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Calibration intensity

Figure 6 illustrates a block diagram of a crossed-coil variable frequency spectrometer and associated electromagnet. A calibrator circuit 66) is useful for intensity calibration of absorption and dispersion mode signals. A calibrator circuit for the Pound-Knight type of spectrometer is also used... [Pg.47]

Fig. 2. Mass spectrometer with photoionization 1—built-in hydrogen lamp 2—vacuum monochromator filled with hydrogen 3—LiF window 4—ionic source container 5—photoionization space with the accelerating grids 6—fluorescent layer for intensity calibration of the incident u.v. light 7—photomultiplier 8—magnetic mass analyzer 9—electron multiplier. Fig. 2. Mass spectrometer with photoionization 1—built-in hydrogen lamp 2—vacuum monochromator filled with hydrogen 3—LiF window 4—ionic source container 5—photoionization space with the accelerating grids 6—fluorescent layer for intensity calibration of the incident u.v. light 7—photomultiplier 8—magnetic mass analyzer 9—electron multiplier.
Fig. 115. Arrangements for printing intensity calibration strips on X-ray photographs. a. Sector wheel to give a stepped wedge. b. Cam to give a continuous wedge. Fig. 115. Arrangements for printing intensity calibration strips on X-ray photographs. a. Sector wheel to give a stepped wedge. b. Cam to give a continuous wedge.
The images are calibrated to the inner diameter of the 10-mm NMR tube, which is 8.9 mm [4]. The total volume for each cross-sectional slice is determined by first calculating the area of the coke bean, and then multiplying the area by the 300 pm slice thickness. The mean intensity was calculated, and the image intensity calibrated internally such that the brightest... [Pg.513]

Comparatively low spectral resolution % 0.6 j) and difficulties with the intensity calibration did not warrant any detailed abundance analysis of our spectral material. Instead, the stars with similar spectral types were divided into four groups according to the strength of the lithium line. The groups may be described as follows (see Fig. 1) 1 - the lithium line is... [Pg.15]

The J=2-l, v=0 emissions of ZBSiO,Z9SiO, and 30SiO from Villi Oph, NML Tau, and X Cyg were observed with the Nobeyama 45-m telescope in Jaunuary 19871 At 86 GHz, the half-power beamwidth was 20 , and the aperture efficiency 0.37. The three lines were simultaneously observed using two receivers with instantaneous bandwidths of 2 GHz and 0.5 GHz to reduce errors in relative intensities due to pointing and intensity calibration errors. The intensity scale reported here is the antenna temperature T, corrected for atmospheric and ohmic losses. [Pg.51]

Finally, the impact of possible calibration instability on the prediction quality must be understood. In this case, spectrograph and laser wavelength calibrations were very stable and easy to update, but of minor concern because of the broad bands being used. However, since the intensity calibration function is non-linear, any changes in it could unequally affect bands used in the calibration ratio and introduce error in the prediction. Newer equipment offers easy intensity calibration routines but this can be difficult to use automatically with immersion probes since it requires that they be removed from the process. [Pg.153]

Fig. 25. 250-MHz H NMR spectra of Hb A in both deoxy and oxy forms in 0.1 M Bis-Tris plus 10 mM IHP in D20 at pH 6.6 at 27°C. The resonance at 27 ppm was that of the NMR shift reagent. This reference signal was used for the intensity calibration of the ferrous hyperfine-shifted proton resonances. [From Ho et al. (1982b)]. Fig. 25. 250-MHz H NMR spectra of Hb A in both deoxy and oxy forms in 0.1 M Bis-Tris plus 10 mM IHP in D20 at pH 6.6 at 27°C. The resonance at 27 ppm was that of the NMR shift reagent. This reference signal was used for the intensity calibration of the ferrous hyperfine-shifted proton resonances. [From Ho et al. (1982b)].
In order to probe some of these questions - an essential endeavor in forming a clear interpretation of our results - we wish to compare our experimentally-determined data with predictions from a simple model. The experimental data available (See Fig. 3) are instantaneous values of flame temperature from the N2 Stokes/anti-Stokes intensity ratio (plotted as histograms in Fig. 4) and simultaneously-obtained values of Nj density (determined from the absolute value of the N. Stokes intensity calibrated against the value obtained for N2 in ambient air). Accordingly, we have produced "comparison" plots using the following scheme (24) If we calculate flame gas density and temperature as a function of flame stoichiometry (i.e., as a function of the fuel/air equivalence ratio see Fig.7), then we can... [Pg.220]

