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Matrix experimental procedures

The role of yeast in fermenting dough maturation is even less clear. The alcohol and carbon dioxide developed during fermentation must influence the elastic properties of the protein matrix. However, experimental procedures that would permit this to be checked in the absence of yeast have not been developed. [Pg.390]

Matrix available in pure form. Known euiounts of substance added to matrix and determined by the same experimental procedure as samples. [Pg.925]

Wang et al. also addressed the mass spectral reproducibility. They conducted a carefully controlled interlaboratory experiment where the effects of a number of parameters were systematically investigated.22 They demonstrated that nearly identical spectra could be obtained in carefully controlled experiments. Minor variations in the sample/matrix preparation procedures for MALDI and in the experimental conditions used for bacterial protein extraction or analysis were shown to result in changes in the resulting spectra. They also noted that a subset of peaks was less sensitive to experimental variables. These ions appeared to be conserved in spectra obtained even under different experimental conditions so long as they were obtained using genetically identical bacteria. The existence of these conserved peaks helped explain... [Pg.132]

This book encompasses indiscriminately all the types of reductions and superimposes them over a matrix of types of compounds to be reduced. The manner of arrangement of the compounds is a somewhat modified Beilstein system and is explained in the introduction. Numerous tables summarize reducing agents and correlate them with the starting compounds and products of the reductions. Reaction conditions and yields of reductions are mentioned briefly in the text and demonstrated in 175 examples of reductions of simple types of compounds and in 50 experimental procedures. [Pg.319]

Observed agreement between the experimental and model cross-relaxation rates within the estimated error limits confirms validity of the full matrix analysis procedure but not necessarily its usefulness. Namely, the agreement is achieved mainly within the broad limits of cross-relaxation rate errors. Errors span the range 0.25 to 0.62 s but are clustered around the values 0.35 s and 0.55 s All the errors involving cross-relaxation rates of ProH and GlyH are clustered around 0.35 s . This is mainly because... [Pg.296]

Microwave spectrometer, 219-221 Microwave spectroscopy, 130, 219-231 compilations of results of, 231 dipole-moment measurements in, 225 experimental procedures in, 219-221 frequency measurements in, 220 and molecular structure, 221-225 and rotational barriers, 226-228 and vibrational frequencies, 225-226 Mid infrared, 261 MINDO method, 71,76 and force constants, 245 and ionization potentials, 318-319 Minimal basis set, 65 Minor, 14 Modal matrix, 106 Molecular orbitals for diatomics, 58 and group theory, 418-427 for polyatomics, 66... [Pg.247]

The simplest ligand is N2 itself. Using matrix isolation techniques the IR spectra of Pt(N2) (n = 1, 2, 3) show v(N=N) in the range 2170.0-2211.5 cm-1 and v(Pt—N) in the range 360-394 cm-1. By using isotopically labeled N2, accurate force constants have been calculated.917 Using a similar experimental procedure, the compounds Pt(02)(N2) ( = 1, 2) have been observed in a cooled matrix by IR spectroscopy.918... [Pg.422]

Prepare influence matrix Establish experimental procedures Establish design criteria Prepare study plan and protocols... [Pg.52]

Three additional experiments were carried out at 30°C using only 5 mL of terf-butyl hydroperoxide (70% solution in water, 36.4 mmol) instead of 8 mL. The reaction data collected from all six experiments at 30°C were then concatenated to a second Aoata matrix and a second qDaU vector. The experimental procedure is described in further detail elsewhere [20]. [Pg.217]

The general statement that connects quantum theory to experimental observations such as optical activity can be put as follows. We subject the material medium to some experimental procedure using a probe light beam, and observe a certain outcome after the probe has passed through the system, for example by analysing the scattered light. If we define the density matrix tot for the combined system of material medium + probe, and characterize the measurement by some operator, then the probability that the specified outcome of the measurement is observed, is given by,... [Pg.15]

The operational characteristics such as depth resolution, maximum accessible depth and minimum detection limit in ERD are highly subjective to each experiment condition. In our system with the conditions described in the experimental procedures section and assuming Si as the primary matrix for the target, the typical performance characteristics in routine applications are 80-100 A depth resolution, 1 pm maximum depth and about 0.1 at.% minimum detection limit. For more discussion of operation characteristics one may refer to our earlier work (2). [Pg.108]

Quantitative y-ray spectrum analysis of environmental samples such as soil, water or ash of food requires the peak efficiency for volume sample. A Marinelli beaker is often used as a container for a large quantity of sample such as water or soil. As the volume of sample to be measured is usually fixed, the absolute peak efficiency is dependent on energy only, but affected by self-absorption which depends on density of matrix and the elemental composition. The method to be used for determination of the peak efficiency is based on experimental procedures involving the following steps ... [Pg.174]

Instrumentation. The experimental procedure for an AFM equipped with a suitably coated tip has been outlined above. In a study of an aluminum alloy AA2024-T3, intermetallic particles and the matrix phase could be separated clearly [98]. The different surface films on these phases could be associated with their corrosion behavior. Inclusions and their corrosive behavior have been studied with a combination of SKPFM and AFM [101]. The effect of chloride-containing solution on corrosion at the matrix and the intermetallic particles was studied with SKPFM, in addition, light scratching with the AFM in the contact mode was applied to study the effect of the mechanical destabilization [102]. The intermetallic particles dissolved immediately after the film on their surface had been destabilized by mechanical abrasion. [Pg.263]

Recent analysis of thePVrbehavior of PA-6-based CPNCs revealed significant differences between systems having amorphous and semicrystalline matrix. The difference is particularly striking, comparing the region of the main transition vitrification and crystallization, respectively. The experimental procedure has been the same. The basic characteristics of the PA-6 systems are listed in Table 14.2 [Utracki, 2009a,b]. [Pg.567]

Only intermediates that are formed before the rate-determining step can accumulate. Reactions where intermediates can be isolated in a normal work up are rather rare. More often, intermediates might be observable by spectroscopic techniques. The existence of short-lived intermediates or of intermediates occurring after the rate-determining step can still be demonstrated by trapping reactions or by special techniques such as matrix isolation. This chapter provides detailed explanations of reaction mechanisms involving carbanions, possible transition states, and the scope of the reactions. The selected experimental procedures can be implemented quickly and easily in the laboratory. [Pg.65]

Figure 2. The hybrid-hybrid relaxation matrix refinement procedure for 3D NOESY-NOESY data. A starting model is used to simulate NOE data for the first iteration. Experimental 3D data is scaled and merged with simulated 3D data to produce a linear table of 3D experimental volumes and the simulated volumes needed for deconvolution. Deconvoluted 2D data is merged with any available 2D experimental data and then with a simulated, complete 2D volumes matrix. The structures resulting from the standard 2D MORASS refinement are used in subsequent iterations until convergence is reached. (Reproduced with permission from reference 24. Copyright 1996.)... Figure 2. The hybrid-hybrid relaxation matrix refinement procedure for 3D NOESY-NOESY data. A starting model is used to simulate NOE data for the first iteration. Experimental 3D data is scaled and merged with simulated 3D data to produce a linear table of 3D experimental volumes and the simulated volumes needed for deconvolution. Deconvoluted 2D data is merged with any available 2D experimental data and then with a simulated, complete 2D volumes matrix. The structures resulting from the standard 2D MORASS refinement are used in subsequent iterations until convergence is reached. (Reproduced with permission from reference 24. Copyright 1996.)...

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See also in sourсe #XX -- [ Pg.328 , Pg.329 , Pg.330 , Pg.354 ]




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Experimental matrix

Experimental procedures

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