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Representations for

The projection of a domain plot onto its base makes a convenient two-dimensional graphical representation for describing adsorption-desorption operations. Here, the domain region that is filled can be indicated by shading the appropriate portion of the 45° base triangle. Indicate the appropriate shading for (a) adsorption up to Xa - 0.8 (b) such adsorption followed by desorption to Xd - 0.5 and (c) followed by readsorption from Xd = 0.5 to Xa = 0.7. [Pg.675]

Smith F T 1962 A symmetric representation for three-body problems. I. Motion in a plane J. Math. Phys. 3 735-48... [Pg.1003]

As well as obtaining tlie scattering amplitude from the above asymptotic boundary conditions, can also be obtained from the integral representation for the scattering amplitude is... [Pg.2044]

Baer M 1975 Adiabatic and diabatic representations for atom-molecule collisions treatment of the collinear arrangement Chem. Rhys. Lett. 35 112... [Pg.2323]

Colbert D T and Miller W H 1992 A novel discrete variable representation for quantum mechanical reactive scattering via the S-matrix Kohn method J. Chem. Phys. 96 1982... [Pg.2326]

Manthe U 1996 A time-dependent discrete variable representation for mulitconfigurational Hartree methods J. Chem. Phys. 105 2646... [Pg.2329]

Henriet A, Masnou-Seeuws F and Dulieu O 1991 Diabatio representation for the exoited states of the NSj... [Pg.2481]

In the further manipulations the site representation will be used for convenience. The Fourier transform with respect to time of a single-exciton retarded Green s function (t) of a system under the Hamiltonian in the site representation for exciton coordinates and Fock s representation for phonon coordinates is written as... [Pg.446]

A major disadvantage of a matrix representation for a molecular graph is that the number of entries increases with the square of the number of atoms in the molecule. What is needed is a representation of a molecular graph where the number of entries increases only as a linear function of the number of atoms in the molecule. Such a representation can be obtained by listing, in tabular form only the atoms and the bonds of a molecular structure. In this case, the indices of the row and column of a matrix entry can be used for identifying an entry. In essence, one has to distinguish each atom and each bond in a molecule. This is achieved by a list of the atoms and a list of the bonds giving the coimections between the atoms. Such a representation is called a connection table (CT). [Pg.40]

In 1971 the Protein Data Bank - PDB [146] (see Section 5.8 for a complete story and description) - was established at Brookhaven National Laboratories - BNL -as an archive for biological macromolccular cr7stal structures. This database moved in 1998 to the Research Collaboratory for Structural Bioinformatics -RCSB. A key component in the creation of such a public archive of information was the development of a method for effreient and uniform capture and curation of the data [147], The result of the effort was the PDB file format [53], which evolved over time through several different and non-uniform versions. Nevertheless, the PDB file format has become the standard representation for exchanging inacromolecular information derived from X-ray diffraction and NMR studies, primarily for proteins and nucleic acids. In 1998 the database was moved to the Research Collaboratory for Structural Bioinformatics - RCSB. [Pg.112]

J.M. Barnard, C.J. Jochum, S.M. Wel-ford, ROSDAL A universal structure/ substmcture representation for PC-host communication, in Chemical Structure Information Systems Interfaces Communication and Standards, WA. Warr (Ed.), ACS Symposium Series No. 400, American Chemical Sodety, Washington, DC, 1989, pp. 76- 81. [Pg.162]

The problem of perception complete structures is related to the problem of their representation, for which the basic requirements are to represent as much as possible the functionality of the structure, to be unique, and to allow the restoration of the structure. Various approaches have been devised to this end. They comprise the use of molecular formulas, molecular weights, trade and/or trivial names, various line notations, registry numbers, constitutional diagrams 2D representations), atom coordinates (2D or 3D representations), topological indices, hash codes, and others (see Chapter 2). [Pg.292]

To make further progress, one needs to evaluate the Rik matrix elements for the partieular orbitals given above and to then use these explieit values in the above equations. The matrix representations for the two e orbitals ean easily be formed and are as follows ... [Pg.271]

We ean likewise write matrix representations for eaeh of the symmetry operations of the C3v point group ... [Pg.584]

We have found three distinet irredueible representations for the C3V symmetry group two different one-dimensional and one two dimensional representations. Are there any more An important theorem of group theory shows that the number of irredueible representations of a group is equal to the number of elasses. Sinee there are three elasses of operation, we have found all the irredueible representations of the C3V point group. There are no more. [Pg.589]

For a function to transform according to a specific irreducible representation means that the function, when operated upon by a point-group symmetry operator, yields a linear combination of the functions that transform according to that irreducible representation. For example, a 2pz orbital (z is the C3 axis of NH3) on the nitrogen atom... [Pg.590]

This set of eharaeters is the same as Dl2) above and agrees with those of the E representation for the C3V point group. Henee, 2px and 2py belong to or transform as the E representation. This is why (x,y) is to the right of the row of eharaeters for the E representation in the C3V eharaeter table. In similar fashion, the C3V eharaeter table states... [Pg.592]

The above representation for the shell energy contains three different terms describing the bending energy of the shell, the deformation energy of the middle surface, and the work done by the exterior force /, respectively. [Pg.139]

