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Sensitivity measurement

The magnitude of the phase shift relates to the total depth of the metal penetrated and hence is a sensitive measure of the wall thiekness and loss of thiekness. [Pg.321]

Figure 2 Targets and for sensitivity measurements aJ dual array probe b inner SW tube probe c/ Encircling probe... Figure 2 Targets and for sensitivity measurements aJ dual array probe b inner SW tube probe c/ Encircling probe...
The surface work fiincdon is fonnally defined as the minimum energy needed m order to remove an electron from a solid. It is often described as being the difference in energy between the Fenni level and the vacuum level of a solid. The work ftmction is a sensitive measure of the surface electronic structure, and can be measured in a number of ways, as described in section B 1.26.4. Many processes, such as catalytic surface reactions or resonant charge transfer between ions and surfaces, are critically dependent on the work ftmction. [Pg.300]

Thus, by measuring the intemiolecular vibrations of a WBC, ultimately with resolution of the rotational, tuimelling and hyperfme stmcture, the most sensitive measure of the IPS is accessed directly. The difficulty of measuring these VRT spectra is the fact that they lie nearly exclusively at THz frequencies. As expected, the stiffer die interaction, the higher in frequency these modes are found. In general, the total 0.3-30 THz interval must be accessed, although for the softest or heaviest species the modes rarely lie above 10-15 THz. [Pg.1255]

Equally strict purity requirements apply to dimethyl terephthalate, as shown in Table 21. Freezing point is a sensitive measure of purity and can be ... [Pg.491]

Spectroscopic methods such as uv and fluorescence have rehed on the polyene chromophore of vitamin A as a basis for analysis. Indirectly, the classical Carr-Price colorimetric test also exploits this feature and measures the amount of a transient blue complex at 620 nm which is formed when vitamin A is dehydrated in the presence of Lewis acids. For uv measurements of retinol, retinyl acetate, and retinyl palmitate, analysis is done at 325 nm. More sensitive measurements can be obtained by fluorescence. Excitation is done at 325 nm and emission at 470 nm. Although useful, all of these methods suffer from the fact that the method is not specific and any compound which has spectral characteristics similar to vitamin A will assay like the vitamin... [Pg.102]

Include mea.surements that repre.sent the internal conditions of equipment. Including internal measurements such as tray compositions, between-catalyst-bed measurements or spatial measurements in a CSTR improve the hkelihood that the parameter estimates are accurate. These measurements are particularly useful when product compositions (e.g., principal component composition in superfractionation) are not a sensitive measure of the parameter estimate. [Pg.2575]

SALI is a reladvely new surface technique that delivers a quantitative and sensitive measure of the chemical composition of solid surfaces. Its major advantage, compared to its parent technique SIMS, is that quantitative elemental and molecular informadon can be obtained. SPI offers exciting possibilities for the analytical characterization of the surfaces of polymers and biomaterials in which chemical differ-endation could be based solely on the characteristic SALE spectra. [Pg.568]

In the UV most of the materials of interest, e.g. Si, polysilicon, SiGe, GaAs, and other semiconductor materials, are strongly absorbing this enables surface-sensitive measurements. Surface roughness, native oxide covering, material composition, and structural properties can be analyzed. [Pg.269]

Before equations such as Eqs. 6, 7 and 8 can be used, values for the surface energies have to be obtained. While surface energies of liquids may be measured relatively easily by methods such as the du Nouy ring and Wilhelmy plate, those of solids present more problems. Three approaches will be briefly described. Two involve probing the solid surface with a liquid or a gas, the third relies on very sensitive measurement of the force required to separate two surfaces of defined geometry. All involve applying judicious assumptions to the experimental results. [Pg.322]

As the current pulse is largely dominated by the stress differences, a short duration current pulse is observed upon loading with a quiescent period during the time at constant stress. With release of pressure upon arrival of the unloading wave from the stress-free surface behind the impactor, a current pulse of opposite polarity is observed. The amplitude of the release wave current pulse provides a sensitive measure of the elastic nonlinearity of the target material at the peak pressure in question. [Pg.110]