Further barriers to a broader use of Raman spectroscopy are problems with intensity calibration and benchmarking, lack of reference materials, and the expense of the equipment. The calibration equipment, which is typically supplied with the instruments by the manufacturers, varies for instance neon or mercury lamps are delivered with dispersive instruments and HeNe lasers with FT spectrometers. [Pg.54]

Fig. 1 depicts a characteristic time-resolved Cu" emission spectrum of Cu-ZSM-5 with two main bands at 480 and 540 nm with different decay times. It evidences different defined Cu sites. Very low intensity bands at 450 and 605 nm (Fig. 5) have been shown to correspond additional defined Cu site and Cu bonded via Si-OH, resp. (9). The intensity of the band at 605 nm had never exceed 3% of the total spectrum intensity and is neglected in the spectra analysis. A lifetime of 5 s was chosen for the spectra evaluation note the importance of the luminescence lifetime for the spectra monitoring, cf Fig. 1. It is suppossed that the Cu luminescence intensity is proportional to the number of the corresponding Cu sites and the saturation of the luminescence intensity is not expected. Zeolites with the Cu/Al ratio below 0.5 were used for luminescence intensity calibration. The relationship between the Cu content in the zeolite and the intensities of the individual bands at 450, 480 and 540 nm (for Cu-ZSM-5) is... Fig. 1 depicts a characteristic time-resolved Cu" emission spectrum of Cu-ZSM-5 with two main bands at 480 and 540 nm with different decay times. It evidences different defined Cu sites. Very low intensity bands at 450 and 605 nm (Fig. 5) have been shown to correspond additional defined Cu site and Cu bonded via Si-OH, resp. (9). The intensity of the band at 605 nm had never exceed 3% of the total spectrum intensity and is neglected in the spectra analysis. A lifetime of 5 s was chosen for the spectra evaluation note the importance of the luminescence lifetime for the spectra monitoring, cf Fig. 1. It is suppossed that the Cu luminescence intensity is proportional to the number of the corresponding Cu sites and the saturation of the luminescence intensity is not expected. Zeolites with the Cu/Al ratio below 0.5 were used for luminescence intensity calibration. The relationship between the Cu content in the zeolite and the intensities of the individual bands at 450, 480 and 540 nm (for Cu-ZSM-5) is...
For this evaluation, an intensity calibration in absolute units (here crn g srad) ) is necessary. [Pg.362]

Since the thermal emission curve from a black-botdy radiator may be calculated from first principles, it can serve as a primary standard for an intensity vs. wavelength curve. Petty et al. (16) described a procedure for intensity calibration of an FT-Raman spectrometer using such a source. Provided the source acts as a black body to the required accuracy, its temperature is known, and the laser wavelength is known accurately, the black-body provides a known i(AT>) curve to use in Eq. (10.3). Since most modern spectrometers measure photons/second rather than watts, the proper units for b fAv) are photons per second per wavenumber. ... [Pg.272]

An ideal luminescent standard for Raman intensity calibration would have several characteristics (17), some of which are difficult to achieve ... [Pg.276]

The admixture of the standard should be dimensioned so that the strongest lines of sample and standard become about equal. The right ratio can be calculated if the I/I -values of standard (Is/Ic) and sample (Ip/Ic) are known (see above at intensity calibration). The weight ratio Xp ( sample) (standard) can be estimated by ... [Pg.128]

Peak intensity calibration is another essential procedure required for correct determination of the isotope concentrations from the observed spectra. Here we should note that the peak intensity per one OH bond is not necessary equal to that per one OD bond. Calibration spectra are taken for an ice specimen containing homogeneously distributed H and D isotopes prepared by freezing an... [Pg.743]


See other pages where Calibration intensity is mentioned: [Pg.14]    [Pg.286]    [Pg.372]    [Pg.14]    [Pg.19]    [Pg.1445]    [Pg.1449]    [Pg.1471]    [Pg.1472]    [Pg.1486]    [Pg.1490]    [Pg.5]    [Pg.134]    [Pg.79]    [Pg.188]    [Pg.120]    [Pg.6105]    [Pg.108]    [Pg.275]    [Pg.276]    [Pg.276]    [Pg.426]    [Pg.92]    [Pg.77]   
See also in sourсe #XX -- [ Pg.276 ]




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