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Detection atomic

Fig. 4.13. 3(t limit of detection [atoms surface preparation system (WSPS) for... [Pg.191]

The isotope dilution method can be used for the measurement of molecules or elemental species (about 60 elements have stable isotopes). This approach allows ultratrace analysis because, contrary to radioactive labelling where the measurement relies on detecting atoms that decay during the period of measurement, all of the labelled atoms are measured. [Pg.660]

If N is the total number of detected atoms of the segregating element i, N the total number of atoms detected, cm the matrix concentration of the element, then... [Pg.12]

Winefordner JD, Parsons ML, Mansfield JM, McCarthy WJ (1967) Derivation of expressions for calculation of limiting detectable atomic concentration in atomic fluorescence flame spectrometry. Anal Chem 39 436... [Pg.241]

Two improvements to the FPD design have been made in recent years. First, the addition of an oxygen-rich burner upstream of the FPD oxidizes hydrocarbons to CO and C02 and thereby eliminates the hydrocarbon interference within the analytical flame [105, 106], This increases the sensitivity of the detector to approximately 20 pg S s"1 for a nonlinearized FPD [102], In a second improvement, the PFPD was developed to significantly reduce the background and increase the sensitivity to all detectable atoms [107], This detector is now commercially... [Pg.377]

Phosphorus-32, for example, produced by irradiating sulphur or natural phosphorus ( P) with high-energy particles, has a half-life of 14.8 days and can be rapidly taken up (in the form of phosphate) by body tissues such as muscles, the liver, bones, and teeth. De Hevesy found that different phosphorus compounds would be incorporated in a tissue-specific manner certain compounds were concentrated in the liver, for example. One can use stable isotopes as biological tracers too, since they are detectable atom by atom using mass spectrometry. De Hevesy observed that it takes deuterium twenty-six minutes to pass from ingested heavy water into urine. [Pg.134]

Winefordner, J. D., M. L. Parsons, J. M. Mansfield, and W. J. McCarthy Derivation of Expressions for Calculation of the Limiting Detectable Atomic Concentration in Atomic Fluorescence Flame Spectrometry. Anal. Chem. 39, 436 (1967). [Pg.111]

By using lasers of suitable frequency, fluorescence can be extended into the infrared and microwave. Offshoots of laser technology include resonance fluorescence for detecting atoms, and laser magnetic resonance for radicals. [Pg.15]

Microwave-induced plasma (MIP), direct-current plasma (DCP), and inductively coupled plasma (ICP) have also been successfully utilized. The abundance of emission lines offer the possibility of multielement detection. The high source temperature results in strong emissions and therefore low levels of detection. Atomic absorption (AA) and atomic fluorescence (AF) offer potentially greater selectivity because specific line sources are utilized. On the other hand, the resonance time in the flame is short, and the limit of detectability in atomic absorption is not as good as emission techniques. The linearity of the detector is narrower with atomic absorption than emission and fluorescence techniques. [Pg.312]

NMR spectra of nuclei such as 57Fe (spin V2) in magnetic materials can be measured without external magnetic field. Also in the case of nuclear quadrupole resonance (NQR) no static magnetic field is necessary. For this reason NQR is sometimes called "zero field NMR". It is used to detect atoms whose nuclei have a nuclear quadrupole moment, such as 14N and 35C1. [Pg.361]

Nuclear magnetic resonance (NMR) allows us to detect atomic nuclei and say what sort of environment they are in, within their molecule. Clearly, the hydrogen of, say, propanol s hydroxyl group is... [Pg.56]

Multiple bonds, internal rings, and other molecular substructures or subgraphs (see Figure 4.10a) are recognized through a circular inspection method. A circle of inspection centered on each detected atom is considered (see Figure 4.10b). Unknown border pixels found in this way are kept and used as the initial point for a new counterclockwise contour search, and the perception of new vertices and probable new atoms is carried out as described earlier. [Pg.58]

The architecture of the individual instruments used to detect atoms and small free radicals by atomic and molecular resonance fluorescence or by laser-induced fluorescence is shown in Figure 13, but is discussed in detail elsewhere. Briefly, a nacelle, hollow through the core from nose to tail with an impeller in the anterior section, provides for the laminar flow of stratospheric air around and through the instrument. Detection of trace species is carried out at one (or. more) optical axes within the nacelle. A major subset of the important stratospheric radicals can be detected using the configuration shown in Figure 13. [Pg.365]

Analytical techniques need to be applied to a variety of sample types. Methods should be chosen which are applicable to individual particles, gases, liquid solution, and bulk materials such as soils and other solids. Many such techniques have been developed. Listed in Table 12.9 is a summary of those methods which have been utilized effectively for environmental sample analysis. Those techniques which are more highly recommended are so marked. Most, although not all, of the equipment is commercially available. It is important to emphasize that the open literature shows that scientists have the ability to detect atomic, nanogram, and/or milligram levels of target species. A combination of several techniques for both bulk and individual particle analysis that will yield the level of information is necessary. [Pg.629]

The discussion of emission spectroscopy will be concluded by a description of a rather unusual application. Bay and Steiner have measured atomic hydrogen concentrations in the presence of molecular hydrogen by microwave excitation of the atomic hydrogen line spectrum. With low power fed into the gas (ca. 5 watts), there is not enough energy available for the dissociation of molecular hydrogen and subsequent excitation. Thus the measured intensities of the atomic hydrogen lines correspond to the concentrations of atoms already present in the reaction mixture. The method is curiously similar to that adopted to detect atoms and free radicals by mass spectrometry (see Section 3). [Pg.290]

Thermal conductivity measurements offer a further possible method for detecting unstable reaction intermediates. Such studies have been made by Senftleben et al. to detect atomic hydrogen in the mercury sensitised photolysis of molecular... [Pg.324]

In WDS, the analyzing crystal should be carefully selected because it determines the range of detectable atomic numbers. The wavelength that can be detected by a crystal is defined by Bragg s Law. [Pg.180]

Elemental composition is an important chemical property which can be used to establish the nature and source of humic substances. When the percent composition data are displayed as the atom ratios H C, 01C, and NIC, some general characteristics become visible. Soil, coal, marine, and aquatic humates may be distinguished, one from the other. Structural trends may be identified in specific environments, such as lake sediments and soil profiles. Nonhumate contaminants can be detected. Atom ratios may also aid the investigator in proposing hypothetical structures for humic and fulvic acids and serve as a guide in the synthesis of artificial humates. [Pg.457]

We now note that, according to the principles of quantum theory, not the path, but causality in the transmission of information from one object to another is important [3,10-13,31]. In the Hertz experiment with two atoms separated by empty space, this means that the detecting atom cannot be excited earlier than in d/c seconds after the emission of a photon by the first atom. Here d denotes the interatomic distance. Such a causality has been proven recently by Kaup and Rupasov [96]. Here we briefly discuss their proof. [Pg.472]

Figure 18. Time dependence of the mean population of the excited level of the detecting atom. Figure 18. Time dependence of the mean population of the excited level of the detecting atom.

See other pages where Detection atomic is mentioned: [Pg.119]    [Pg.20]    [Pg.178]    [Pg.168]    [Pg.36]    [Pg.1415]    [Pg.132]    [Pg.460]    [Pg.69]    [Pg.405]    [Pg.201]    [Pg.119]    [Pg.881]    [Pg.274]    [Pg.191]    [Pg.462]    [Pg.273]    [Pg.9]    [Pg.191]    [Pg.206]    [Pg.209]    [Pg.181]    [Pg.469]    [Pg.471]    [Pg.475]   


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