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Intermediate observation distances

Another kind of cell, made by Graham and Curran, was based on an internal reflection crystal [80]. A gold minigrid was mounted directly on a prism (9 x 9 x 45 mm) and on top of this was a zinc selenide prism. The distance (observation) between the minigrid and the prism is typically 13-15 pm, which results in a very short response time. For a potential-step experiment, maximum absorbance is achieved within a couple of seconds. The cell is especially well-suited for potential-scan experiments because the intermediate generated at the electrode will rapidly fill out most of the observation distance even when moderately fast sweep rates (50 mV s ) are applied. Some memory effect is, however, present, because the diffusion layer will not be completely evolved on this timescale. At smaller sweep rates (2 mV s ) all of the observation layer behaves like a thin layer, where the concentrations are in equilibrium with the electrode surface concentrations. The cell has been used to study the reduction process of Fe(CO)s by CV, where it was pos-... [Pg.564]

Fig. 22.12 is the graphical representation of the results obtained using the different versions of SS-MRCEPA. At shorter distances the performance of SS-MRCEPA(O) and the approximate SS-MRCEPA(I) are very close to one another, whereas, for larger separations R > 7.0 a.u.) the results of CEPA(I) are very close to the FCI as compared to CEPA(O). At intermediate internuclear distances, the SS-MRCEPA(O) performs better than the corresponding CEPA(I) approach. Akin to our observation for LiH, the approximate SS-MRCEPA(I) in the relaxed and frozen contexts show almost identical behaviour as is evident from Fig. 22.12. At shorter interatomic separations the frozen... Fig. 22.12 is the graphical representation of the results obtained using the different versions of SS-MRCEPA. At shorter distances the performance of SS-MRCEPA(O) and the approximate SS-MRCEPA(I) are very close to one another, whereas, for larger separations R > 7.0 a.u.) the results of CEPA(I) are very close to the FCI as compared to CEPA(O). At intermediate internuclear distances, the SS-MRCEPA(O) performs better than the corresponding CEPA(I) approach. Akin to our observation for LiH, the approximate SS-MRCEPA(I) in the relaxed and frozen contexts show almost identical behaviour as is evident from Fig. 22.12. At shorter interatomic separations the frozen...
The description of both water-metal and ion-metal interactions by purely local potentials derived from ab initio SCF calculations leads to contact adsorption of the ion on Pt(lOO). The observed distance spectrum of Li+ is intermediate between that expected for specific and non-specific adsorption. [Pg.53]

If the analogies of table 1 were complete and comprised both theories then the analysis of the small cable net shown in table 2 - the net consists of two high and two low fixpoints and 8 intermediate nodes in space - should be transferable to the adjustment of a trilateration in space. Judging only very elementary we see, however, immediately that in the analogue trilateration problem we have 8 3=24 unknown coordinatecomponents and only 17 observed distances in space. Speaking in the terms of adjustment theory the problem has no redundancy, even more, it is underdetermined, and for this the classical theory offers no solution. [Pg.59]

Because the carbons that are singly bonded m one resonance form are doubly bonded m the other the resonance description is consistent with the observed carbon-carbon bond distances m benzene These distances not only are all identical but also are intermediate between typical single bond and double bond lengths... [Pg.427]

Where pipelines and high-voltage cables cross, a distance of at least 0.2 m must be observed to prevent contact between cable and pipeline (this can be achieved by interposing insulating shells or plates). Such intermediate materials can be PVC or PE. Their disposition and shape must be determined by mutual agreement [2,6]. [Pg.508]

One of the complicating factors in the use of a TNT-blast model for vapor cloud explosion blast modeling is the effect of distance on the TNT equivalency observed in actual incidents. Properly speaking, TNT blast characteristics do not correspond with gas explosion blast. That is, far-field gas explosion blast effects must be represented by much heavier TNT charges than intermediate distances. [Pg.121]

Alloys of lead and thallium have a structure based upon cubic closest packing from 0 to about 87-5 atomic percent thallium. The variation of the lattice constant with composition gives strong indication that ordered structures PbTl, and PbTl, exist. In the intermediate ranges, solid solutions of the types Pb(Pb,Tl)a and Pb(Pb,Tl)TlB exist. Interpretation of interatomic distances indicates that thallium atoms present in low concentration in lead assume the same valence as lead, about 2-14, and that the valence of thallium increases with increase in the mole fraction of thallium present, having the same value, about 2-50, in PbTls and PbTl, as in pure thallium. A theory of the structure of the alloys is presented which explains the observed phase diagram,... [Pg.591]

Si4 revealed a distorted tetrahedral configuration, and the Sil-Si2 and Si2-Si3 bond distances of 2.240(2) and 2.244(2) A were intermediate between the Si=Si and Si-Si bond lengths of the precursor 19. This was explained by the delocalization of the positive charge over the Sil, Si2, and Si3 atoms, accompanied by the Sil-Si3 through-space orbital interaction, resulting in the overall homoaromaticity of 20. The hypothesis of homoaromaticity was further supported by the observation of an extremely low-field shifted signal of Si2, the central atom of the Sis homoaromatic system, at 315.7 ppm. [Pg.64]


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See also in sourсe #XX -- [ Pg.344 ]




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