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Current distribution definition

In resolving the apparent paradox of how an antenna with no charge (in free space) can have an electric-dipole moment, one can go back to definitions. In Ref. 14 the fields from a current distribution are evaluated by expanding... [Pg.636]

The primary potential distribution is, by definition, uniform adjacent to the electrode surface, but the current distribution is highly nonuniform (Fig. 10). It is a general characteristic of the primary current distribution that the current density is infinite at the intersection of an electrode and a coplanar insulator. This condition obtains at the periphery of the disk electrode, and the current density becomes infinite at that point. Additional resistance due to kinetic limitations invariably reduces the nonuniformity of the current distribution. In this system the current distribution becomes more uniform as the Wagner number increases. Theoretically, the current distribution is totally uniform as the Wagner number approaches infinity. [Pg.246]

In the case of solid electrolytes, such a calibration is usually impossible. The configuration of measuring cells should be selected to provide uniform current distribution or to enable use of a definite solution of differential Ohm s law for the conductivity calculations [ii-iv]. The conductivity values are typically verified comparing the data on samples with different geometry and/or electrode arrangement, or using alternative measurement methods. [Pg.111]

Following the definition of / given in equation (13.49), the curves for / = 0 in Figures 13.6(a) and (b) correspond to an ideally capacitive blocking electrode. The steady-state solution for the current distribution at a blocking electrode is that the current is equal to zero. The primary current distribution given as equation (5.65) therefore applies, not at the steady state, but at infinite frequency. For the special case of a Faradaic system with an Ohmic resistance that is mudh larger than the kinetic resistance, / —> oo, and equation (5.65) provides the steady-state current distribution. [Pg.247]

We digress for a moment to recall that surface current density, in parallel with the definition of surface charge, is the limit of the current distribution flowing within a surface layer of finite thickness 8 when 6—>0, where the current per unit width of surface in the direction normal to that of the current flow remains finite. The surface current density is expressed through the relation... [Pg.203]

Ibl carries the argument on equalizing action of overvoltage a step further. As we have seen, current distribution is more uniform when ratio RJRg is greater. Now R is the resistance of the solution per m of cross-sectional area, and is given by the specific resistance times the distance between the two electrodes (d). Expressed in terms of the specific conductivity K, Rg = d/K. Remembering the definition of R , we obtain ... [Pg.214]

Fig. 2.17 Current distributions for a parallel-plate reactor in fully developed laminar flow, (a) Definition sketch, (b) Normalized current as a function of dimensionless distance along the electrode. Fig. 2.17 Current distributions for a parallel-plate reactor in fully developed laminar flow, (a) Definition sketch, (b) Normalized current as a function of dimensionless distance along the electrode.
Fig. 2.22 Potential and current distributions in a fluidized-bed electrode (a definition of terms is given in the caption to Fig. 2.21). (a) and (b) thin beds, (c) and (d) thick beds. Fig. 2.22 Potential and current distributions in a fluidized-bed electrode (a definition of terms is given in the caption to Fig. 2.21). (a) and (b) thin beds, (c) and (d) thick beds.
The sub-micro level cannot easily be seen directly, and while its principles and components are currently accepted as tme and real, it depends on the atonuc theory of matter. The scientific definition of a theory can be emphasised here with the picture of the atom constantly being revised. As Silberberg (2006) points out, scientists are confident about the distribution of electrons but the interactions between protons and neutrons within the nucleus are still on the frontier of discovery (p. 54). This demorrstrates the dynamic and exciting nature of chemistry. Appreciating this overview of how scierrtific ideas are developing may help students to expand their epistemology of science. [Pg.173]

Despite the ubiquitous distribution of chlorophylls in all photosynthetic plants, quantitative information exists only for a few vegetables. The most common edible plants lack definitive data and consequently no information is available about chlorophyll distribution in current food composition tables. Still more difficult is to find analytical data in literature about the individual amounts of chlorophyll a and b and their respective derivatives. [Pg.195]

Another property relevant to the current discussion is the distribution of water in the active site. Specifically, we characterize the population of various water wires connecting the zinc-bound water/hydroxide and His 64 found in the SCC-DFTB/MM simulations. These wires were identified following a definition of hydrogen-bond in terms of both distance (O—O < 3.5 A) and angle (O—H—O > 140°) and care... [Pg.184]

This section summarizes the current information about different human keratins, their functional significance, cell-type-specific distribution as well as their coexpression with myoepithelial markers and estrogen receptor alpha (ER), because these markers exhibit characteristic expression patterns in some human breast tumors. In many of these cases, a definite diagnosis can be achieved only when additional information is provided by immunohistochemistry. [Pg.110]

Here n designates the density or distribution function j the diffusion current vd the apparent velocity, namely, the drift velocity, of a Brownian particle and D the diffusion constant. Equation (1) is a continuity equation while Eq. (2) is simply Fick s law augmented by a definition of vd. [Pg.364]


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See also in sourсe #XX -- [ Pg.28 , Pg.74 ]




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