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X-ray data

The greater the intensity of the X-ray beam that reaches a particular position, [Pg.11]

An optical scanner precisely measures the position and the intensity of each reflection and transmits this information in digital form to a computer for analysis. The position of a reflection can be used to obtain the direction in which that particular beam was diffracted by the crystal. The intensity of a reflection is obtained by measuring the optical absorbance of the spot on the film, giving a measure of the strength of the diffracted beam that produced the spot. The computer program that reconstructs an image of the molecules in the unit cell requires these two parameters, the beam intensity and direction, for each diffracted beam. [Pg.11]

Although film for data collection has largely been replaced by devices that feed diffraction data (positions and intensities of each reflection) directly into computers, I will continue to speak of the data as if collected on film because of the simplicity of that format, and because diffraction patterns are usually published in a form identical to their appearance on film. I will discuss other methods of collecting data in Chapter 4. [Pg.11]


A Real Time X-Ray Inspection System is introduced to replace Film X-Ray. The main objective is to reduce the consumption of film and to reduce the environmental pollution due to lead intensifying screens and chemicals. Other benefits are the reduction of space to storage X-ray data and the shorter inspection time, which gives a faster feed back to production. [Pg.453]

In this paper the technical specifications of a Real Time X-Ray system are given. The procedure for inspection is explained briefly. The resolution of film and of Real Time X-Ray inspection are compared. The basic equipment needed to inspect Real Time X-Ray data is defined. [Pg.453]

The greatest value of molecular dynamic simulations is that they complement and help to explain existing data for designing new experim en ts. Th e sun ulation s are in creasin gly n sefn I for stnictural relinemcnt of models generated from XMR, distance geometry, an d X-ray data. [Pg.10]

The commercially accepted value has been given. Measured values and density calculations from x-ray data show some variations. To convert MPa to psi, multiply by 145. [Pg.378]

Thermal Analyses. Thermal analysis often complements x-ray data in providing information on phase composition. The thermal behavior of aluminum hydroxides is particularly important in filler type appHcations. [Pg.172]

The analysis of siUcon carbide involves identification, chemical analysis, and physical testing. For identification, x-ray diffraction, optical microscopy, and electron microscopy are used (136). Refinement of x-ray data by Rietveld analysis allows more precise deterrnination of polytype levels (137). [Pg.468]

Figure 2 Internal RMSF of residues (average over heavy atoms) determined for human lysozyme by the X-ray normal mode refinement method applied to real X-ray data (heavy curve), m comparison with results from a normal mode analysis on a single isolated lysozyme molecule (lightweight curve). (From Ref. 33.)... Figure 2 Internal RMSF of residues (average over heavy atoms) determined for human lysozyme by the X-ray normal mode refinement method applied to real X-ray data (heavy curve), m comparison with results from a normal mode analysis on a single isolated lysozyme molecule (lightweight curve). (From Ref. 33.)...
X-ray data are recorded either on image plates or by electronic detectors... [Pg.377]

The situation is different for other examples—for example, the peptide hormone glucagon and a small peptide, metallothionein, which binds seven cadmium or zinc atoms. Here large discrepancies were found between the structures determined by x-ray diffraction and NMR methods. The differences in the case of glucagon can be attributed to genuine conformational variability under different experimental conditions, whereas the disagreement in the metallothionein case was later shown to be due to an incorrectly determined x-ray structure. A re-examination of the x-ray data of metallothionein gave a structure very similar to that determined by NMR. [Pg.391]

X-ray structures are determined at different levels of resolution. At low resolution only the shape of the molecule is obtained, whereas at high resolution most atomic positions can be determined to a high degree of accuracy. At medium resolution the fold of the polypeptide chain is usually correctly revealed as well as the approximate positions of the side chains, including those at the active site. The quality of the final three-dimensional model of the protein depends on the resolution of the x-ray data and on the degree of refinement. In a highly refined structure, with an R value less than 0.20 at a resolution around 2.0 A, the estimated errors in atomic positions are around 0.1 A to 0.2 A, provided the amino acid sequence is known. [Pg.392]

X-ray data are recorded either on image plates or by electronic detectors The rules for diffraction are given by Bragg s law Phase determination is the major crystallographic problem Phase information can also be obtained by Multiwavelength Anomalous Diffraction experiments... [Pg.418]

The X-Ray Data Booklet. Lawrence Berkeley Laboratory, Berkeley, is an excellent source of information. [Pg.239]

