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We need to point out that, if the wavelengths of laser radiation are less than the size of typical structures on the optical element, the Fresnel model gives a satisfactory approximation for the diffraction of the wave on a flat optical element If we have to work with super-high resolution e-beam generators when the size of a typical structure on the element is less than the wavelengths, in principle, we need to use the Maxwell equations. Now, the calculation of direct problems of diffraction, using the Maxwell equations, are used only in cases when the element has special symmetry (for example circular symmetry). As a rule, the purpose of this calculation in this case is to define the boundary of the Fresnel model approximation. In common cases, the calculation of the diffraction using the Maxwell equation is an extremely complicated problem, even if we use a super computer. [Pg.265]

The measurement and evaluation methods of chapter 3.1. and 3.2. work with inductive sensors in an absolute circuit. The results on two different formed coils, a pot core coil and a cylinder core coil are selected. For presentation in this paper the third method, described in chapter 3.3., uses a Hall-effect device to detect the information and a coil system in a differential circuit to excite the electromagnetic field. [Pg.368]

The obtained signal is filtered with a low-pass filter having the cut-off frequency of 5Hz and a slope of 6 dB/octave. Since we are working with e.m.f modulus, the phase lag does not influence the control. [Pg.377]

Due to the quality, an increasing number of users work with film systems (film, chemistry. [Pg.550]

For such an estimation it is not sufficient to define compliance to the requirements of ISO standards 9000 series. It is necessary to take into account other requirements arising in the process of work with the particular test objects and the customer. [Pg.954]

The Ukrainian Research Institute of Pipes and Metallurgy Automation Research Institute have effective developments in the field of NDT in metallurgy (pipes and rolled stock). Other organisations were experts are working with success in the NDT field are ... [Pg.971]

The film pressure is defined as the difference between the surface tension of the pure fluid and that of the film-covered surface. While any method of surface tension measurement can be used, most of the methods of capillarity are, for one reason or another, ill-suited for work with film-covered surfaces with the principal exceptions of the Wilhelmy slide method (Section II-6) and the pendant drop experiment (Section II-7). Both approaches work very well with fluid films and are capable of measuring low values of pressure with similar precision of 0.01 dyn/cm. In addition, the film balance, considerably updated since Langmuir s design (see Section III-7) is a popular approach to measurement of V. [Pg.114]

A newer and perhaps more useful application of ellipsometry to Langmuir films is their lateral characterization via ellipsometric microscopy [146], A simple modification of the nuU ellipsometer allows one to image features down to 10-/im resolution. Working with a fixed polarizer and analyzer, some domains are at extinction while others are not and appear bright. This approach requires no fluorescent label and can be applied to systems on reflective supports. [Pg.129]

While much early work with dispersed electrochemical systems focused on silver halide sols [16], more recent studies by Rusling and co-workers and others exploited... [Pg.203]

Much of the classic work with boundary lubrication was carried out by Sir William Hardy [44,45]. He showed that boundary lubrication could be explained in terms of adsorbed films of lubricants and proposed that the hydrocarbon surfaces of such films reduced the fields of force between the two parts. [Pg.444]

A thorough reference work with emphasis on the detennination of intemiolecular potentials from experimental data. [Pg.217]

To derive tire boundary condition, it is better to work with the chemical potential instead of the diffiision field. We have... [Pg.747]

It is usually convenient to work with the decadic absorbance. A, defined by... [Pg.1121]

There are cases where the variation of the electtonic ttansition moment with nuclear configuration caimot be neglected. Then it is necessary to work with equation (B 1.1.6) keeping the dependence of on Q and integrating it over the vibrational wavefiinctions. In most such cases it is adequate to use only the tenns up to first-order in equation (B 1.1.7). This results in modified Franck-Condon factors for the vibrational intensities [12]. [Pg.1129]

Unfortimately for modem crystallographers, all of tlie crystal stmctiires that could be solved by the choose-the-best-of-a-small-niunber-of-possibilities procedure had been solved by 1920. Bragg has been quoted as saying that the pyrite stmcture was very complicated , but he wrote, in about 1930, It must be realized, however, that (cases having one or two parameters) are still extremely simple. The more typical crystal may have ten, twenty, or forty parameters, to all of which values must be assigned before the analysis of the stmcture is complete. This statement is read with amusement by a modem crystallographer, who routinely works with hundreds and frequently with thousands of parameters. [Pg.1373]

The available sensitivity depends strongly on the equipment as well as the sample. H is the nucleus of choice for most experiments. 1 mg of a sample of a medium-sized molecule is adequate for almost all types of H-only spectra, and with specialized equipment one can work with nanogram quantities. At this lower level, the... [Pg.1439]

Wlien working with any coordinate system other than Cartesians, it is necessary to transfonn finite displacements between Cartesian and internal coordinates. Transfomiation from Cartesians to internals is seldom a problem as the latter are usually geometrically defined. However, to transfonn a geometry displacement from internal coordinates to Cartesians usually requires the solution of a system of coupled nonlinear equations. These can be solved by iterating the first-order step [47]... [Pg.2347]

