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Polarity variables

To the best of our knowledge, this is the only free energy functional that can be readily introduced in an ASC implicit solvent model as it involves only surface integrals in terms of the independent polarization variable which is no longer a three-dimensional field, but instead assumes the form of a surface charge distribution on the dielectric boundary. [Pg.69]

The absorption of two different photons also significantly increases the number of polarization variables arising in the rate equations. The ability of the experimentalist to independently vary the polarization and experimental configuration of the two laser beams allows a choice of values for these polarization parameters which significantly increases the amount of information that can be derived from the spectra. In contrast to the case of single-beam excitation, this also affords the opportunity to observe the induction of circular dichroism in a system of achiral molecules. [Pg.51]

According to equation (5.63d), the standard form of the system has the following form (in polar variables r, [Pg.183]

We refer to a previous paper [5] for a description of the model and of its relevance for a semiclassical discussion of regular and irregular modes in classical and quantum mechanics [30,31]. By relating the polar variable p and the parameter q... [Pg.391]

To transpose these polar variables into dipolar variables, it is convenient to define the Peltier potential difference, notated with an uppercase pi (U), as the dipolar potential... [Pg.643]

The rough grid search was carried out as follows The polar variables that determine the relative positions of the two adjacent molecules were altered in constant intervals. The colatitutes and 62 were varied in 4 degree steps, and the longitudes (j)i and 02 8 degree steps. Unequal step size in these variables represent roughly... [Pg.395]

We start by recalling the basis of Marcus theory, formulated with the microscopic energy gap variable AE instead of the macroscopic solvent polarization variable used originally by Marcus. The derivation is standard but makes it possible to introduce the various quantities of interest and for the relationships to be generalized. [Pg.468]

Using the polarity example as mentioned earlier, it can be demonstrated how the various polarity variables are related. The most frequently used McReynolds polarity (MR) served as dependent variable. The following model can be built ... [Pg.152]

Backward elimination procedure has kept X variables DC and XB from among six polarity variables. The remaining variables (YB, XN, XD, and Kc) are not significant at the 5% level. [Pg.152]

It is clear from our discussion of contact angle hysteresis that there is some degree of variability in reported contact angle values. The data collected in Table X-2, therefore, are intended mainly as a guide to the type of behavior to be expected. The older data comprise mainly results for refractory and relatively polar solids, while newer data are for polymeric surfaces. [Pg.364]

For the interaction between a nonlinear molecule and an atom, one can place the coordinate system at the centre of mass of the molecule so that the PES is a fiinction of tlie three spherical polar coordinates needed to specify the location of the atom. If the molecule is linear, V does not depend on <() and the PES is a fiinction of only two variables. In the general case of two nonlinear molecules, the interaction energy depends on the distance between the centres of mass, and five of the six Euler angles needed to specify the relative orientation of the molecular axes with respect to the global or space-fixed coordinate axes. [Pg.186]

The remarkable stability and eontrollability of NMR speetrometers penults not only the preeise aeeiimulation of FIDs over several hours, but also the aequisition of long series of speetra differing only in some stepped variable sueh as an interpulse delay. A peak at any one ehemieal shift will typieally vary in intensity as this series is traversed. All the sinusoidal eomponents of this variation with time ean then be extraeted, by Fourier transfomiation of the variations. For example, suppose that the nomial ID NMR aequisition sequenee (relaxation delay, 90° pulse, eolleet FID) is replaeed by the 2D sequenee (relaxation delay, 90° pulse, delay i -90° pulse, eolleet FID) and that x is inereased linearly from a low value to ereate the seeond dimension. The polarization transfer proeess outlined in die previous seetion will then eause the peaks of one multiplet to be modulated in intensity, at the frequeneies of any other multiplet with whieh it shares a eoupling. [Pg.1457]

The phase of a transition in a CIDNP speetnim ean be detennined rising niles developed by Kaptein [20]. The nile for the net effeet is shown in equation (Bl.16.6). For eaeh tenn, the sign (-t or -) of that value is inserted, and the final sign detennines the phase of the polarization phis is absorptive and minns is emissive. The variables are defined in the eaption to figure B 1.16.7. [Pg.1599]

