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Relative absorbance

An example of the results obtained in the form of a chromatoelectropherogram can be seen in Figure 9.6. The contour type data display showed the three variables that were studied, namely chromatographic elution time, electrophoretic migration time, and relative absorbance intensity. Peptides were cleanly resolved by using this two-dimensional method. Neither method alone could have separated the analytes under the same conditions. The most notable feature of this early system was that (presumably) all of the sample components from the first dimension were analyzed by the second dimension, which made this a truly comprehensive multidimensional technique. [Pg.205]

In similar fashion, we have plotted the spectrum of a third sample which contains 3 concentration units of Component I and none of Component 2. Of course, this spectrum also lies in the same direction from the origin as the first spectrum and at 3 times the distance. It is clear that, when we use this approach to plot the spectra of samples which contain only Component 1, each such spectrum must lie somewhere along a line extending from the origin of the data space in some unique direction that is determined by the relative absorbances of Component 1 at each of the wavelengths plotted. [Pg.82]

Several collaborating laboratories (usually five participating laboratories) test the proposed substance using a variety of techniques. The relative reactivity or relative absorbance of the impurities present in a substance must be checked when a nonspecific assay method is employed, e.g. by colorimetry or ultraviolet spectrophotometry. It is particularly important to quantify the impurities when a selective assay is employed. In such a case, it is best to examine the proposed substance by as many methods as practicable, including, where possible, absolute methods. For acidic and basic substances, titration with alkali or acid is simple but other reactions which are known to be stoichiometric may be used. Phase solubility analysis and differential scanning calorimetry may also be employed in certain cases. [Pg.183]

Figure 6. Relative absorbance of symmetric and asymmetric COO vibrations of 0.90 fim palladium acetate film on silicon as a function of 2 MeV He+ ion dose. Decrease in film thickness with dose also shown. Figure 6. Relative absorbance of symmetric and asymmetric COO vibrations of 0.90 fim palladium acetate film on silicon as a function of 2 MeV He+ ion dose. Decrease in film thickness with dose also shown.
Similarly, in Chapter 44, we have previously derived the absorbance noise and relative absorbance noise, and presented those as equations 44-24 and 44-77, respectively. [Pg.281]

Figure 48-19 Relative absorbance precision for Poisson-distributed detector noise. Figure 48-19 Relative absorbance precision for Poisson-distributed detector noise.
The resulting plot is presented in Figure 51-29. From the plot, and from examining the list of values from which the plot was made, there appears to be no shift in the transmittance corresponding to the optimum value of relative absorbance, as the reference reading varies. [Pg.320]

Figure 51-29 Relative absorbance noise for Poisson-distributed data, determined by numerical computation using equation 51-77. Figure 51-29b is an ordinate expansion of Figure 51-29a. (see Color Plate 18)... Figure 51-29 Relative absorbance noise for Poisson-distributed data, determined by numerical computation using equation 51-77. Figure 51-29b is an ordinate expansion of Figure 51-29a. (see Color Plate 18)...
In conformance with our regular pattern, we now derive the behavior of the relative absorbance noise for the low-noise case. Here we start with equation 52-100, the derivation of which is found in [9] ... [Pg.326]

Equation 52-149 presents a minor difficulty one that is easily resolved, however, so let us do so the difficulty actually arises in the step between equation 52-148 and 52-149, the taking of the square root of the variance to obtain the standard deviation conventionally we ordinarily take the positive square root. However, T takes values from zero to unity that is, it is always less than unity, the logarithm of a number less than unity is negative, hence under these circumstances the denominator of equation 52-149 would be negative, which would lead to a negative value of the standard deviation. But a standard deviation must always be positive clearly then, in this case we must use the negative square root of the variance to compute the standard deviation of the relative absorbance noise. [Pg.326]

In Figure 52-30 we plot the function -1 /ln(T) to complete this part of the analysis. We note that there is no minimum to the curve, and the noise from source continually improves as the transmittance decreases in this case the previous, conventional derivations agree with our results, although they do not indicate the V2 factor. Noting the transitions from equation 52-140 to 52-142 (and the corresponding portions of the derivation for absorbance noise and relative absorbance noise), we see that this factor arises from the equal noise contributions of the sample and reference channels therefore we conclude that in this case also, the missing factor is due to the neglect of the reference channel noise contribution. [Pg.326]

Fig. 8. Difference spectrum (green irradiated minus red irradiated) of phycochrome c (solid line), action spectrum for induction of filamentous growth of Nostoc muscorum (dotted line), and action spectrum for inhibition of C-phycoerythrin synthesis in Tolypothrix tenuis (dashed-dotted line). Abscissa wavelength in nm Ordinates relative absorbance change und relative action (after Bjorn and Bjorn 5))... Fig. 8. Difference spectrum (green irradiated minus red irradiated) of phycochrome c (solid line), action spectrum for induction of filamentous growth of Nostoc muscorum (dotted line), and action spectrum for inhibition of C-phycoerythrin synthesis in Tolypothrix tenuis (dashed-dotted line). Abscissa wavelength in nm Ordinates relative absorbance change und relative action (after Bjorn and Bjorn 5))...
The relative absorbance E3/4 to characterize the turbidity in the supernatant liquid. [Pg.368]

The relative absorbance E3/5 to characterize the variation in the sedimenting flocculated dispersion. [Pg.368]

