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Ion distributions

Debye and Htickel [42] assumed that the ion distribution fiinctions are related to by... [Pg.486]

Particularly in polar solvents, electrostatic charges usually have an important contribution to tire particle interactions. We will first discuss tire ion distribution near a single surface, and tlien tire effect on interactions between two colloidal particles. [Pg.2676]

This is an inverse lengtli k is known as tire Debye screening lengtli (or double layer tliickness). As demonstrated below, it gives tire lengtli scale on which tire ion distribution near a surface decays to tire bulk value. Table C2.6.4 gives a few numerical examples. [Pg.2676]

The increased acidity of the larger polymers most likely leads to this reduction in metal ion activity through easier development of active bonding sites in siUcate polymers. Thus, it could be expected that interaction constants between metal ions and polymer sdanol sites vary as a function of time and the sihcate polymer size. The interaction of cations with a siUcate anion leads to a reduction in pH. This produces larger siUcate anions, which in turn increases the complexation of metal ions. Therefore, the metal ion distribution in an amorphous metal sihcate particle is expected to be nonhomogeneous. It is not known whether this occurs, but it is clear that metal ions and siUcates react in a complex process that is comparable to metal ion hydrolysis. The products of the reactions of soluble siUcates with metal salts in concentrated solutions at ambient temperature are considered to be complex mixtures of metal ions and/or metal hydroxides, coagulated coUoidal size siUca species, and siUca gels. [Pg.7]

Essential for MD simulations of nucleic acids is a proper representation of the solvent environment. This typically requires the use of an explicit solvent representation that includes counterions. Examples exist of DNA simulations performed in the absence of counterions [24], but these are rare. In most cases neutralizing salt concentrations, in which only the number of counterions required to create an electrically neutral system are included, are used. In other cases excess salt is used, and both counterions and co-ions are included [30]. Though this approach should allow for systematic smdies of the influence of salt concentration on the properties of oligonucleotides, calculations have indicated that the time required for ion distributions around DNA to properly converge are on the order of 5 ns or more [31]. This requires that preparation of nucleic acid MD simulation systems include careful consideration of both solvent placement and the addition of ions. [Pg.454]

At each phase boundary there exists a thermodynamic equilibrium between the membrane surface and the respective adjacent solution. The resulting thermodynamic equilibrium potential can then be treated like a Donnan-potential if interfering ions are excluded from the membrane phase59 6,). This means that the ion distributions and the potential difference across each interface can be expressed in thermodynamic terms. [Pg.226]

Isolation "b memhnnt Ifncmbranc T solution k = single ion distribution coefficient ... [Pg.227]

In all cases, broad diffuse reflections are observed in the high interface distance range of X-ray powder diffraction patterns. The presence of such diffuse reflection is related to a high-order distortion in the crystal structure. The intensity of the diffuse reflections drops, the closer the valencies of the cations contained in the compound are. Such compounds characterizing by similar type of crystal structure also have approximately the same type of IR absorption spectra [261]. Compounds with rock-salt-type structures with disordered ion distributions display a practically continuous absorption in the range of 900-400 cm 1 (see Fig. 44, curves 1 - 4). However, the transition into a tetragonal phase or cubic modification, characterized by the entry of the ions into certain positions in the compound, generates discrete bands in the IR absorption spectra (see Fig. 44, curves 5 - 8). [Pg.115]

Conceptual Flowsheet for the Extraction of Actinides from HLLW. Figure 5 shows a conceptual flowsheet for the extraction of all the actinides (U, Np, Pu, Am, and Cm) from HLLW using 0.4 M 0< >D[IB]CMP0 in DEB. The CMPO compound was selected for this process because of the high D m values attainable with a small concentration of extractant and because of the absence of macro-concentrations of uranyl ion. Distribution ratios relevant to the flowsheet are shown in previous tables, IV, V, VI, and VII and figures 1 and 2. One of the key features of the flowsheet is that plutonium is extracted from the feed solution and stripped from the organic phase without the addition of any nitric acid or use of ferrous sulfamate. However, oxalic acid is added to complex Zr and Mo (see Table IV). The presence of oxalic acid reduces any Np(VI) to Np(IV) (15). The presence of ferrous ion, which is... [Pg.439]

Nicholls, D.G. (1974). The influence of respiration and ATP hydrolysis on the proton electrochemical gradient across the inner membrane of rat liver mitochondria as determined by ion distribution. Eur. J. Biochem. 50,305-315. [Pg.153]

