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Conductivity complex

Other potassium channels also play important roles here. For example, Kv4.3/ KChIP complex conducts the transient outward current, Ito, responsible for the descending phase 1 of the cardiac action potential, whereas Kvl.5 is underlying the ultra rapid delayed rectifying current, IKur, responsible for descending phase 2. Finally, inward rectifier potassium channel (Kir2 family) is responsible for IKl current, which maintains the action potential close to or at the resting level (phase 4). [Pg.391]

Contrary to the lanthanide metals, at least in the first half of the series, the conduction band of the actinide metals (bonding band of the metal) will be very complex. It will consist of 6 d, 7 s and 5 f admixtures. The physical properties, even the magnetic ones will be determined by this complex conduction band. [Pg.23]

IV. Photopolymerization Sensitized by Metal Complexes Conducting Charge... [Pg.321]

An interesting feature can be read from Figure 5-6. If the temperature is sufficiently low, a power-law behavior is found, the exponent being <1. This power-law behavior has been denoted in the literature as the universal dielectric response . It is equivalent to a nearly circular arc in the complex conductivity and impedance plane. [Pg.116]

TJased on several kinetic investigations on hydrogenations catalyzed by transition metal complexes conducted over the last few years, certain general requirements must be fulfilled if a complex is to form an effective homogeneous catalyst in solution (see Ref. 1). One condition is that the catalytically active complex must be coordinatively unsaturated another that M-H or M-C bonds must be present in the complex. [Pg.142]

Fricke, H. 1955. The complex conductivity of a suspension of stratified particles of spherical or cylindrical form. Journal of Physical Chemistry 59 168-170. [Pg.230]

In 1,2-dichloroethane, UV/VIS spectroscopic data indicate that in the mixtures of 33 and bromine there are 2 1, 1 1, 1 2 and 1 3 (33 Br2) complexes. Conductivity measurements of the same mixtures indicate that the complex 1 1 is a CT complex whilst the other complexes are ionic in character. The complexes with stoichiometry 1 2 and 1 3 (33 Br2) are bromonium tribromide and pentabromide, respectively, as indicated in Scheme 13. CT complexes with moderate stability were also reported90 between 33 and different charged electrophiles (nitrosonium and nitronium salts)... [Pg.380]

Using the theory presented in Sections II and VII, we find in analytic form the frequency dependence of the ionic complex conductivity. The features of this dependence are as follows. [Pg.81]

We conditionally may refer to the susceptibility y (327a) as translational, since it is determined by back-and-forth motion of the bound charges. Note that Eqs. (327a)-(327f) are also applicable for calculation of the ionic susceptibility y (o>) stipulated by a moving single charge, to which the complex conductivity... [Pg.253]

Section VII for a homogeneous induced distribution, characterized by F = 1. Substituting this formula into Eq. (388), we have the following expression for the complex conductivity ... [Pg.275]

At small complex frequency Z, such that Zd simple formula for the complex conductivity, analogous to Eq. (405) ... [Pg.278]

Figure 48. Real (a) and imaginary (b) parts of the normalized complex conductivity S versus normalized frequency X calculated from Eq. (400) for one-dimensional ensemble. Curves 1 are for d = 1 curves 2 are for d = 0.5. Normalized collision frequency Y = 0.05 (solid lines) and 0.1 (dashed lines). Figure 48. Real (a) and imaginary (b) parts of the normalized complex conductivity S versus normalized frequency X calculated from Eq. (400) for one-dimensional ensemble. Curves 1 are for d = 1 curves 2 are for d = 0.5. Normalized collision frequency Y = 0.05 (solid lines) and 0.1 (dashed lines).
The quantity er is the relative dielectric constant or permittivity of a dielectric medium, eo = 8.85 x 10 12 As/Vm. The quantity tan 6 represents the loss tangent of a dielectric medium. Metals in the microwave range are usually described by a complex conductivity with dominant real part for normal metals and dominant imaginary part for superconductors. [Pg.100]

