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Calculated normalized absorption

Under normal conditions (e.g. 10 mA) with the sample in the flame, a global measurement of background absorption and absorption by the element is obtained. However, under strained lamp conditions (e.g. 500 mA), only background absorption is measured. Comparison of both measurements allows the calculation of absorption due only to the analyte. [Pg.267]

The normalized absorption and fluorescence spectra of Dye 1 on 200 nm AgBr are shown in Fig. 3. The absorbance was calculated from the measured reflection spectrum using the Kubelka-Munk equation. The absorption spectrum of Dye 1 in methanol solution is also given. The absorption spectrum of Dye 1 on AgBr crystals shows a typical J-aggregate character and gives a sharp and red-shifted band relative to the monomeric band. [Pg.511]

The work of Rostkowska s group132 on 2-thiocytosine and 5-fluoro-2-thiocytosine deals with molecular systems which are closely related to thioguanine. Similarly to what was found for mercaptopyridines and mercaptodiazines, the IR absorption spectra of these two compounds show that when the interactions with the environment are weak, as in low-temperature matrices, both molecules exist only in the amino-thiol forms 26a, while in the crystalline phase the amino-thione forms 26b predominate. In this work the observed IR absorption bands in the spectra were assigned to the theoretically calculated normal modes. These ab initio calculations were carried out at the HF/6-31G(d,p) level. [Pg.1385]

IR transmission spectra (T) of the thin polycrystalline specimens or powders were measured using IR microscope of the Fourier-spectrometer at room temperature in the spectral range of 600 5,000 cm-1. Optical absorption spectra were calculated as -ln(T). Figure 11.11 demonstrates normalized absorption spectra of fulleranes C60Hx with x = 36, 42, 48 and 60 together with the well known spectrum of fullerit... [Pg.244]

Figure 22. (a, b) Normalized absorption versus normalized frequency. Calculation for the hat-... [Pg.170]

Figure 31. Normalized absorption versus normalized frequency. Solid curve Calculation for the parameters of the hat-curved model typical for liquid D20 (these parameters are presented in Table XIII, lower line.) Dashed curve The lifetime Tvib becomes two times longer, other parameters remain the same. Dashed-and-dotted curve Calculation, when s becomes two times larger, other parameters remain the same. Figure 31. Normalized absorption versus normalized frequency. Solid curve Calculation for the parameters of the hat-curved model typical for liquid D20 (these parameters are presented in Table XIII, lower line.) Dashed curve The lifetime Tvib becomes two times longer, other parameters remain the same. Dashed-and-dotted curve Calculation, when s becomes two times larger, other parameters remain the same.
Figure 3-10. (Normalized) experimental (PAdU) and calculated (PAUMe) absorption and emission spectra in MeCN. Dashed line experimental absorption dash-dot experimental emission. Solid line calculated absorption dotted line experimental emission... Figure 3-10. (Normalized) experimental (PAdU) and calculated (PAUMe) absorption and emission spectra in MeCN. Dashed line experimental absorption dash-dot experimental emission. Solid line calculated absorption dotted line experimental emission...
Figure 13. Calculated normalized refractive index change produced by the dimerization of anthracene, and of various other compounds, as functions of wavelength. Molecular structures, absorption spectra, and further details are given in ref. 28. Figure 13. Calculated normalized refractive index change produced by the dimerization of anthracene, and of various other compounds, as functions of wavelength. Molecular structures, absorption spectra, and further details are given in ref. 28.
As predicted by the calculation, the absorption features of the P-polarised spectrum (coupling to Pt) correspond to the transmission features of the S polarised spectrum, and also correspond to the expectation values for the assigned modes of the bulk crystalline material [56]. The transmission features of the P-polarised spectrum (coupling to Pn) correspond to the blue shifted bands associated with a net dipole coupling of the normal components of the dynamic dipoles in a thin film. [Pg.528]

Thus the aim of a good CD model is to define the chromophores in such a way that, ideally, (i) a single perturbation term dominates, and (ii) the quantities appearing in this term may be calculated realistically or determined empirically (e.g. from the normal absorption spectrum). [Pg.74]

Let us consider now the number of additional ideal stages required in the rectifying section (NR) to achieve the desired distillate concentration xD - 0.001. This portion of the column behaves like a water absorber with very dilute solutions of water in methanol. From the construction in Figure 6.18, the vapor entering the absorber contains 2.3 mol% water (97.7 mol% methanol), while the vapor leaving it contains only 0.1 mol% water. The liquid entering it has a concentration x = xD = 0.001. To calculate the absorption factor for the absorber, we must estimate the slope of the equilibrium curve in the limit as xg tends to zero (mab)- In that portion of the column, the temperature is very close to the normal boiling point of pure methanol then Tab = 337.7 K. From the modified form of Raoult s law,... [Pg.350]

First, the ratio is constructed from the spectra at each rotation angle a or tilt angle / with the help of the linear correlation analysis (K. Fahmy, personal communication) A(a)/A(o=0) [A(/ )/A(/ =0)]. The ratio of each transition moment as a function of the angle a or can thus be obtained. This theoretical function can be calculated with the help of the Jones Formalism (4) and this function is necessary for fitting the ratios at o=90 and 0=90 degrees to obtain the dichroic ratio Ax/Ay and Ay/Az. Finally the normalized absorption axes can be determined. [Pg.1080]