Figure 2b. Relative absorbance as a function of thickness of the film. Relative absorbance (AR/R)/d values normalized to unity at the surface. (Reproduced with permission from Ref. 11. Copyright 1987 North Holland.)... Figure 2b. Relative absorbance as a function of thickness of the film. Relative absorbance (AR/R)/d values normalized to unity at the surface. (Reproduced with permission from Ref. 11. Copyright 1987 North Holland.)...
Fig. 2.114. RP-HPLC profiles of ACTs and SEC fractions (fr.) of ACTs. Each lyophilized sample was dissolved in water (1 mg/ml), and analysed by RP-HPLC. Upper chromatogram RP-HPLC profile of ACTs. Lower chromatograms with fraction numbers RP-HPLC profiles of SEC fractions of ACTs. The numbers of identified peaks in each chromatogram are (1) procyanidin B1 (PB1), (2) (+)-catechin, (3) procyanidin B2 (PB2), (4) procyanidin Cl (PCI), 5 (—)-epicatechin (EC). AU means relative absorbance units (at 280 nm). For details on the RP-HPLC conditions see text. Reprinted with permission from A. Yanagida et al. [253]. Fig. 2.114. RP-HPLC profiles of ACTs and SEC fractions (fr.) of ACTs. Each lyophilized sample was dissolved in water (1 mg/ml), and analysed by RP-HPLC. Upper chromatogram RP-HPLC profile of ACTs. Lower chromatograms with fraction numbers RP-HPLC profiles of SEC fractions of ACTs. The numbers of identified peaks in each chromatogram are (1) procyanidin B1 (PB1), (2) (+)-catechin, (3) procyanidin B2 (PB2), (4) procyanidin Cl (PCI), 5 (—)-epicatechin (EC). AU means relative absorbance units (at 280 nm). For details on the RP-HPLC conditions see text. Reprinted with permission from A. Yanagida et al. [253].
Selected ion monitoring GC/MS trace of the HFBA derivatives of nine neuroactive steroids found in human plasma. The separations were accomplished on a Restek Rtx-200 MS column. Relative absorbance was measured at negative Cl for m/z values of 474 (pregnanolones), 492 (pregnenolone), 664 (androstanediols), and 706 (pregnanediolones). (Everhart et al., unpublished)... [Pg.182]

The absorbance changes shown below occur for the reaction of the radicals with penta-ammine(histidine-33)ruthenium(III) ferricytochrome c, PFe "-Ru" (see (5.84)). The final product is PFe Ru ". Absorbance increases at 550 nm are largely as a result of the step PFe " PFe . Interpret the changes (particularly the relative absorbances associated with the very fast and slower absorbances). [Pg.296]

Figure 3. Relative absorbance of culture supernatant at 360 nm ( ) and 288 nm (o) vs. time after addition of quinone 13 to ligninolytic cultures of P. chrysosporium.. Figure 3. Relative absorbance of culture supernatant at 360 nm ( ) and 288 nm (o) vs. time after addition of quinone 13 to ligninolytic cultures of P. chrysosporium..
The FTIR spectrum of PS-MIPK is shown in Figure 4. Band A is the ketone carbonyl absorption at 1700 cm-1 and is used to monitor changes in photochemistry. Bands (1600 cm-1), C (1495 cm-1) and D (1455 cm-1) are well resolved bands from the styrene portion of the copolymer. Provided that they are not involved in the photochemistry, which seems unlikely, they can be used as a practical measure of film thickness. Measurements were made on the actual thickness of a number of PS and PS copolymer films using a Talley-step apparatus, followed by FTIR measurements. Based on these results, the relative absorbance values were found to be B, 2.56 C, 7.40 and D, 6.83 absorbance units per micron. The UV absorbance was also measured for films of various thickness at 254 nm, and the data are summarized in Table III. The constancy of these data suggests that this also could be used as a simple method of determination of film thickness. [Pg.393]

Measures of the sensitivity were made in two ways, (l) Loss of ketone carbonyl was determined by FTIR on the exposed samples by measuring the relative absorbance A at 1700 cm-1. The ratio (Aq/A))7oo, was adjusted for film thickness using the styrene bands at 1600, 1495, and 1455 cm-1. This value is proportional to the rates of the Norrish type I and photoreduction processes in the copolymer (2). Changes in molecular weight result from scission in the backbone of the polymer chain. A measure, Z, of the sensitivity to main-chain scission can be derived as follows. [Pg.396]

Melting temperatures (Tm) of DNA molecules with different nucleotide compositions. (At a wavelength of 260 nm, single-stranded DNA has a higher relative absorbance than does double-stranded DNA.)... [Pg.396]

Effect of temperature on the relative absorbance of native, renatured, and denatured DNA. When native DNA is heated in aqueous solution, its absorbance does not change until a temperature of about 80°C is reached, after which the absorbance rises sharply, by about 40%... [Pg.638]

The relative absorbance values obtained by these self-modeling procedures are proportional to concentrations of the components in the mixtures and are used as the first estimates for concentrations. The method of alternating least squares14 is then applied to the data. In this method, the mixture spectra in the absorbance matrix, A, are written in terms of Beer s law as... [Pg.112]


See other pages where Relative absorbance is mentioned: [Pg.371]    [Pg.253]    [Pg.313]    [Pg.320]    [Pg.320]    [Pg.324]    [Pg.538]    [Pg.538]    [Pg.112]    [Pg.359]    [Pg.243]    [Pg.529]    [Pg.214]    [Pg.126]    [Pg.153]    [Pg.240]    [Pg.23]    [Pg.395]    [Pg.83]    [Pg.327]   
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