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Effect spatial

The nonlocal diffuse-layer theory near Eam0 has been developed283 with a somewhat complicated function oLyjind of solvent structural parameters. At low concentrations,/ ) approaches unity, reaching the Gouy-Chapman Qatc- 0. At moderate concentrations, deviations from this law are described by the effective spatial correlation range A of the orientational polarization fluctuations of the solvent. [Pg.55]

Figure 10.47 The 13 Archimedian semiregular solids, constructed from combinations of two or more different two-dimensional figures. Note that, in addition to the triangles, squares and pentagons allowed in the Platonic solids, hexagons, octagons and decagons also make an appearance, but always in conjunction with other shapes. In particular, structure (j) corresponds to buckminsterfullerene, C60, which requires pentagons to effect spatial closure, even though the structure consists predominantly of hexagons. Figure 10.47 The 13 Archimedian semiregular solids, constructed from combinations of two or more different two-dimensional figures. Note that, in addition to the triangles, squares and pentagons allowed in the Platonic solids, hexagons, octagons and decagons also make an appearance, but always in conjunction with other shapes. In particular, structure (j) corresponds to buckminsterfullerene, C60, which requires pentagons to effect spatial closure, even though the structure consists predominantly of hexagons.
In this beam-sweeping scheme the effective spatial distribution of the ions sampled is defined by the characteristics of the sweeping action and the detector slit parameters [20]. Maintaining the fast rise time of the deflection pulse is critical in maintaining spatially small ion packets at the detector surface, and thus adequate resolution. The overall resolution for the differential impulse-sweeping mode in Fig. 12.3 can be estimated with the following equation developed by Bakker [20] ... [Pg.459]

The technique used to (effectively) overcome the VBE is to reduce the effective spatial coherence of the light source used for the development exposure by rotating the sample. Alternatively, the sample could be illuminated simultaneously from many different directions, but it is more convenient to use a moderately collimated beam striking the sample surface at a shallow angle while rotating the sample about an axis perpendicular to that surface. The time constants involved in the polymerization process are typically of the order of minutes, so that rotation rates of the order of 1 rps are usually more than sufficient. [Pg.258]

Patel J.S., Lee Sin-Don and Goodby J. W. Physical Properties of Smectic Liquid Crystals and Novel Electro-optic Effects. Spatial Light Modulator Technology, Materials, Devices, and Applications (Uzi Efron, Marcel Dekker, New York, 1995). [Pg.58]

Certain reactions have distinct stereoelectronic requirements that must be met if the reaction is to proceed efficiently.The effect of conformation on reactivity is conveniently divided into (1) steric effects—close approach of two groups, and (2) stereoelectronic effects—spatial disposition of a particular electron pair, either bonded or nonbonded, as in and E2 reactions. [Pg.47]

The product of the collision frequency 2, the fraction of collisions having the effective spatial orientations p (called the steric factor), and the fraction of collisions having sufficient relative energy (where Ea is the activation energy) gives the rate constant k of a reaction. This relationship is called tire Arrhenius equation ... [Pg.30]

Small-molecule libraries may be created by a variety of methods. These include traditional solution chemistry performed in parallel using multiple reaction vessels so that the individualized chemistry performed in each vessel is, in effect, spatially encoded and hence the structure of the product is implicit by vessel. Alternatively, the chemistry can be performed on a solid support, usually polystyrene beads, in individual vessels, or the supports can be combined into pools where each bead is viewed as a separate reaction vessel. This allows a whole range of design strategies to be employed (vide supra). According to a recent literature survey, two-thirds of reported libraries are prepared on solid support and one-third by solution chemistry. ... [Pg.25]

In the model experiment under consideration, the field is represented by the outgoing and incoming spherical waves of photons, which are specified by a continuous distribution of k or of co = ck. Assume that the two identical atoms are the two-level atoms of the type of (34) with the electric dipole transition. Because of the simple geometry of the problem (Fig. 17), it can be considered as a quasiunidimensional integrable system [69]. The effective spatial dependence of the photon operators can be introduced with the aid of the Fourier transformation... [Pg.472]

The term NAcct> is multiplied by M to account for the difference between the NA on the object side of the microscope objective and the NA on the image side of the microscope objective. The sixth factor which influences the effective numerical aperture is the numerical aperture of microscope objective (NA cro)- These multiple NA terms can be interpreted as multiple low-pass spatial frequency filtering operations of the transverse light amplitude field. The effective spatial frequency is roughly limited by the lowest spatial cutoff frequency or the smallest NA term. Hence, the effective NA (AMeff) of the whole... [Pg.2079]

The diameter of the laser beam used to probe the sample surface typically determines the effective spatial resolution of a measurement performed in microprobe mode. Obviously, the laser beam diameter can be reduced by focusing the beam to smaller dimensions. However, as the laser beam diameter is reduced, it illuminates a smaller area, fewer molecules of each analyte are present within the probe beam, and so fewer molecules are ionized at each location. Therefore, smallest diameter beams are rarely practical because the amount of analyte that can be desorbed and ionized from a smaller sample area is not sufficient for detection and high-accuracy mass measurement. Consequently, the laser probe diameter for the analyses of proteins and peptides usually is larger than 10 xm. [Pg.30]

P. Ewart, P.G.R. Smith, R.G. Williams Imaging of trace species distributions by degenerate four-wave mixing Diffraction effects, spatial resolution, and image referencing. Appl. Opt. 36, 5959 (1997)... [Pg.555]

Improved effective spatial resolution as compared to ordinary light microscopes... [Pg.479]

The concept of the triple quadmpole instrument may be expanded by adding an-otha- RF-only quadmpole and a third mass-analyzing quadmpole to build a QqQqQ instrument. The penta quadmpole represents one of the rare tandem-inspace concepts to achieve MS. A commercial penta quadmpole instmment has once been offered by Extrel, but remained fairly exotic. Nonetheless, the penta quadmpole instmment may serve as a versatile tool for the study of gas phase ion chemistry and in particular ion-molecule reactions [99-102]. For the latter application the effective spatial separation of the zone with neutral reagent from that of preparation of the /n/z-selected precursor ion presents a clear advantage over tandem-in-time concepts. [Pg.438]

Photocatalysis over irradiated semiconductor dispersions provides a method that can lead to a highly effective, spatially controlled oxidation and reduction of organic and... [Pg.579]

The distribution of PAA in model laminates of nanocellulose and PVOH was investigated by FT-IR chemical imaging as can be seen in Figure 15.8. The method was effective spatially in discerning the three components of the composite. However, PAA was found to migrate out of the PVOH matrix and concentrate in the nanocellulose layer of the laminate. This led to a PAA-depleted region in the matrix near the nanocellulose layer, which would likely lead to a weak interphase and limited stress transfer between the fiber and the matrix in the heat-treated composite [24]. [Pg.600]

The exciton binding energy Eio in O Eq. 23.20 for the ground exciton state (n = 1) in commonly used bulk semiconductors is less than 10 meV so that their room temperature luminescence is very weak (exciton thermally dissolved so that n is large). Moreover, exciton Bohr radii, that is, the effective spatial extensions of the excitons, in bulk materials are also quite extended, see O Table 23-2. [Pg.877]


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See also in sourсe #XX -- [ Pg.345 ]




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