Study of the structure of cellulose (Figure 22.2) leads one to expect that the molecules would be essentially extended and linear and capable of existing in the crystalline state. This is confirmed by X-ray data which indicate that the cell repeating unit (10.25 A) corresponds to the cellobiose repeating unit of the molecule. [Pg.614]

The CK" ion can act either as a monodentate or bidentate ligand. Because of the similarity of electron density at C and N it is not usually possible to decide from X-ray data whether C or N is the donor atom in monodentate complexes, but in those cases where the matter has been established by neutron diffraction C is always found to be the donor atom (as with CO). Very frequently CK acts as a bridging ligand - CN- as in AgCN, and AuCN (both of which are infinite linear chain polymers), and in Prussian-blue type compounds (p. 1094). The same tendency for a coordinated M CN group to form a further donor-aceeptor bond using the lone-pair of electrons on the N atom is illustrated by the mononuclear BF3 complexes... [Pg.322]

So, back then to aspirin. Very often, X-ray data is available for the molecule of interest or related molecules. The lingua franca for molecular modelling purposes is a file of Cartesian coordinates such as the following. pdb (Protein Database) file. Figure 1.13, for aspirin. [Pg.46]

Mono saponification of diethyl 3,4-dihydroxythiophene-2,5-dicarbox-ylate 96 (67T2437) (1 N NaOH, then HCl) results in the formation of 97 (28%) as a white solid. According to and X-ray data, this compound... [Pg.112]

According to X-ray data, 2,5-diamino-l,3,4-triazole retains its diamino form in the heterovalent cobalt complex 375 (91IC4858) and in the polymeric complex with manganese thiocyanate (93ICA53). [Pg.291]

For pyra20l-3-ones die following spectral and X-ray data are available. [Pg.139]

Semiempirical PM 3 MO calculations were performed on eight 4-aryl-2,3,5,6,7,8-hexahydro-l//-pyrido[l,2-c]pyrimidin-l,3-diones and on their dimers (00JPO213). In all of the calculated structures the aromatic ring is almost perpendicular to the plane of the pyrido[l,2-c]pyrimidin-l,3-dione fragment, which is in accordance with the X-ray data for 4-(4-methylphenyl) derivative. [Pg.247]

In general, X-ray data are used in conjunction with other techniques to obtain as full a picture as possible. For liquid-crystalline materials, differential scanning calorimetry (DSC) and polarizing optical microscopy (POM) are conventionally used. [Pg.139]

Figure 2. Thermal strain vs temperature curves for VsSi measured along [001] on heating (4.2-60K) and cooling (4.2-1.5K). Curve (a) is for an uniaxial stress (s 0.03o doo)) along [001] (b) and (c) are for biaxial stress applied along [100] and [010] with 0.5o (ioo> and o (ioo>, respectively. The x-ray data of Batterman and Barrett (reference 15) are also plotted for comparison. The insets show the directions of applied stresses and [in case of the curve (a)] the martensite-phase domains. (From reference 5)... Figure 2. Thermal strain vs temperature curves for VsSi measured along [001] on heating (4.2-60K) and cooling (4.2-1.5K). Curve (a) is for an uniaxial stress (s 0.03o doo)) along [001] (b) and (c) are for biaxial stress applied along [100] and [010] with 0.5o (ioo> and o (ioo>, respectively. The x-ray data of Batterman and Barrett (reference 15) are also plotted for comparison. The insets show the directions of applied stresses and [in case of the curve (a)] the martensite-phase domains. (From reference 5)...

See other pages where X-ray data is mentioned: [Pg.24]    [Pg.399]    [Pg.1167]    [Pg.167]    [Pg.288]    [Pg.542]    [Pg.546]    [Pg.206]    [Pg.539]    [Pg.199]    [Pg.12]    [Pg.18]    [Pg.3]    [Pg.377]    [Pg.1167]    [Pg.164]    [Pg.290]    [Pg.1177]    [Pg.69]    [Pg.150]    [Pg.140]    [Pg.51]    [Pg.207]    [Pg.137]    [Pg.435]    [Pg.78]   
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See also in sourсe #XX -- [ Pg.214 , Pg.216 ]

See also in sourсe #XX -- [ Pg.97 ]

See also in sourсe #XX -- [ Pg.182 ]

See also in sourсe #XX -- [ Pg.142 ]




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