If the amplitude of the amplifier output is normalized to unity, then this signal represents the sample absorption in per cent. If, furthermore, the amplifier has a logarithmic response (so-called balanced detectors are such devices), then the signal output is ln(/ //o), or log(/i//o), and thus is directly proportional to the absorbance A (see Equations (6.1) and (6.2)). Thus, an unknown absorber particle density N can easily be derived from the signal, provided the absorption cross-section a is known. Alternatively, one can calculate the absorption cross-section if the absorber particle density is predetermined. [Pg.93]

Fig. 4.5 a Normalized absorption spectra of BDOPV in CHCI3 (1 x 10 M, dashed line) and BDPPV in CHCI3 (1 X 10 M), in film and in annealed film solid line), b Cyclic voltammograms of BDOPV in DCB solution (5 mg/mL) and BDPPV in drop-casted film, c Calculated molecular orbitals of the trimers of BDPPV and PPV (B3LYP/6-311G(d,p)). Both trimers display similar frontier orbital distributions as indicated by the color boxes... [Pg.96]

Calculated from the intersection of the normalized absorption and fluorescence spectra. In toluene. [Pg.43]

Fig. 7. Changes in the difference spectra of whole cells of C. reinhardi y-1 mutant during growth in the dark. The curves were calculated from absorption spectra after normalization to equal amounts of chlorophyll. (For experimental details see ref. 38.)... Fig. 7. Changes in the difference spectra of whole cells of C. reinhardi y-1 mutant during growth in the dark. The curves were calculated from absorption spectra after normalization to equal amounts of chlorophyll. (For experimental details see ref. 38.)...
One type of single point calculation, that of calculating vibrational properties, is distinguished as a vibrations calculation in HyperChem. A vibrations calculation predicts fundamental vibrational frequencies, infrared absorption intensities, and normal modes for a geometry optimized molecular structure. [Pg.16]

Nonisothermal Gas Absorption. The computation of nonisothermal gas absorption processes is difficult because of all the interactions involved as described for packed columns. A computer is normally required for the enormous number of plate calculations necessary to estabUsh the correct concentration and temperature profiles through the tower. Suitable algorithms have been developed (46,105) and nonisothermal gas absorption in plate columns has been studied experimentally and the measured profiles compared to the calculated results (47,106). Figure 27 shows a typical Hquid temperature profile observed in an adiabatic bubble plate absorber (107). The close agreement between the calculated and observed profiles was obtained without adjusting parameters. The plate efficiencies required for the calculations were measured independendy on a single exact copy of the bubble cap plates installed in the five-tray absorber. [Pg.42]

ASTM E1050-90 also makes use of a tube with a test specimen at one end and a loudspeaker at the other end, but iastead of a single movable microphone there are two microphones at fixed locations ia the tube. The signals from these microphones are processed by a digital frequency analysis system which calculates the standing wave pattern and the normal iacidence sound-absorption coefficients. [Pg.312]

The percentage markup on cost is calculated for a known capital-turnover ratio and a desired rate of return on capital. As with absorption pricing, the percentage markup on manufac turing cost per unit of prodlic tion is calculated for a normal annual produc tion rate. If this produc tion rate is exceeded, the rate of return on capital will be higher than projected because of the decrease in unit cost. Conversely, if the... [Pg.856]

In gas absorption, the new phase consists of an inert nonvolatile solvent (absorption) or an inert nonsoluble gas (stripping), and normally no reflux is involved. The following paragraphs discuss some of the considerations peculiar to gas-absorption calculations for plate towers and some of the approximate design methods that can be employed when simplifying assumptions are vahd. [Pg.1357]

In concentrated wstems the change in gas aud liquid flow rates within the tower and the heat effects accompanying the absorption of all the components must be considered. A trial-aud-error calculation from one theoretical stage to the next usually is required if accurate results are to be obtained, aud in such cases calculation procedures similar to those described in Sec. 13 normally are employed. A computer procedure for multicomponent adiabatic absorber design has been described by Feiutnch aud Treybal [Jnd. Eng. Chem. Process Des. Dev., 17, 505 (1978)]. Also see Holland, Fundamentals and Modeling of Separation Processes, Prentice Hall, Englewood Cliffs, N.J., 1975. [Pg.1361]


See other pages where Calculated normalized absorption is mentioned: [Pg.292]    [Pg.84]    [Pg.235]    [Pg.183]    [Pg.292]    [Pg.175]    [Pg.16]    [Pg.292]    [Pg.108]    [Pg.322]    [Pg.76]    [Pg.110]    [Pg.183]    [Pg.1080]    [Pg.4703]    [Pg.61]    [Pg.77]    [Pg.333]    [Pg.5]    [Pg.312]    [Pg.141]    [Pg.14]    [Pg.573]    [Pg.848]    [Pg.367]    [Pg.251]   


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