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Current, chemical potential

Here Po, is the current chemical potential of thermalized entity A, and G is the Gibbs potential of the entire system under consideration. [Pg.6]

Figure 2.4 Graphical interpretation of processes in a system with two conjugate reactions in respect to current chemical potentials in the presence (A) and absence (B) of a common intermediate for synthesis of products Pi and P2. Asterisks indicate points of the process reversion to involve the by-product P2 in synthesis of the "main" product P ... Figure 2.4 Graphical interpretation of processes in a system with two conjugate reactions in respect to current chemical potentials in the presence (A) and absence (B) of a common intermediate for synthesis of products Pi and P2. Asterisks indicate points of the process reversion to involve the by-product P2 in synthesis of the "main" product P ...
The discussed chemical transfomiations can be visualized in the coordi nates of current chemical potential values (see Figure 2.4a), where chemi cal potentials of components R, Pj, and P2 are the external parameters. While this is the case of the absence of common intermediates, an indirect influence of the second reaction on the first reaction is possible only when chemical potential iTp2 of compound P2 (its thermodynamic rush P2) is higher than the chemical potential of compound R (its thermodynamic rush R). When so, the consecutive reaction P2 — R Pi becomes pos sible, and this compound P2 can be involved as an additional substrate into the main reaction R — Pi. In the considered example, the phenomenon of conjugation of chemical processes is not observed. The conjuga tion takes place only in the presence of common intermediates for both channels of the transformations. [Pg.87]

Figure 4.5 A graphical interpretation of the stationary occurrence of a catalytic reaction with one catalytic intermediate in coordinates of standard and current chemical potentials. The dashed lines show distortions of the potential curves upon changes in standard thermodynamic characteristics of catalytic intermediate Kq. TSq and TS2 are the transition states. Figure 4.5 A graphical interpretation of the stationary occurrence of a catalytic reaction with one catalytic intermediate in coordinates of standard and current chemical potentials. The dashed lines show distortions of the potential curves upon changes in standard thermodynamic characteristics of catalytic intermediate Kq. TSq and TS2 are the transition states.
Analytic teclmiques often use a time-dependent generalization of Landau-Ginzburg ffee-energy fiinctionals. The different universal dynamic behaviours have been classified by Hohenberg and Halperin [94]. In the simple example of a binary fluid (model B) the concentration difference can be used as an order parameter m.. A gradient in the local chemical potential p(r) = 8F/ m(r) gives rise to a current j... [Pg.2383]

The current density j is, according to linear nonequilibrium thermodynamics, proportional to the gradient of a chemical potential difference... [Pg.868]

Thermodynamic information can also be obtained from simulations. Currently we are measuring the differences in chemical potential of various small molecules in dimethylimidazolium chloride. This involves gradually transforming one molecule into another and is a computationally intensive process. One preliminary result is that the difference in chemical potential of propane and dimethyl ether is about 17.5 kj/mol. These molecules are similar in size, but differ in their polarity. Not surprisingly, the polar ether is stabilized relative to the non-polar propane in the presence of the ionic liquid. One can also investigate the local arrangement of the ions around the solute and the contribution of different parts of the interaction to the energy. Thus, while both molecules have a favorable Lennard-Jones interaction with the cation, the main electrostatic interaction is that between the chloride ion and the ether molecule. [Pg.161]

An electrochemical reaction is said to be polarized or retarded when it is limited by various physical and chemical factors. In other words, the reduction in potential difference in volts due to net current flow between the two electrodes of the corrosion cell is termed polarization. Thus, the corrosion cell is in a state of nonequilibrium due to this polarization. Figure 4-415 is a schematic illustration of a Daniel cell. The potential difference (emf) between zinc and copper electrodes is about one volt. Upon allowing current to flow through the external resistance, the potential difference falls below one volt. As the current is increased, the voltage continues to drop and upon completely short circuiting (R = 0, therefore maximum flow of current) the potential difference falls toward about zero. This phenomenon can be plotted as a polarization diagram shown in Figure 4-416. [Pg.1262]

The electrolyte is sandwiched between two electrodes which have different but precisely known chemical potentials for the electroactive species. Since no overall current is allowed to pass the external electric circuit (i.e., =0), integration of Eq. [Pg.547]

Under most conditions, the process is spontaneous/ A chemical potential difference drives the reaction and AG < 0. When the reactants are separated as shown in Figure 9.3, the chemical potential difference can be converted to an electrical potential E. When the electrodes are connected through an external circuit, the electrical potential causes an electric current to flow. Because the electrical potential is the driving force for electrons to flow, it is sometimes... [Pg.475]

