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Atomic symbol array

This hypothesis has been sometimes put forward, but, for the time being, real proof of individual existence of such valence isomers is still lacking. Although we cannot exclude the possibility that future refinements of experimental techniques may eventually prove the existence of such isomers, it does not seem advisable to accept as a fact the existence of isomers for which no conclusive evidence has ever been produced. We shall then prefer the single bond-no bond resonance theory to the rapid isomerization theory. In so doing we admit that there exists, in trithiapentalenes, an array of atoms which can be represented as in 85, in which the lines between atomic symbols mean only that some sort of bonding exists, without prejudice of the nature of this bonding. [Pg.209]

Your worksheet should look like the one shown in Figure 3-13, with the molar mass of fluorine displayed in cell 12. Excel has looked up the atomic mass of fluorine (specified by its symbol F as the Iookup value) in the rectangular region of the worksheet specified by the variable table array, which in this example is B2 F114. This region, or array, contains the atomic symbols in the first column of the array (column B in the worksheet) and the extracted atomic masses in the fifth... [Pg.66]

Each row in the coordtest table represents a molecule. The smiles column is a string of atom symbols and bonds and the coord column is an array of atom coordinates. How is it possible to keep the ordering of atoms in the smiles string in sync with the ordering of atom coordinates in the coord array When the coordinates are initially entered from the external source, they are likely to be in a common chemical file format. The program that converts from that file format to SMILES would have to output the atom coordinates in the same order as the atoms in the SMILES. [Pg.116]

These functions are called with a string argument. This argument is an SQL statement that is expected to provide the required information. For ctable, this is an array of bonds. For symbol coords, these are an array of symbols and an array of coordinates for each atom. [Pg.174]

A four-subscript matrix can be imagined as a four-dimensional array of symbols a six-subscript matrix can be imagined as a six-dimensional array, and so on these arrays are the periodic system (Hefferlin and Kuhlman 1980 Hefferlin 1989a, Chapter 10). In general, the outer product is taken N — 1 times to create the 2/V-dirncnsional periodic system for N atomic molecules. [Pg.233]

The suggested nomenclature that is most nearly complete is then as follows. The name of the substrate surface is followed by the Park-Madden symbol, which is then followed by the name of the adsorbate, and last by the coverage of adsorbate in square brackets. Thus the complete names for the oxygen structures on Ni(llO) shown in Fig. 8 read Ni(110)-( )-O-[i], Ni(110)-( )-O-[J], and Ni(110)-( )-O-[f]. In these arrays of symbols, 0 refers to oxygen atoms and the final fractions in square brackets to fractions of a monolayer. One monolayer is defined as the number of atoms in a single plane of the substrate. When the unit mesh vectors dg and 5g are, respectively, parallel to d and 5, the shorthand Lander notation is convenient. Thus the three structures of Fig. 8 can also be called (3 X 1), (2 x 1), and (3 X 1), respectively, where the first number in each set of brackets refers to the magnitude of dg in units of a, and the second to the magnitude of 5g in units of 6. When a centered mesh is chosen, the symbol C is written prior to the shorthand symbol. Thus the structure of Fig. 28a (p. 223) is written (2 X 2) and that of Fig. 28b, C(2 X 2). [Pg.176]

Compounds arise from the combination of atoms in fixed ratios. In any such combination, the resultant substance behaves differently from the atoms alone. In many compounds, atoms combine to form discrete particles called molecules. Molecules can be broken down into their constituent atoms, but the resulting collection of atoms no longer behaves like the original molecule. Other materials are composed of vast arrays or extended structures of atoms or ions but do not form discrete molecules. Alloys, metals, and ionic solids (composed of paired ions) fall into this category of chemical compounds. We ve seen how we can use atomic symbols as shorthand notation to designate atoms. That same idea can be extended to describe the composition of either molecules or extended compounds in a simple symbolic representation. [Pg.49]

The table uses a system of symbols for the elements and a system of conventions for atomic weights it employs a classification, or a visual array, that groups the symbols so that their relations and properties are immediately suggested to the viewer who knows the principles of classification and a few facts. Deductions can be made both to the facts that established the table and to the facts that were unknown when the table was first set out. Here is a scheme that is an explanatory and predictive model and an icon in both the semiotic and the popular senses of the word. But its power comes from visual display, from image, not the principles and facts that can be recorded in ordinary or conventional language. [Pg.108]

