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Methods model

Computer graphics has had a dramatic impact upon molecular modelling. It should always be remembered, however, that there is much more to molecular modelling than computer graphics. It is the interaction between molecular graphics and the imderlying theoretical methods that has enhanced the accessibility of molecular modelling methods and assisted the analysis and interpretation of such calculations. [Pg.25]

Most of the modeling methods discussed in this text model gas-phase molecular behavior, in which it is reasonable to assume that there is no interaction with other molecules. However, most laboratory chemistry is done in solution where the interaction between the species of interest and the solvent is not negligible. [Pg.206]

PRISM (polymer reference interaction-site model) method for modeling homopolymer melts... [Pg.367]

SACM (statistical adiabatic channel model) method for computing reaction rates... [Pg.368]

Structure Generation, QSAR, and GoMFA Modeling Methods. [Pg.167]

Quantitative Structure—Activity Relationships (QSAR). Quantitative Stmcture—Activity Relationships (QSAR) is the name given to a broad spectmm of modeling methods which attempt to relate the biological activities of molecules to specific stmctural features, and do so in a quantitative manner (see Enzyme INHIBITORS). The method has been extensively appHed. The concepts involved in QSAR studies and a brief overview of the methodology and appHcations are given here. [Pg.168]

Approximate prediction of flow pattern may be quickly done using flow pattern maps, an example of which is shown in Fig. 6-2.5 (Baker, Oil Gas]., 53[12], 185-190, 192-195 [1954]). The Baker chart remains widely used however, for critical calculations the mechanistic model methods referenced previously are generally preferred for their greater accuracy, especially for large pipe diameters and fluids with ysical properties different from air/water at atmospheric pressure. In the chart. [Pg.652]

For pressure drop and holdup in inclined pipe with upward or downward flow, see Beggs and Brill ]. Pet. Technol, 25, 607-617 [1973]) the mechanistic model methods referenced above may also be apphed to inchned pipes. Up to 10° from horizontal, upward pipe inclination has httle effecl on holdup (Gregory, Can. J. Chem. Eng., 53, 384-388 [1975]). [Pg.654]

In an isolated two-spin system, the NOE (or, more accurately, the slope of its buildup) depends simply on where d is the distance between two protons. The difficulties in the interpretation of the NOE originate in deviations from this simple distance dependence of the NOE buildup (due to spin diffusion caused by other nearby protons, and internal dynamics) and from possible ambiguities in its assignment to a specific proton pair. Mofec-ufar modeling methods to deaf with these difficulties are discussed further below. [Pg.255]

All current comparative modeling methods consist of four sequential steps (Fig. 2) [5,6]. The first step is to identify the proteins with known 3D structures that are related to the target sequence. The second step is to align them with the target sequence and pick those known structures that will be used as templates. The third step is to build the model... [Pg.275]

There are two main classes of loop modeling methods (1) the database search approaches, where a segment that fits on the anchor core regions is found in a database of all known protein structures [62,94], and (2) the conformational search approaches [95-97]. There are also methods that combine these two approaches [92,98,99]. [Pg.285]

This section briefly reviews prediction of the native structure of a protein from its sequence of amino acid residues alone. These methods can be contrasted to the threading methods for fold assignment [Section II.A] [39-47,147], which detect remote relationships between sequences and folds of known structure, and to comparative modeling methods discussed in this review, which build a complete all-atom 3D model based on a related known structure. The methods for ab initio prediction include those that focus on the broad physical principles of the folding process [148-152] and the methods that focus on predicting the actual native structures of specific proteins [44,153,154,240]. The former frequently rely on extremely simplified generic models of proteins, generally do not aim to predict native structures of specific proteins, and are not reviewed here. [Pg.289]

J Greer. Comparative modelling methods Application to the family of the mammalian serine proteases. Proteins 7 317-334, 1990. [Pg.301]

L Jaroszewski, L Rychlewski, B Zhang, A Godzik. Fold prediction by a hierarchy of sequence, threading, and modeling methods. Protein Sci 6 1431-1440, 1998. [Pg.303]

Evbuomwan, N. F. O., Sivaloganathan, S. and Webb, J. 1996 A Survey of Design Philosophies, Models, Methods and Systems. Proc. Instn Mech. Engrs, Part B, 210(B4), 301-320. [Pg.385]

The engineer is offered a large variety of flow-modeling methods, whose complexity ranges from simple order-of-magnitude analysis to direct numerical simulation. Up to now, the methods of choice have ordinarily been experimental and semi-theoretical, such as cold flow simulations and tracer studies. [Pg.812]

Depending on the purpose of the computer calculations, different tools are selected. The modeling methods described in this chapter and their pri maty application are listed in Table 11.1. [Pg.1028]

Which model is preferred depends on the final information needed. If the interest is in the magnitude of air velocity that is to be found, the discrete modeling method is certainly better. [Pg.1052]

At present, trial-and-error proeedures of experimental sereening are usually employed. Leusen etal. (1993) hypothesized that separability eorrelates with the differenee in the internal or lattiee energy of the two diastereomer adduets and the extent to whieh moleeular modelling methods may be applied to estimate sueh energy differenees. [Pg.6]

For these and other purposes, blast-modeling methods are needed in order to quantify the potential explosive power of the fuel present in a particular setting. The potential explosive power of a vapor cloud can be expressed as an equivalent explosive charge whose blast characteristics, that is, the distribution of the blast-wave properties in the environment of the charge, are known. [Pg.112]

Ligand recognition in the opioid receptors by modeling methods and design of opioids 98YZ1. [Pg.226]

In the second section we present a brief overview of some currently used dynamic modeling methods before introducing cellular automata. After a brief history of this method we describe the ingredients that drive the dynamics exhibited by cellular automata. These include the platform on which cellular automata plays out its modeling, the state variables that define the ingredients, and the rules of movement that develop the dynamics. Each step in this section is accompanied by computer simulation programs carried on the CD in the back of the book. [Pg.181]

The mathematical aspects of the model (mathematieal model). Methods and approximations used to study the seleeted physieal interaetions in the given material model. [Pg.4]

Thermal methods in kinetic modelling. Methods for the estimation of thermokinetic parameters based on experiments in a reaction calorimeter will be discussed below. As mentioned in section 5.4.4.3, instantaneous heat evolved due to a single reaction is directly proportional to the reaction rate. Assume that the reaction is of first order. Then for isothermal operation ... [Pg.320]

Suzuki, T., Kudo, Y. Automated logP estimation based on combined additive modeling methods. J. Comput.-Aided Mol. Des. 1990, 4,155-198. [Pg.377]


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See also in sourсe #XX -- [ Pg.397 ]




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