The indicated transition pressure of 15 GPa is in agreement with the published data with shock-wave structure measurements on a 3% silicon-iron alloy, the nominal composition of Silectron. A mixed phase region from 15 to 22.5 GPa appears quite reasonable based on shock pressure-volume data. Thus, the direct measure of magnetization appears to offer a sensitive measure of characteristics of shock-induced, first-order phase transitions involving a change in magnetization. [Pg.126]

Fig. 7.6. The weak ferromagnetic (WF) fraction (high temperature form) of hematite provides a sensitive measure of shock modification. Sample 31G836 is an 8 GPa experiment. Sample 29G836 is a 17 GPa experiment, while 17G846 is a 27 GPa sample (after Williamson et al. [86W03]). Fig. 7.6. The weak ferromagnetic (WF) fraction (high temperature form) of hematite provides a sensitive measure of shock modification. Sample 31G836 is an 8 GPa experiment. Sample 29G836 is a 17 GPa experiment, while 17G846 is a 27 GPa sample (after Williamson et al. [86W03]).
Four different material probes were used to characterize the shock-treated and shock-synthesized products. Of these, magnetization provided the most sensitive measure of yield, while x-ray diffraction provided the most explicit structural data. Mossbauer spectroscopy provided direct critical atomic level data, whereas transmission electron microscopy provided key information on shock-modified, but unreacted reactant mixtures. The results of determinations of product yield and identification of product are summarized in Fig. 8.2. What is shown in the figure is the location of pressure, mean-bulk temperature locations at which synthesis experiments were carried out. Beside each point are the measures of product yield as determined from the three probes. The yields vary from 1% to 75 % depending on the shock conditions. From a structural point of view a surprising result is that the product composition is apparently not changed with various shock conditions. The same product is apparently obtained under all conditions only the yield is changed. [Pg.182]

As with alternating electrical currents, phase-sensitive measurements are also possible with microwave radiation. The easiest method consists of measuring phase-shifted microwave signals via a lock-in technique by modulating the electrode potential. Such a technique, which measures the phase shift between the potential and the microwave signal, will give specific (e.g., kinetic) information on the system (see later discussion). However, it should not be taken as the equivalent of impedance measurements with microwaves. As in electrochemical impedance measurements,... [Pg.451]

As mentioned at the beginning of this chapter real phase-sensitive measurements of electrochemical systems have not yet been performed. Not only is the experimental technique difficult, but a reliable theory of... [Pg.514]

Several other techniques for have evolved for biochemical assays. In chapter 2 of this book, Omann and Sklar report on a method of fluoroimmunoassay where the bound and unbound antigen are separated by the quenching of fluorescence that accompanies antibody binding. Then, in chapter 3, Holl and Webb show how they achieved a sensitive measurement of nucleic acids by the enhancement in fluorescence that accompanies the binding of fluorescent dyes to nucleic acids. Chandler et al, also used fluorescence enhancement to monitor calcium mobility in neutrophil cells. [Pg.15]

The most direct way to test the validity of a mechanism is to determine what intermediates are present during the reaction. If oxygen atoms were detected, we would know that Mechanism I is a reasonable description of NO2 decomposition. Likewise, the observation of NO3 molecules would suggest that Mechanism II is reasonable. In practice, the detection of intermediates is quite difficult because they are usually reactive enough to be consumed as rapidly as they are produced. As a result, the concentration of an intermediate in a reaction mixture is very low. Highly sensitive measuring techniques are required for the direct detection of chemical intermediates. [Pg.1052]

The cancellation of gas phase spectral features using the "half plate design Is far superior to methods Involving a second gas cell placed In the reference beam. This Is because the gas density and Its rotational state population will differ In the two cells for different sample (and therefore gas) temperatures. For high sensitivity measurements, these effects can be difficult to handle using two cells. [Pg.407]

Sheik-Bahae, M., Said, A. A., Wei, T. H., Hagan, D. J. and Van Stryland, E. W. (1990) Sensitive measurement of optical nonlinearities using a single beam. IEEE J Quantum Electron., 26, 760-769. [Pg.167]


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See also in sourсe #XX -- [ Pg.78 , Pg.79 ]




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