The potential of reversed micelles needs to be evaluated by theoretical analysis of the metal ion distribution within micelles, by evaluation of the free energy of the solvated ions in the reversed micelle organic solution and the bulk aqueous water, and by the experimental characterization of reversed micelles by small-angle neutron and x-ray scattering. [Pg.137]

Pitman, M.G., Lauchli, A. Stelzer (1981). Ion distribution in roots of barley seedlings as measured by electron probe X-ray micro-analysis. Plant Physiology, 66, 673-9. [Pg.113]

As the copper content of cell walls increases, the Cu " ions distribute between the two types of uronates most of them on high affinity sites first, at low copper contents more on low affinity sites afterwards. The percentage of the uronic acids that bind Cu with a high affinity is plotted on Fig. 5 as a function of the relative amount of copper in the walls. We can see that about 30% of the uronic acids consist of high affinity sites. [Pg.139]

Figure 13. Ion distribution in transverse section of flax hypocotyl. SIMS microscopy. Figure 13. Ion distribution in transverse section of flax hypocotyl. SIMS microscopy.
Space charge arises because the character of cation distribution differs from that of anion distribution (the signs of Zj are different). The volume charge density depends on the ion distribution,... [Pg.702]

The volume charge density depends on the ion distribution, which obeys the Boltzmann equation ... [Pg.705]

Implants at different energies can be used in order to obtain a flat doping ion distribution. [Pg.270]

Focusing on the example of a sohd/gas interface, in the following, we will describe how to evaluate the stabihty of non-electrochemical interfaces, which are not influenced by a potential apphed externally or caused by an inhomogeneous ion distribution within the system. In the case that both the solid and the gaseous phase are present in macroscopic quantities, we have already seen in the previous section that each of these reservoirs is characterized by its chemical potential fifT, pi), which for the non-electrochemical interface is a function of temperature and partial pressure. [Pg.132]

However, these classical models neglect various aspects of the interface, such as image charges, surface polarization, and interactions between the excess charges and the water dipoles. Therefore, the widths of the electrode/electrolyte interfaces are usually underestimated. In addition, the ion distribution within the interfaces is not fixed, which for short times might lead to much stronger electric helds near the electrodes. [Pg.138]

The term G T, a,, A/, ) is the Gibbs free energy of the full electrochemical system x < x < X2 in Fig. 5.4). It includes the electrode surface, which is influenced by possible reconstructions, adsorption, and charging, and the part of the electrolyte that deviates from the uniform ion distribution of the bulk electrolyte. The importance of these requirements becomes evident if we consider the theoretical modeling. If the interface model is chosen too small, then the excess charges on the electrode are not fuUy considered and/or, within the interface only part of the total potential drop is included, resulting in an electrostatic potential value at X = X2 that differs from the requited bulk electrolyte value < s-However, if we constrain such a model to reproduce the electrostatic potential... [Pg.139]

The above equation allows the calculation of Galvani potentials at the interfaces of immiscible electrolyte solutions in the presence of any number of ions with any valence, also including the cases of association or complexing in one of the phases. Makrlik [26] described the cases of association and formation of complexes with participation of one of the ions but in both phases. In a later work [27] Le Hung extended his approach and also considered any mutual interaction of ions and molecules present in both phases. Buck and Vanysek performed the detailed analysis of various practical cases, including membrane equilibria, of multi-ion distribution potential equations [28,29]. [Pg.22]

Selectivity of ion channels for metal ions is of great current interest (66), as it relates to conduction of nerve signals, maintenance of the appropriate metal ion distribution in the intracellular and extracellular... [Pg.131]

The output of a Nd YLF laser is focussed by a series of lenses to a spot size of 0.5 pm upon a sample which may be positioned by an x-y-z stepping motor stage and scanned by a computer-controlled high frequency x-y-z piezo stage. Ions are accelerated and transmitted through the central bore of the objective into a time-of-flight (TOF) mass spectrometer. The laser scans an area of 100 x 100 pm with a minimum step size of 0.25 pm. TOF mass spectra of each pixel are evaluated with respect to several ion signals and transformed into two-dimensional ion distribution plots. [Pg.62]

The 3D density contour maps for the Na+ ion distribution determined over the last 250 ns of simulation (Figure 14-8) show that the overall highest probability Na+ occupation sites were concentrated in the active site for both the reactant and activated precursor. This suggests that the HHR folds to form a strong local electronegative pocket that is able to attract and bind Mg2+ if present in solution, or recruit a high local concentrations of Na+ ions in the absence of Mg2+. [Pg.397]

