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Transmission curves, normal

The classification of linings in the U.S. model building codes is based on the FSI and SDI (smoke developed index). The latter is based on the area under the light transmission versus time curve normalized to the area for red oak flooring, which by definition has an SDI of 100. There are three classes Class A for products with FSI < 25, Class B for products with 25 < FSI < 75, and Class C for products with 75 < FSI < 200. In all cases, the SDI must be 450 or less. Class A products are generally permitted in enclosed vertical exits. Class B products can be used in exit access corridors and Class C products are allowed in other rooms and areas. [Pg.369]

Figure 1. Normal transmission curves (T vs, wavelength) compared with log density or log absorbance curves [log(log 1/T) vs, wavelength]... Figure 1. Normal transmission curves (T vs, wavelength) compared with log density or log absorbance curves [log(log 1/T) vs, wavelength]...
Thus x(vq, m) is proportional to dT/dt>o> the derivative of the normal transmission curve. The amplitude of the secondary modulation must be much less than the width of the Mossbauer line so that dr/dvo is nearly constant over the amplitude. [Pg.27]

With these sets of angles and with fixed n and X the transmission curves for two combinations of An and d are calculated. The first combination is d=10 ym and An=0.2. The transmission curves for normal incidence are presented in Fig. 6. The curve parameter is K33/KH. The transmission characteristics is steepest for smallest values of K33/K11. [Pg.66]

Normalized transmittance curves (verses time) for identical EB and D 1 photosensitizer concentrations are given in Figure 8.8. Due to the weak absorptivity of D 1 (see Figure 8.8(b)), the transmission curve, which, when t = 0, has a large value To - T t = 0) = 0.75, only increases by approximately 0.01. [Pg.266]

The three normal means of presenting the spectrophotometric data are described below by far the most common procedure is to plot absorbance against wavelength (measured in nanometres). The wavelength corresponding to the absorbance maximum (or minimum transmission) is read from the plot and is used for the preparation of the calibration curve. This point is chosen... [Pg.708]

The example is valid for the most simple case SAXS or USAXS in normal-transmission geometry. 27The same line of code evaluates curves, images or data structures of higher dimensionality (imagine time as an additional coordinate)... [Pg.48]

Figure 26. (a) Transmission electron micrograph of PDHS cast as a thin film from THF at 100 °C and subsequently cooled slowly to ambient temperature. Thick crystals with characteristic striations normal to the crystal length and parallel to the molecular backbones are seen in edge-on orwntations. (b) A different region from the same specimen shown in part a, which demonstrates the parallelism of the striations even in curved crystals. [Pg.374]

Figure Bl.22.8. Sum-frequency generation (SFG) spectra in the C N stretching region from the air/aqueous acetonitrile interfaces of two solutions with different concentrations. The solid curve is the IR transmission spectrum of neat bulk CH CN, provided here for reference. The polar acetonitrile molecules adopt a specific orientation in the air/water interface with a tilt angle that changes with changing concentration, from 40° from the surface normal in dilute solutions (molar fractions less than 0.07) to 70° at higher concentrations. This change is manifested here by the shift in the C N stretching frequency seen by SFG [57]. SFG is one of the very few techniques capable of probing liquid/gas, liquid/liquid, and even liquid/solid interfaces. Figure Bl.22.8. Sum-frequency generation (SFG) spectra in the C N stretching region from the air/aqueous acetonitrile interfaces of two solutions with different concentrations. The solid curve is the IR transmission spectrum of neat bulk CH CN, provided here for reference. The polar acetonitrile molecules adopt a specific orientation in the air/water interface with a tilt angle that changes with changing concentration, from 40° from the surface normal in dilute solutions (molar fractions less than 0.07) to 70° at higher concentrations. This change is manifested here by the shift in the C N stretching frequency seen by SFG [57]. SFG is one of the very few techniques capable of probing liquid/gas, liquid/liquid, and even liquid/solid interfaces.
The normal calibration curve is asymptotic to the value of (B), which represents the transmission of unabsorbed light. Unabsorbed light may be due to straylight or non-absorbing lines from the radiation source (cathode material or filler gas) which pass within the spectral bandwidth of the monochromator. The slope of the calibration graph is also dependent on the ratio of the half-widths of the emission line (zt e) and absorption line w (i) The curve is linear when wjw < l/5 (ii) The curve is slightly curved when /b < wjw < / (hi) The initial slope starts to decrease when > 1/1 ... [Pg.47]

This is the simplest, qualitative extension of Eq. (49) when ignoring the variation of the transmission T with energy. With semiconductors and higher gap voltages the normalized differential conductance Psampie( ) oc dlldU)/ I/U) is used [208]. Such Psampie( ) curves reproduce pronounced features of the real... [Pg.88]

Fig. 14. Curves for detector gamma ray counting rate vs. neutron time of flight for 35-22 meters for a l/ = 103.3 barns/ atom thickness sample of normal Ag at the detector position (D only) and for foils having l/ = 103.3 bams/atom thickness at both detector and transmission positions. The measurements were made using the Columbia Nevis velocity spectre-meter system with 0,25 xsec detection interval gates for / O.Ol (isec/m resolution. Fig. 14. Curves for detector gamma ray counting rate vs. neutron time of flight for 35-22 meters for a l/ = 103.3 barns/ atom thickness sample of normal Ag at the detector position (D only) and for foils having l/ = 103.3 bams/atom thickness at both detector and transmission positions. The measurements were made using the Columbia Nevis velocity spectre-meter system with 0,25 xsec detection interval gates for / O.Ol (isec/m resolution.
Gray scale inversion is explained in Fig. 9.9. Figure 9.9a shows a transmission voltage curve for normal incidence angles. For normal incidence the... [Pg.135]


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See also in sourсe #XX -- [ Pg.174 ]




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Curve normal

Normal transmission

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