Modelling plasma chemical systems is a complex task, because these system are far from thennodynamical equilibrium. A complete model includes the external electric circuit, the various physical volume and surface reactions, the space charges and the internal electric fields, the electron kinetics, the homogeneous chemical reactions in the plasma volume as well as the heterogeneous reactions at the walls or electrodes. These reactions are initiated primarily by the electrons. In most cases, plasma chemical reactors work with a flowing gas so that the flow conditions, laminar or turbulent, must be taken into account. As discussed before, the electron gas is not in thennodynamic equilibrium... [Pg.2810]

The concept of macroscopic kinetics avoids the difficulties of microscopic kinetics [46, 47] This method allows a very compact description of different non-thennal plasma chemical reactors working with continuous gas flows or closed reactor systems. The state of the plasma chemical reaction is investigated, not in the active plasma zone, but... [Pg.2810]

As has been shown previously [243], both sets can be described by eigenvalue equations, but for the set 2 it is more direct to work with projectors Pr taking the values 1 or 0. Let us consider a class of functions/(x), describing the state of the system or a process, such that (for reasons rooted in physics)/(x) should vanish for X D (i.e., for supp/(x) = D, where D can be an arbifiary domain and x represents a set of variables). If Pro(x) is the projector onto the domain D, which equals 1 for x G D and 0 for x D, then all functions having this state property obey an equation of restriction [244] ... [Pg.111]

Under circumstances that this condition holds an ADT matrix, A exists such that the adiabatic electronic set can be transformed to a diabatic one. Working with this diabatic set, at least in some part of the nuclear coordinate space, was the objective aimed at in [72]. [Pg.148]

A related algorithm can be written also for the Brownian trajectory [10]. However, the essential difference between an algorithm for a Brownian trajectory and equation (4) is that the Brownian algorithm is not deterministic. Due to the existence of the random force, we cannot be satisfied with a single trajectory, even with pre-specified coordinates (and velocities, if relevant). It is necessary to generate an ensemble of trajectories (sampled with different values of the random force) to obtain a complete picture. Instead of working with an ensemble of trajectories we prefer to work with the conditional probability. I.e., we ask what is the probability that a trajectory being at... [Pg.266]

Almost all chemical information systems work with tlicir own special type of connection table. They often use various formats distinguishing between internal and external connection tables. In most cases, the internal connection tables arc redundant, thus allowing maximum flexibility and increasing the speed of data processing. The external connection tables are usually non-redundant in order to save disk space. Although a connection table can be cprcsented in many different ways, the core remains the same the list of atoms and the list of bonds. Thus, the conversion of one connection table format into another is usually a fairly straightforward task. [Pg.42]

Nevertheless, there are situations where one wants to work with six four-membered rings in cubane (e.g., when considering the symmetry of the ring system). In this situation, one adds a sixth four-membered ring to obtain firom the SSSR the so-called extended set of smallest rings (ESSR). [Pg.56]

We shall discuss here the methods that have been developed for enabling the computer to perceive both complete chemical structures and fragments of them, as well as their mutual similarity. This is very important in many fields of chemistry, The recognition of flill structures is required routinely in everyday work with large databases. [Pg.291]

The same structure representation as the one taken in the original study [39] is selected in order to show some possibilities evolving from working with a neural network method. Tabic 10.1-1 gives the ten descriptors chosen lor the representation of the 115 molecules of the data set. [Pg.508]

Thus, in the area of combinatorial chemistry, many compounds are produced in short time ranges, and their structures have to be confirmed by analytical methods. A high degree of automation is required, which has fueled the development of software that can predict NMR spectra starting from the chemical structure, and that calculates measures of similarity between simulated and experimental spectra. These tools are obviously also of great importance to chemists working with just a few compounds at a time, using NMR spectroscopy for structure confirmation. [Pg.518]

A number of other software packages are available to predict NMR spectra. The use of large NMR spectral databases is the most popular approach it utilizes assigned chemical structures. In an advanced approach, parameters such as solvent information can be used to refine the accuracy of the prediction. A typical application works with tables of experimental chemical shifts from experimental NMR spectra. Each shift value is assigned to a specific structural fragment. The query structure is dissected into fragments that are compared with the fragments in the database. For each coincidence, the experimental chemical shift from the database is used to compose the final set of chemical shifts for the... [Pg.519]


See other pages where Working with is mentioned: [Pg.190]    [Pg.338]    [Pg.59]    [Pg.293]    [Pg.84]    [Pg.273]    [Pg.472]    [Pg.509]    [Pg.770]    [Pg.790]    [Pg.918]    [Pg.590]    [Pg.688]    [Pg.41]    [Pg.799]    [Pg.1038]    [Pg.1141]    [Pg.1253]    [Pg.1513]    [Pg.1969]    [Pg.2340]    [Pg.424]    [Pg.192]   
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