It is easy to build an explicit representation for the measure Taking... [Pg.356]

Fig. 2. Schematic representation for the two-film theory of gas transfer = partial pressure of gas Pj = partial pressure of the gas at the interface Cj = concentration of gas at time t, Cj = initial concentration of gas at the interface Cg = initial concentration of gas at t = 0 and S = gas saturation. Fig. 2. Schematic representation for the two-film theory of gas transfer = partial pressure of gas Pj = partial pressure of the gas at the interface Cj = concentration of gas at time t, Cj = initial concentration of gas at the interface Cg = initial concentration of gas at t = 0 and S = gas saturation.
Fig. 7. AT in a feed—effluent exchanger (a) schematic (b) corresponding graphic representation. For example, the optimum AT for a feed—effluent exchanger is computed as follows ... Fig. 7. AT in a feed—effluent exchanger (a) schematic (b) corresponding graphic representation. For example, the optimum AT for a feed—effluent exchanger is computed as follows ...
The boron atoms ia resonance stmctures A and B possess a formal negative charge. The simplest representation for these compounds is... [Pg.264]

The Chemical Abstracts Service has institutionalized the use of graphic representations for identification of and retrieval of information about chemical compounds through their Graphical Data Stmcture (GDS) and connection table (CT). Two information packages. Messenger and STN Express, are the basis for this on-line retrieval system (42). [Pg.63]

Rules are cleady a usehil form of representation for knowledge-based appHcations, with their advantages of representational simplicity, wide apphcabihty, and history of past successes. However, certain important design criteria govern the proper appHcation of rules and there are shortcomings of the rule-based representation. [Pg.534]

In this case, the shear stress is linear in the shear strain. While more physically reasonable, this is not likely to provide a satisfactory representation for the large deformation shear response of many materials either, since most materials may be expected to stiffen with deformation. Note that the hypoelastic equation of grade zero (5.117) is not invariant to the choice of indifferent stress rate, the predicted response for simple shear depending on the choice which is made. [Pg.151]

The early approaches to this model used perturbative expansion for weak coupling [Silbey and Harris 1983]. Generally speaking, perturbation theory allows one to consider a TLS coupled to an arbitrary bath via the term where / is an operator that acts on the bath variables. The equations of motion in the Heisenberg representation for the a operators, 8c/8t = ih [H, d], have the form... [Pg.85]

Schematic representation for the ray paths of both unscattered and scattered electrons beneath the sample. Schematic representation for the ray paths of both unscattered and scattered electrons beneath the sample.
An amino acid having the constitution shown has been isolated from horse chestnuts. It is configurationally related to L-proline and has the R configxuation at C-3. Write a stereochemically correct representation for this compoimd. [Pg.121]

Figure 4.5 Segregation, interception and recycle representation for the AN case study. Figure 4.5 Segregation, interception and recycle representation for the AN case study.

See other pages where Representations for is mentioned: [Pg.362]    [Pg.151]    [Pg.2024]    [Pg.2984]    [Pg.2998]    [Pg.28]    [Pg.568]    [Pg.43]    [Pg.133]    [Pg.613]    [Pg.208]    [Pg.267]    [Pg.364]    [Pg.488]    [Pg.357]    [Pg.519]    [Pg.65]    [Pg.11]    [Pg.83]    [Pg.52]    [Pg.49]   
See also in sourсe #XX -- [ Pg.95 ]

See also in sourсe #XX -- [ Pg.95 ]




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An Integral Representation for Solutions of the Creeping-Flow Equations due to Ladyzhenskaya

Approximate techniques for alternative representations of quantum mechanics

Basis for a representation

Basis for representation

D Descriptors for Spectrum-Like Representation

Eikonal representation for nuclear motions

Elimination for Different Representations of Dirac Matrices

Energy operator for a molecular crystal with fixed molecules in the second-quantization representation. Paulions and Bosons

General formula for the representation of specific heats

Generalization of path-branching representation for arbitrary optical and nonadiabatic transitions

Graphical representation for binary systems

Integral representations for electromagnetic migration field

Inventory Representation For Chemical

Inventory Representation For Chemical Substances

Inventory Representation For Chemical Substances Of Unknown Or Variable

Inventory Representation For Products

Inventory Representation For Products Containing Two Or More Substances

Languages for Knowledge Representation

Mathematical representation for flux balance analysis

Methods for the Representation of Impedance Spectroscopy Data

Multiplication Tables for Character Representations

N representability condition for

Notation for irreducible representations

Nyquist (or Argand) Complex-Plane Plots for Representation of Impedance Behavior

Pictorial Representation of MOs for Molecules

Representation for Problem Analysis

Representation for Problem Solving

Representation theorems for

Representations for Cyclic Groups

Representations for Cyclic and Related Groups

Schematic representation of a reactive flash for an isomerization reaction in the liquid phase

Symmetry representations for wavefunctions

The Foldy Wouthuysen and Dirac representations for a free particle

The GMA representation for a reversible reaction

The General Mass Action (GMA) representation for complex reactions

Toxic Substances Control Act Inventory Representation for Combinations of Two

Tree representation for branch and bound

Warrants for Judgment The Textual Representation of Embodied Sensory Experience

Wave Functions as Bases for Irreducible Representations

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