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X interference

Fig. 10.1 (a) First-order chemical sensor in which absorbance is uniquely related to concentration by calibration curve, (b) Second-order sensor in which absorbance is shown as a function of wavelength X. Interferant is easily identified in the spectrum, (c) Third-order sensor yielding information in 3-D space. The red dashed line shows conversion of third-order sensor to second-order sensor when the value of response R is obtained at a fixed retention time/ ... [Pg.315]

Assume that there exists a substructure X which is transformed into substructure X by reaction A. Similarly there is a substructure Y which is transformed into substructure Y by reaction B. We further assume that X and Y have no atoms in common in the molecules of interest. Suppose that a molecule contains both substructure X and Y and reactions A and B are used successively to produce a molecule with substructures X and Y. In many cases the order of performance of A and B is immaterial. In other words, neither substructure X nor substructure X interfere with reaction B and neither Y nor Y ... [Pg.339]

Should tho tliuinb pie interfere with the head of the hammer in raising the bceech block, it b probable that either the tnmUcr or sear screvi is too loose or broken. [Pg.408]

Substances capable of undergoing cationic polymerization, such as isobutene, styrene and a-methylstyrene, polymerize by a cationic mechanism if subjected to irradiation with y or X-rays, provided that they have been rigorously purified from impurities, in particular from traces of water. Scheme 5.5 presents a kinetic scheme of cationic polymerization which takes into account that an impurity X interferes with the polymerization. The initiation comprises the generation of free ions A" and B , the latter being a free electron or a molecular ion. [Pg.259]

Fig. 5.7.1 DifiEraction of a plane wave at a set of parallel narrow slits. Radiation of wavelength X interferes constractively with itself at particular angles where a constant difference, mX, exists between adjacent shts. A spectram forms at the focal plane of the lens. Fig. 5.7.1 DifiEraction of a plane wave at a set of parallel narrow slits. Radiation of wavelength X interferes constractively with itself at particular angles where a constant difference, mX, exists between adjacent shts. A spectram forms at the focal plane of the lens.
Fig. 11 shows a composite model of the wave at U X =0.25. In the interfering wave on the upper and lower part of the insert metal, (a) is the same phase, and (b) is the opposite phase. A composite wave is attenuated by the weakened interference as the same phase, and is amplified by the strengthened interference as the opposite phase. [Pg.838]

Figure Bl.8.2. Bragg s law. Wlien X = 2d sin 0, there is strong, constructive interference. (B) THE RECIPROCAL LATTICE... Figure Bl.8.2. Bragg s law. Wlien X = 2d sin 0, there is strong, constructive interference. (B) THE RECIPROCAL LATTICE...
Diffraction is based on wave interference, whether the wave is an electromagnetic wave (optical, x-ray, etc), or a quantum mechanical wave associated with a particle (electron, neutron, atom, etc), or any other kind of wave. To obtain infonnation about atomic positions, one exploits the interference between different scattering trajectories among atoms in a solid or at a surface, since this interference is very sensitive to differences in patii lengths and hence to relative atomic positions (see chapter B1.9). [Pg.1752]

Eden G J, Gao X and Weaver M J 1994 The adsorption of suiphate on goid(111) in acidic acqueous media Adiayer structurai interferences from infrared spectroscopy and scanning tunneiing microscopy J. Electroanal. Chem. 375 357-66... [Pg.2757]

Knowing the selectivity coefficient provides a useful way to evaluate an inter-ferent s potential effect on an analysis. An interferent will not pose a problem as long as the term K/ i X i in equation 3.7 is significantly smaller than or A,i X Q in equation 3.8 is significantly smaller than Ca. [Pg.41]

A sample contains a weak acid analyte, HA, and a weak acid interferent, HB. The acid dissociation constants and partition coefficients for the weak acids are as follows Ra.HA = 1.0 X 10 Ra HB = 1.0 X f0 , RpjHA D,HB 500. (a) Calculate the extraction efficiency for HA and HB when 50.0 mF of sampk buffered to a pH of 7.0, is extracted with 50.0 mF of the organic solvent, (b) Which phase is enriched in the analyte (c) What are the recoveries for the analyte and interferent in this phase (d) What is the separation factor (e) A quantitative analysis is conducted on the contents of the phase enriched in analyte. What is the expected relative erroi if the selectivity coefficient, Rha.hb> is 0.500 and the initial ratio ofHB/HA was lO.O ... [Pg.229]

If real growth fronts were to impinge on a point like this, their growth would terminate at x. Suppose we imagine point x to be charmed in some way such that any number of growth fronts can pass through it without interference. [Pg.220]

Basically, Newtonian mechanics worked well for problems involving terrestrial and even celestial bodies, providing rational and quantifiable relationships between mass, velocity, acceleration, and force. However, in the realm of optics and electricity, numerous observations seemed to defy Newtonian laws. Phenomena such as diffraction and interference could only be explained if light had both particle and wave properties. Indeed, particles such as electrons and x-rays appeared to have both discrete energy states and momentum, properties similar to those of light. None of the classical, or Newtonian, laws could account for such behavior, and such inadequacies led scientists to search for new concepts in the consideration of the nature of reahty. [Pg.161]

Chromium (ITT) can be analy2ed to a lower limit of 5 x 10 ° M by luminol—hydrogen peroxide without separating from other metals. Ethylenediaminetetraacetic acid (EDTA) is added to deactivate most interferences. Chromium (ITT) itself is deactivated slowly by complexation with EDTA measurement of the sample after Cr(III) deactivation is complete provides a blank which can be subtracted to eliminate interference from such ions as iron(II), inon(III), and cobalt(II), which are not sufficiently deactivated by EDTA (275). [Pg.274]

The biochemical basis for the toxicity of mercury and mercury compounds results from its ability to form covalent bonds readily with sulfur. Prior to reaction with sulfur, however, the mercury must be metabolized to the divalent cation. When the sulfur is in the form of a sulfhydryl (— SH) group, divalent mercury replaces the hydrogen atom to form mercaptides, X—Hg— SR and Hg(SR)2, where X is an electronegative radical and R is protein (36). Sulfhydryl compounds are called mercaptans because of their ability to capture mercury. Even in low concentrations divalent mercury is capable of inactivating sulfhydryl enzymes and thus causes interference with cellular metaboHsm and function (31—34). Mercury also combines with other ligands of physiological importance such as phosphoryl, carboxyl, amide, and amine groups. It is unclear whether these latter interactions contribute to its toxicity (31,36). [Pg.109]


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See also in sourсe #XX -- [ Pg.68 , Pg.81 ]




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