Figure 14-8. The 3D density contour maps (yellow) of Na+ ion distributions derived from the activated precursor simulation. The hammerhead ribozyme is shown in blue with the active site in red. Only the high-density contour is shown here to indicate the electrostatic recruiting pocket formed in the active site... Figure 14-8. The 3D density contour maps (yellow) of Na+ ion distributions derived from the activated precursor simulation. The hammerhead ribozyme is shown in blue with the active site in red. Only the high-density contour is shown here to indicate the electrostatic recruiting pocket formed in the active site...
Describe how differences in ion distribution and permeability contribute to the resting membrane potential... [Pg.17]

In specific applications, it is critically important to know which isomer is produced in a particular situation in order to ascertain its further reactivity. Indeed, further reactivity, in the form of rate coefficients and product ion distributions, both identifies which reactions generate the same isomeric forms and gives information to enable the isomeric forms to be identified (often by determining the energetics and comparing them with theoretical calculations). One such application is to molecular synthesis in interstellar gas clouds. In the synthesis of the >115 molecules (mainly neutral -85%) detected in these clouds,14 a major production route is via the radiatively stabilized analog of the collisional association discussed above,15 viz. ... [Pg.86]

The reactions and identification of small isomeric species were reviewed by McEwan in 199223 Since that time, additional experimental data have been obtained on more complex systems. In the present review, smaller systems will only be mentioned where there has been an advance since the previous review and emphasis here will be concentrated on the correlation between reactivity, the form of the potential surface, and the isomeric forms. There is also a wealth of kinetic data (rate coefficients and product ion distributions) for ion-molecule reactions in the compilations of Ikezoe et al.24 and Anicich,25,26 some of which refer to isomeric species. Thermochemical data relevant to such systems, and some isomeric information, is contained in the compilations of Rosenstock et al.,27 Lias et al.,28 29 and Hunter and Lias.30... [Pg.87]

Table 1. Summarized Rate Coefficients (cm3 s 1) and Product Ion Distributions (%) for the Reactions of the Acyclic Isomer, HC3H2, of C3H3 with the Reactant Neutral... Table 1. Summarized Rate Coefficients (cm3 s 1) and Product Ion Distributions (%) for the Reactions of the Acyclic Isomer, HC3H2, of C3H3 with the Reactant Neutral...

See other pages where Ion distributions is mentioned: [Pg.169]    [Pg.620]    [Pg.212]    [Pg.354]    [Pg.118]    [Pg.74]    [Pg.179]    [Pg.255]    [Pg.257]    [Pg.630]    [Pg.318]    [Pg.318]    [Pg.272]    [Pg.209]    [Pg.288]    [Pg.509]    [Pg.88]    [Pg.88]   
See also in sourсe #XX -- [ Pg.115 , Pg.116 ]

See also in sourсe #XX -- [ Pg.236 ]




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Alkaline earth ions distribution coefficients

Angular distribution of product ions

Angular distribution of secondary Ions

Angular distribution, secondary ions

Boltzmann distribution of ions

Boltzmann distribution, solution potential-determining ions

Charge Distribution around an Ion

Cobalt ions, equilibrium distribution

Distribution functions oxidized ions

Distribution functions reduced ions

Distribution of ions

Distribution superoxide ions

Distributions of divalent transition metal ions between coexisting ferromagnesian silicates

Distributions of transition metal ions in the Mantle

Distributions of trivalent transition metal ions in mineral assemblages

Electron Stimulated Ion Angular Distribution

Electron stimulated desorption ion angular distribution

Electron-stimulated desorption ion angular distribution, ESDIAD

Em, measurement permeant ion distribution

Energy Distribution in Products of Ion-Molecule Reactions

Energy distribution of ions

Enolate ions electron distribution

Equilibrium distribution of ions

Field ion energy distributions

Flight times spatially distributed ions

Fluoride ions, charge distribution

Ion cluster distribution

Ion distribution determination

Ion energy distribution

Ion exchange selectivity distribution coefficient

Lithium ions, charge distribution

Metal ion distribution

Non-equilibrium distribution of adsorbing ions along the diffuse layer

Secondary ion energy distribution

The Ion Distribution

The distribution of ions in an electric field near a charged surface

Theoretical background for the distribution of ion-pairs

Velocity distribution, MALDI ions

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