The range of integration and the meaning of the variables x will be defined by the specific problem of interest for example, in polar coordinates for one particle, x r,0,( ), and for N... [Pg.543]

Figure 10,5 Definition of the variables used to describe the electric field produced by the oscillation of the charge q under the influence of vertically polarized light. (Reprinted from Ref. 2, p. 164.)... Figure 10,5 Definition of the variables used to describe the electric field produced by the oscillation of the charge q under the influence of vertically polarized light. (Reprinted from Ref. 2, p. 164.)...
As can be seen from Eigure 11b, the output voltage of a fuel cell decreases as the electrical load is increased. The theoretical polarization voltage of 1.23 V/cell (at no load) is not actually realized owing to various losses. Typically, soHd polymer electrolyte fuel cells operate at 0.75 V/cell under peak load conditions or at about a 60% efficiency. The efficiency of a fuel cell is a function of such variables as catalyst material, operating temperature, reactant pressure, and current density. At low current densities efficiencies as high as 75% are achievable. [Pg.462]

Membrane Characterization Membranes are always rated for flux and rejection. NaCl is always used as one measure of rejection, and for a veiy good RO membrane, it will be 99.7 percent or more. Nanofiltration membranes are also tested on a larger solute, commonly MgS04. Test results are veiy much a function of how the test is run, and membrane suppliers are usually specific on the test conditions. Salt concentration will be specified as some average of feed and exit concentration, but both are bulk values. Salt concentration at the membrane governs performance. Flux, pressure, membrane geome-tiy, and cross-flow velocity all influence polarization and the other variables shown in Fig. 22-63. [Pg.2035]

Further, as the current density of the fuel cell increases, a point is inevitably reached where the transport of reactants to or products from the surface of the electrode becomes limited by diffusion. A concentration polarization is estabhshed at the elec trode, which diminishes the cell operating potential. The magnitude of this effect depends on many design and operating variables, and its value must be obtained empirically. [Pg.2410]

One should try to remove as much hexane as possible from the n-butyl-llthium solution (i.e. greater than 90%) because the purity of the product depends on the polarity of the reaction medium. A warm water bath was used to facilitate solvent removal. The checkers used a variable pressure oil pump with the vacuum adjusted to ca. 10-20 imi. [Pg.61]

A variable pressure oil pump was used in this distillation. Approximately 10 g of a volatile component, consisting mostly of hexamethyl-disiloxane, was obtained at room temperature (15 (in) before the forerun. The forerun contained the desired product and mineral oil from the n-butyllithium solution. The pot residue was about 5 g. The submitters find the disilyl compound thus obtained is contaminated with a trace amount of mineral oil and 4-6% of a vinylsilane, probably 2-methyl-l-trimethylsiloxy-3-trimethylsilyl-2-propene. This impurity becomes quite significant if the reaction medium is less polar than the one described (e.g., too much hexane from n-butyllithium is allowed to remain behind). The spectral properties of the desired product... [Pg.63]


See other pages where Polarity variables is mentioned: [Pg.556]    [Pg.643]    [Pg.337]    [Pg.65]    [Pg.12]    [Pg.133]    [Pg.247]    [Pg.178]    [Pg.193]    [Pg.824]    [Pg.55]    [Pg.556]    [Pg.643]    [Pg.337]    [Pg.65]    [Pg.12]    [Pg.133]    [Pg.247]    [Pg.178]    [Pg.193]    [Pg.824]    [Pg.55]    [Pg.2]    [Pg.1280]    [Pg.1508]    [Pg.1509]    [Pg.1566]    [Pg.2494]    [Pg.236]    [Pg.127]    [Pg.677]    [Pg.288]    [Pg.70]    [Pg.156]    [Pg.428]    [Pg.107]    [Pg.363]    [Pg.337]    [Pg.2035]    [Pg.2039]    [Pg.2430]   
See also in sourсe #XX -- [ Pg.152 ]




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Variable Amplitude Cross-Polarization

Variable Amplitude Cross-Polarization VACP)

Variable temperature polarizing

Variable temperature polarizing microscopy

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