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Signal , generally intensity

The photon counter is used in the processing of weak signals generated from a photomultiplier. The photomultiplier output signal generally consists of a series of discrete peaks with different intensities (see Figure 3.22). The reason for this is that. [Pg.103]

The reaction of [Ag(n-Bu2 Dtc)] 6 with w-Bu4Tds in a 1 6 molar ratio afforded a dark red solution, which faded within 10 minutes to an EPR active blue solution. On the basis of the intensity of the EPR signal, generally attributed to the blue Ag(II) R2Dtc complexes, it was suggested that the red solution contained an Ag(III) complex (27). [Pg.330]

This type of ENDOR is generally not so sensitive to experimental conditions such as temperature and microwave and rf power as is steady-state ENDOR. Marked peculiarities do exist, however. For example, for this type of ENDOR, depending on experimental conditions, the ENDOR response can be either an increase or a decrease in the EPR signal. Generally a decrease is the norm. In addition, some cross-relaxation effects can make the intensities and relative directions of the and v transitions anomalously different we have often found the transitions to be more intense, particularly at the higher (35 GHz) microwave frequency. [Pg.567]

Standard IR cells with windows appropriate for the materials under investigation are used. To avoid erroneous VCD signals, absorption intensities should be kept in the range 0.2-0.8, and it is usually good practice to check instrument performance regularly with a compound for which the VCD spectrum is well documented, e.g., a-pinene. With an FT interferometer, VCD intensities must be calibrated, - a procedure in which the sample is replaced by a second polarizer. Samples are usually in solution in a suitable solvent, in a matrix of solid inert gas, or neat liquids. The spectra of a few selected gaseous materials have been reported.Solid samples of chiral compounds are not suitable for CD measurements because they also exhibit linear dichroism that generally dominates and obscures the circular dichroism. [Pg.264]

We often see splitting patterns in which the intensities of the individual peaks do not match those given in Table 13 2 but are distorted in that the signals for coupled protons lean toward each other This leaning is a general phenomenon but is most easily illus trated for the case of two nonequivalent vicinal protons as shown m Figure 13 18... [Pg.541]

In color technology and measurement, both types of approaches are used. Color printing, for example, generally employs three colors (usually plus black), and the ever useful CIE system was founded on experiments in which colors were matched by mixtures of three primary colors, often blue, green, and red. Yet transmitted television signals are based on the opponent system, with one intensity and two color-balance signals, as are the modern representations of color, such as the CIELAB and related color spaces based on red-green and yeUow-blue opponent axes. [Pg.406]

Figures 1.9a and b demonstrate the effeet of proton broadband deeoupling in the C NMR speetrum of a mixture of ethanol and hexadeuterioethanol. The C//j and CH2 signals of ethanol appear as intense singlets upon proton broadband deeoupling while the CD3 and CD2 resonanees of the deuteriated eompound still display their septet and quintet fine strueture deuterium nuelei are not affected by H decoupling because their Larmor frequeneies are far removed from those of protons further, the nuelear spin quantum number of deuterium is 7/3=/ in keeping with the general multiplieity rule (2nx Ix+ 1, Seetion 1.4), triplets, quintets and septets are observed for CD, CD2 and CD3 groups, respeetively. The relative intensities in these multiplets do not follow Paseal s triangle (1 1 1 triplet for CD 1 3 4 3 1 quintet for CD2 1 3 6 7 6 3 1 septet for CD3). Figures 1.9a and b demonstrate the effeet of proton broadband deeoupling in the C NMR speetrum of a mixture of ethanol and hexadeuterioethanol. The C//j and CH2 signals of ethanol appear as intense singlets upon proton broadband deeoupling while the CD3 and CD2 resonanees of the deuteriated eompound still display their septet and quintet fine strueture deuterium nuelei are not affected by H decoupling because their Larmor frequeneies are far removed from those of protons further, the nuelear spin quantum number of deuterium is 7/3=/ in keeping with the general multiplieity rule (2nx Ix+ 1, Seetion 1.4), triplets, quintets and septets are observed for CD, CD2 and CD3 groups, respeetively. The relative intensities in these multiplets do not follow Paseal s triangle (1 1 1 triplet for CD 1 3 4 3 1 quintet for CD2 1 3 6 7 6 3 1 septet for CD3).
Measuring EXAFS spectra In general, transmission EXAFS can be used, provided that the concentration of the element to be investigated is sufficiently high. The sample is placed between two ionization chambers, the signals of which are proportional to the incident intensity Iq and the transmitted intensity through the sample 7f The transmission of the sample is dependent on the thickness of the sample X and on the absorption coefficient, //, in a Beer-Lambert relationship ... [Pg.140]


See other pages where Signal , generally intensity is mentioned: [Pg.112]    [Pg.721]    [Pg.95]    [Pg.90]    [Pg.258]    [Pg.150]    [Pg.99]    [Pg.323]    [Pg.168]    [Pg.238]    [Pg.465]    [Pg.522]    [Pg.28]    [Pg.2022]    [Pg.31]    [Pg.37]    [Pg.1179]    [Pg.1281]    [Pg.1295]    [Pg.1570]    [Pg.1570]    [Pg.1571]    [Pg.1671]    [Pg.1990]    [Pg.2485]    [Pg.401]    [Pg.401]    [Pg.402]    [Pg.405]    [Pg.48]    [Pg.127]    [Pg.319]    [Pg.110]    [Pg.444]    [Pg.4]    [Pg.138]    [Pg.158]    [Pg.724]    [Pg.55]    [Pg.60]    [Pg.670]    [Pg.1302]   
See also in sourсe #XX -- [ Pg.461 , Pg.700 , Pg.704 ]




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Signal intensity

Signals general

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