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Standard representations

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]

For the case of the particle at rest the solutions (9-309) are also eigensolutions of the operator S3. In the standard representation, the representation (9-304) indicates that these two solutions correspond to two different possible orientations of the spin of the particle. However, 2 and H do not commute in general, i.e., when p 0. A more... [Pg.528]

In the standard representation, where A — y°, this requirement becomes... [Pg.533]

Using the standard representation of the Dirac matrices (3 and , the residual P,T-odd interaction operator can be written... [Pg.251]

In Tabel 10-5, we present the standard representation of this breakdown of the data. There are two important points to note about the results in this table first the data,... [Pg.65]

Thus TFD is nothing but a simple example of the standard representation of a w -algebra. [Pg.203]

CRYSTAL STRUCTURE OF THE SOLID PHASE AND ITS STANDARD REPRESENTATION... [Pg.94]

The coordinates indicated in the reported partial list of invariant lattice complexes correspond to the so-called standard setting and to related standard representations. Some of the non-standard settings of an invariant lattice complex may be described by a shifting vector, defined in terms of fractional coordinates, in front of the symbol. The most common shifting vectors also have abbreviated symbols P represents 14, A,AP (that is the coordinates which are obtained by adding A, Vi, Ai to those of P, that is coordinates 14, 14, A), J represents A, A, A J (coordinates A, 0, 0 0, A, 0 0, 0, A) F" represents A,A,AF (coordinates At, A, A A, 3A, A 3A, A, 3A 3A, A, A) and F" represents A, /, 3A F. It can be seen, moreover, that the complex D corresponds to the coordinates F + F". [Pg.118]

The standard representation of a chemical reaction shows an arrow pointing from the reactants to the products ... [Pg.24]

The Pauli form factor also generates a small contribution to the Lamb shift. This form factor does not produce any contribution if one neglects the lower components of the unperturbed wave functions, since the respective matrix element is identically zero between the upper components in the standard representation for the Dirac matrices which we use everywhere. Taking into account lower components in the nonrelativistic approximation we easily obtain an explicit expression for the respective perturbation... [Pg.25]

Similar behavior of a certain physical property common to different material systems can only be visualized by dimensionless representation of the material function of that property (here the viscosity l). It is furthermore desirable to formulate this function as uniformly as possible. This can be achieved by the standard representation (6,11) of the material function in which a standardized transformation of the material function /i(7) is defined in such a way that the expression produced meets the requirement... [Pg.24]

Figure 6 shows the dependency ijl T) for eight different liquids with greatly different temperature coefficients of the viscosity, whose viscosities cover six decades within the range of T= 20-80°C. Figure 7 depicts the standard representation of this behavior. Surprisingly this proves that all these liquids behave similarly in the /r(I) respect. In addition, it proves that this standard representation is invariant to reference temperature. Water is a special juice it behaves like the other liquids only in the vicinity of the standardization range yo(2 —To) 0. [Pg.24]

The type of dimensionless representation of the material function affects the (extended) pi set within which the process relationship is formulated (for more information, see Ref. 11). When the standard representation is... [Pg.24]

Figure 7 Standard representation of the dependency ju(T) for these liquids. The fitting curve presents the reference-invariant function x after Pawlowski. The numerical value of the parameter of this function is —1.2 for water and —0.167 for other fiuids. Logarithmic variation is 5.25 x 10 for water and 1.51 x 10 for other fiuids. Source From Ref. 11, Chapter 8.2. Figure 7 Standard representation of the dependency ju(T) for these liquids. The fitting curve presents the reference-invariant function x after Pawlowski. The numerical value of the parameter of this function is —1.2 for water and —0.167 for other fiuids. Logarithmic variation is 5.25 x 10 for water and 1.51 x 10 for other fiuids. Source From Ref. 11, Chapter 8.2.
To examine the similarity in particle strength of these materials, a standard representation of this physical property must be calculated. Figure 21 shows it in the pi space... [Pg.45]

Figure 21 Standard representation of particle strength of various solids as function of particle size. Source From Ref. 23. Figure 21 Standard representation of particle strength of various solids as function of particle size. Source From Ref. 23.
Zlokarnik M. Standard representation of the particle strength of various solids in dependency on the particle diameter (in German). Chem Ing Tech 2004 76 1110-1111. [Pg.54]

In the language of perturbation theory, the two orbitals will constitute the unperturbed system, the perturbation is the interaction between them, and the result of the interaction is what we wish to determine. The situation is displayed in Figure 3.1a. The diagram shown in Figure 3.1 b conveys the same information in the standard representations of PMO or orbital interaction theory. The two interacting but unperturbed systems are shown on the left and the right, and the system after the interaction is turned on is displayed between them. Our task is to find out what the system looks like after the interaction. Fet us start with the two unperturbed orbitals and seek the best MOs that can be constructed from them. Thus,... [Pg.36]

Figuie 4A shows the dependency p(T) for four different liquids, and Figure 4B depicts the standard representation of this behavior. This confirms that propene, toluene, and CCI4 behave similarly with regard to p(T), whereas water behaves differently. This implies that water cannot be used in model experiments if one of the other three liquids will be employed in the industrial plant. [Pg.24]

The type of dimensionless representation of the material function affects the (extended) pi set within which the process relationship is formulated (for more information see Ref. 5). When the standard representation is used, the relevance list must include the reference density po instead of p and incorporate two additional parameters po. Tq. This leads to two additional dimensionless numbers in the process characteristics. With regard to the heat transfer characteristics of a mixing vessel or a smooth straight pipe, Eq. (27), it now follows that... [Pg.24]

For this reason, the n-dimensional vector space 72Dwith this scalar product is referred to as the standard representation of n-dimensional vector spaces. [Pg.4]

One concludes that all n-dimensional vector spaces are in fact the same abstract space, with the familiar standard representation TV1. Extension to the enumerably infinite spaces with representation 72.00 is straightforward. [Pg.5]

In a standard representation of the SharpUss dihydroxylation, the largest group is shown at the bottom left The chiral reagent used here then attacks preferentially from above... [Pg.34]

The following operators were used in Chapter 7 as representative operators of the five classes of the cubic point group O E, R(2n/3 [1 1 1]), R(n/2 z), R(n z), R(n [1 1 0]). Derive the standard representation for these operators and show that this representation is irreducible. [Hint You may check your results by referring to the tables given by Altmann and Herzig (1994) or Onadera and Okasaki (1966).]... [Pg.251]


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Dirac standard representation

Genetic standard representation

Standard boundary representation

Standard representations temperature dependence

Standard representations viscosity

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