applicable ... [Pg.190]

The general Avrami equation is applicable to any type of crystallization. It is not restricted to polymers. It describes the time evolution of the overall crystallinity. The pioneer work was conducted during the 1930s and 1940s by Evans, Kolmogoroff, Johnson and Mehl, and Avrami. Wunderlich (1978) concludes that without the parallel knowledge of the microscopic, independently proven mechanism, the macroscopic, experimentally derived Avrami equation and the Avrami parameters are only a convenient means to represent empirical data of crystallization. However, interest in the Avrami equation has been... [Pg.175]

An evaluation of the experimental results of this work has shown that this equation is applicable to a Wep/Frp number range of around 28.8 to 1300. Based on the results on the liquid hold-up, it can be concluded that by modifying the models known from literature [12, 19, 44], the total liquid hold-up below the loading line can be determined with... [Pg.285]


See other pages where Equation experimental applications is mentioned: [Pg.615]    [Pg.113]    [Pg.112]    [Pg.649]    [Pg.52]    [Pg.291]    [Pg.292]    [Pg.660]    [Pg.216]    [Pg.427]    [Pg.1030]    [Pg.44]    [Pg.22]    [Pg.345]    [Pg.53]    [Pg.47]    [Pg.422]    [Pg.333]    [Pg.1843]    [Pg.196]    [Pg.123]    [Pg.427]    [Pg.1676]    [Pg.161]    [Pg.282]   
See also in sourсe #XX -- [ Pg.615 ]




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Application of the BET equation to experimental data

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