It is now possible to specify the possible configurations or occupation states for each representation, as shown in Table I. A filled circle indicates a site occupied by an adsorbed atom. The symbol to the right of each figure represents the fraction of all members in each array in the specified configuration. The... [Pg.244]

List Processing (LISP) is a programming language that uses an interpreter for symbolic calculations based on single-scalar values (atoms) and associative arrays (lists). [Pg.58]

Although SMILES is an entirely equivalent way of storing a connection table of atoms and bonds, it is sometimes desirable to create a traditional connection table, for example, when an external program requires it. The extension functions smiles to symbols and smiles to bonds accept a SMILES string and produce an array of either symbols or bonds. These are discussed in a later section of this chapter. Several implementations of these functions are shown in the Appendix. [Pg.125]

In a molecular structure file, an atom record typically contains all of the information about that atom the atomic number or symbol, the charge, coordinates, etc. When such a file is parsed into a SMILES string and an array of coordinates, it is important to be able to associate the proper coordinate with the proper atom. The use of canonical SMILES ensures this. Because canonical SMILES defines a unique order of the atoms in a molecule, that order is used to store the coordinates. Later sections of this chapter will discuss ways in which atomic coordinates might be stored in columns of a table. [Pg.125]

The periodic table is a tabular array of the elements that lists them horizontally in order of increasing atomic number. Each element is represented by its symbol, and its atomic number is written above the symbol. The importance of the atomic number will be discussed in Chapter 3. In addition, the periodic table is organized so that elements with similar chemical properties are aligned in columns. This kind of organization makes the periodic table a valuable tool. If you know the chemical properties of one element, then it is reasonable to assume that the other elements in the same column will have similar properties. For this and many other reasons, the periodic table is the single most useful tool in chemistry. The modern periodic table is shown in the following figure. [Pg.44]

Schematic showing several of the basic forms of magnetism. The arrow representsan individual magnetic moment on an atom or a molecule, and the arrays are meant to symbolize three-dimensional packing of the individual moments. Schematic showing several of the basic forms of magnetism. The arrow representsan individual magnetic moment on an atom or a molecule, and the arrays are meant to symbolize three-dimensional packing of the individual moments.
We have already covered the symmetry elements that apply to individual molecules (in the Schoenflies notation) in Section 2.3.1, and you should read this section now if you have not already done so. We now need to consider the symmetry operations that map the relationships between entire arrays of atoms or molecules in three dimensions. These are generally expressed using the Herman-Mauguin symbols, in which the inversion operation, i, is replaced by 1, the reflection, [Pg.324]

There are precisely 14 different topological ways of arranging equivalent points in an atomic array and this gives rise to the 14 Bravais lattices or space lattices, as it was Auguste Bravais in 1848 who first rigorously established that other suggested lattices were in fact identical to one of his own 14. These lattices are named by their crystal system followed by a symbol P, /, F, C or / always italicized) as indicated in Fig. 7 [1]. [Pg.382]

Note. The Hermann-Mauguin space group notation for any particular crystal comprises two parts. The first part identifies the Bravais lattice type into which the crystal belongs and the second part identifies the total symmetry of the array of atoms in the crystal and therefore also the crystal system. In the second part that identifies the symmetry, only those symmetry elements are included in the symbol that are necessary to describe the space group uniquely. The remainders are being omitted since they follow, as a necessary consequence. [Pg.40]

Figure 11.16. Examples of grain boundaries between cubic crystals for which the projection along one of the crystal axes, z, produces a 2D square lattice. Left asymmetric tilt boundary at 0 =45° between two grains of a square lattice. Right symmetric tilt boundary at 0 = 28° between two grains of a square lattice. Four different sites are identified along the boundary, labeled A, B, C, D, which are repeated along the grain boundary periodically the atoms at each of those sites have different coordination. This grain boundary is equivalent to a periodic array of edge dislocations, indicated by the T symbols. Figure 11.16. Examples of grain boundaries between cubic crystals for which the projection along one of the crystal axes, z, produces a 2D square lattice. Left asymmetric tilt boundary at 0 =45° between two grains of a square lattice. Right symmetric tilt boundary at 0 = 28° between two grains of a square lattice. Four different sites are identified along the boundary, labeled A, B, C, D, which are repeated along the grain boundary periodically the atoms at each of those sites have different coordination. This grain boundary is equivalent to a periodic array of edge dislocations, indicated by the T symbols.

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See also in sourсe #XX -- [ Pg.174 ]




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