Though we and others (27-29) have demonstrated the utility and the improved sensitivity of the peroxyoxalate chemiluminescence method for analyte detection in RP-HPLC separations for appropriate substrates, a substantial area for Improvement and refinement of the technique remains. We have shown that the reactions of hydrogen peroxide and oxalate esters yield a very complex array of reactive intermediates, some of which activate the fluorophor to its fluorescent state. The mechanism for the ester reaction as well as the process for conversion of the chemical potential energy into electronic (excited state) energy remain to be detailed. Finally, the refinement of the technique for routine application of this sensitive method, including the optimization of the effi-ciencies for each of the contributing factors, is currently a major effort in the Center for Bioanalytical Research. [Pg.153]

A brief summary of current and potential processes is given in Table 8.1. As shown in the table, most of the reactions are hydrolysis, hydrogenolysis, hydration, hydrogenation, oxidation, and isomerization reactions, where catalysis plays a key role. Particularly, the role of heterogeneous catalysts has increased in this connection in recent years therefore, this chapter concerns mostly the application of heterogeneous solid catalysts in the transformation of biomass. An extensive review of various chemicals originating from nature is provided by Maki-Arvela et al. [33]. [Pg.167]

Eor galvanic circuits (cells) the OCV generally is not zero. In contrast to metal circuits, where electrons are the sole carriers, in galvanic circuits the current is transported by different carriers in the different circuit parts (i.e., by electrons and by ions). Hence when substituted into Eq. (2.9), the chemical potentials of the carriers in the intermediate circuit parts will not cancel. The concept of OCV in the case of... [Pg.27]

It is typical that in Eq. (3.23) for the EMF, all terms containing the chemical potential of electrons in the electrodes cancel in pairs, since they are contained in the expressions for the Galvani potentials, both at the interface with the electrolyte and at the interface with the other electrode. This is due to the fact that the overall current-producing reaction comprises the transfer of electrons across the interface between two metals in addition to the electrode reactions. [Pg.42]

This gives rise to an important conclusion. For nonconsumable electrodes that are not involved in the current-producing reaction, and for which the chemical potential of the electrode material is not contained in the equation for electrode potential, the latter (in contrast to a Galvani potential) depends only on the type of reaction taking place it does not depend on the nature of the electrode itself. [Pg.42]

According to the literature [21], all reported electrochemical oscillations can be classified into four classes depending on the roles of the true electrode potential (or Helmholtz-layer potential, E). Electrochemical oscillations in which E plays no essential role and remains essentially constant are known as strictly potentiostatic (Class I) oscillations, which can be regarded as chemical oscillations containing electrochemical reactions. Electrochemical oscillations in which E is involved as an essential variable but not as the autocatalytic variable are known as S-NDR (Class II) oscillations, which arise from an S-shaped negative differential resistance (S-NDR) in the current density (/) versus E curve. Oscillations in which E is the autocatalytic variable are knovm as N-NDR (Class III) oscillations, which have an N-shaped NDR. Oscillations in which the N-NDR is obscured by a current increase from another process are knovm as hidden N-NDR (HN-NDR Class IV) oscillations. It is known that N-NDR oscillations are purely current oscillations, whereas HN-NDR oscillations occur in both current and potential. The HN-NDR oscillations can be further divided into three or four subcategories, depending on how the NDR is hidden. [Pg.241]

The percutaneous absorption picture can be qualitatively clarified by considering Fig. 3, where the schematic skin cross section is placed side by side with a simple model for percutaneous absorption patterned after an electrical circuit. In the case of absorption across a membrane, the current or flux is in terms of matter or molecules rather than electrons, and the driving force is a concentration gradient (technically, a chemical potential gradient) rather than a voltage drop [38]. Each layer of a membrane acts as a diffusional resistor. The resistance of a layer is proportional to its thickness (h), inversely proportional to the diffusive mobility of a substance within it as reflected in a... [Pg.211]

Since the ionic fluxes cannot be measured individually, it is preferable to introduce the salt flux, besides solvent flux and charge flux (current density). The driving forces would then be the gradients or differences of the chemical potentials in media with different salt concentrations and different pressures, multiplied by -1. These differences must be relatively small to remain within the framework of linear irreversible thermodynamics, so that... [Pg.432]

Let us assume that the molecular transport is governed only by the differences in the chemical potential (diffusion) and neglect a possible order parameter transport by the hydrodynamic flow [1,144,157]. Then, one can postulate a linear relationship between the local current and the gradient of the local chemical potential difference p(r) [146,147] as... [Pg.177]


See other pages where Current, chemical potential is mentioned: [Pg.736]    [Pg.2383]    [Pg.333]    [Pg.2025]    [Pg.48]    [Pg.122]    [Pg.339]    [Pg.339]    [Pg.1160]    [Pg.547]    [Pg.2]    [Pg.28]    [Pg.218]    [Pg.237]    [Pg.646]    [Pg.201]    [Pg.31]    [Pg.170]    [Pg.99]    [Pg.167]    [Pg.99]    [Pg.5]    [Pg.28]    [Pg.454]    [Pg.8]    [Pg.13]    [Pg.350]    [Pg.19]    [Pg.337]   
See also in sourсe #XX -- [ Pg.32 ]




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