Figure 53. Frequency-dependent conductivity of RbAg4ls at 129 K. (More precisely a- represents the real part of the complex conductivity.) As the continuous line shows, the jump-relaxation model in Ref.278-280 can well describe the behavior in the hopping regime.278 Reprinted from K. Funke, Prog. Solid St Chem., 22 (1993) 111-195. Copyright 1993 with permission from Elsevier. Figure 53. Frequency-dependent conductivity of RbAg4ls at 129 K. (More precisely a- represents the real part of the complex conductivity.) As the continuous line shows, the jump-relaxation model in Ref.278-280 can well describe the behavior in the hopping regime.278 Reprinted from K. Funke, Prog. Solid St Chem., 22 (1993) 111-195. Copyright 1993 with permission from Elsevier.
Gaussian half peak widths (time units) of eluting peaks complex conductivity angular velocity -potential... [Pg.71]

Unfortunately, there are few direct measurements of the complex conductivity at microwave frequencies, thereby avoiding the need for extrapolation from higher frequency data. Martens et al. (2001) present data in the range 8-600 GHz for PPy and PAni that can be described by the Drude model. However, the plasma frequencies are 7 meV, much lower than the 1 eV calculated from the known carrier density. This indicates that most carriers are localised by the disorder in the samples and that the density of delocalised states at the Fermi level is low. Prigodin and Epstein (2003) note that the low frequency response is provided by a very small fraction of the carriers that are highly mobile and have long scattering times. They develop a model for this... [Pg.392]

Here Vp has been replaced with the pressure difference between the two points is AP, K°, and K are, respectively, the usual conductivity and the complex conductivity of the electrolyte solution in the absence of the particles, (f> is the particle volume fraction, (j)c is the volume fraction of the particle core, Vc is the volume of the particle core, volume fraction of the polyelectrolyte segments, I4 is the total volume of the polyelectrolyte segments coating one particle, and po, are respectively, the mass density of the particle core and that of the electrolyte solution, and ps is the mass density of the polyelectrolyte segment, V is the suspension volume, and p(cai) is the dynamic electrophoretic mobility of the particles. Equation (26.4) is an Onsager relation between CVP and pirn), which takes a similar form for an Onsager relation between sedimentation potential and static electrophoretic mobility (Chapter 24). [Pg.511]

Mondal, P. and Hahn, H., Investigation of the complex conductivity of nanocrystalline Y203-stabilized zirconia, Berichte Der Bunsen-Gesellschaft-Physical Chemistry Chemical Physics, 1997, 101, 1765-1768. [Pg.227]

Tetrathiafulvalenes, synthesis, properties of 87MI61. Tetrachalcogenofulvalenes and their charge-transfer complexes, conducting properties and nature of heteroatoms 87YGK502. [Pg.71]

As discussed in sec. 4.5e the complex conductivity K(cu) is measurable. It contains all the required conduction and dielectric properties and can be written... [Pg.586]

Ferrocene-Containing Charge-Transfer Complexes. Conducting and Magnetic Materials... [Pg.433]

Consider a 3-D geoclectrical model with the normal (background) complex conductivity at, and local inhomogeneity D with an arbitrarily varying complex conductivity a = ati + Aa. The inhomogencity is considered to be local, so there exists some radius... [Pg.231]


See other pages where Conductivity complex is mentioned: [Pg.713]    [Pg.238]    [Pg.212]    [Pg.728]    [Pg.328]    [Pg.275]    [Pg.238]    [Pg.851]    [Pg.70]    [Pg.74]    [Pg.65]    [Pg.100]    [Pg.101]    [Pg.432]    [Pg.235]    [Pg.235]    [Pg.233]    [Pg.128]    [Pg.116]    [Pg.438]    [Pg.564]    [Pg.505]    [Pg.588]    [Pg.484]    [Pg.238]   
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