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Sample absorption

The absorption sample is mounted in the standard filter holder located between the monochromator crystal and the geiger-counter receiving slit. Pertinent distances are as follows target to quartz ciystal, 17 cm. quartz crystal to receiving slit, 17 cm. absorption sample to receiving slit, 6 cm. [Pg.155]

Values reported were converted to percent absorption. Sample mixed 1 min. [Pg.184]

Fig. 13. Measured scattering intensity of HDPE melt. Intensity corrections for air scattering, polarization, absorption, sample geometry and Compton scattering have beat performed... Fig. 13. Measured scattering intensity of HDPE melt. Intensity corrections for air scattering, polarization, absorption, sample geometry and Compton scattering have beat performed...
Atomic absorption sample is vaporized and atomized in high temperature flame. Atoms of the analyte element absorb light of a specific wavelength from a hollow cathode lamp, passing through the flame. Amount of energy absorbed by these atoms is measured, which is proportional to the number of atoms in the light path. Components lamp, flame, monochromator, and detector. [Pg.432]

The lowest concentration of herbicide detectable in the atmosphere depends on the sample volume and the collection time. For an absorption sample volume of 5.0 ml. n-decane and a collection time of 24 hours, the lowest detectable atmospheric concentration is 1.0 /xgram/cu. meter for methyl MCP, 0.14 /xgram/cu. meter for the 2,4-D esters, and 0.03 /xgram/cu. meter for methyl 2,4,5-T. [Pg.229]

Atomic absorption sample preparation procedures applied to archaeological samples can be streamlined. Important factors include sample preparation, sample size, sample decomposition, standards, instrumentation, and practical and conceptual applications of atomic absorption analysis. On a comparative basis the sample preparation procedure reported was convenient and rapid the AAS instrumentation proved to be flexible, sensitive, rapid, and inexpensive in the analysis of archaeological materials. [Pg.258]

In bioavailability studies, the shape of and the area under the plasma concentration versus time curves are mostly used to assess rate t and extent (AUC) of absorption. Sampling points or periods should be chosen such that the concentration versus time profile is adequately defined to allow calculation of relevant parameters. For single-dose studies, the following parameters should be measured or calculated ... [Pg.366]

FIGURE 1.3 The air filter-absorption sampling system for semivolatile organic pollutants in ambient air. [Pg.16]

We utilized two sampling methods combined with gas chromatography-mass spectrometry (GC-MS) to identify urinary compounds. Our adsorption and absorption sampling and capture techniques allowed us to encompass a substantial molecular weight (MW) range. We spanned in a somewhat selective manner fix)m small compounds such as acetaldehyde (MW = 44) and trimethylamine (MW = 59) up to large ones such as steroids (MW over 300). For the more volatile compounds, evacuated canister capture... [Pg.129]

FIGURE 10-12. Perkin-Elmer atomic absorption sample cell showing nebulizing chamber and burner. [Courtesy the Perkin-Elmer Corp.]... [Pg.260]

Flame temperatures and fuel-to-oxidant ratios are two of the most important parameters to consider when using a flame as an atomic absorption sample cell. Table 10-2 lists maximum temperatures attainable with various combinations of fuel and oxidant. [Pg.266]

Fig.2. Absorption changes at 548 nm during a sequence of saturating flashes (210 ms apart). Anaerobic, untreated S-30 cells. The dots (shown on a few flashes for clarity) indicate absorption sampling at 3, 20, 50, 200 ms after each flash. 1 no addition. 2 addition of 10 pM myxothiazol. Notice that the 3 ms point after each flash is about half-way down in curve 2, whereas it is close to the peak of the truncated transient in curve 1. Fig.2. Absorption changes at 548 nm during a sequence of saturating flashes (210 ms apart). Anaerobic, untreated S-30 cells. The dots (shown on a few flashes for clarity) indicate absorption sampling at 3, 20, 50, 200 ms after each flash. 1 no addition. 2 addition of 10 pM myxothiazol. Notice that the 3 ms point after each flash is about half-way down in curve 2, whereas it is close to the peak of the truncated transient in curve 1.
In general, for samples with high UV absorptivity, sample concentrations greater than 10 Mg/ml will yield reasonable signals using hydrodynamic injections, irrespec-... [Pg.409]

Y.L. Wei, M. Oshima, J. Simon, S. Motomizu, The application of the chromatomembrane cell for the absorptive sampling of nitrogen dioxide followed by continuous determination of nitrite using a micro-flow injection system, Talanta 57 (2002) 355-364. [Pg.243]

Fig.4. Test of cooling correction with a 2 mm sample cell in absorption. Sample cavity 2x8x9mm, conical windows with diameter 6xl2mm, length 12mm. - Tris-buffer Cresol Red system at pH8.2... Fig.4. Test of cooling correction with a 2 mm sample cell in absorption. Sample cavity 2x8x9mm, conical windows with diameter 6xl2mm, length 12mm. - Tris-buffer Cresol Red system at pH8.2...
In Chapter 8, we characterized the strengths of one-photon transitions in terms of Einstein coefficients and oscillator strengths. According to Beer s law, a weak light beam with incident intensity 7o will emerge from an absorptive sample of concentration C and path length I with diminished intensity I = Iq exp(—aC/), where a is the molar absorption coefficient. Beer s law can be recast in the form... [Pg.326]

Figure 9.25 shows for typical samples the maximum efficiency y(0o) = as a function of the exposure. These growth curves show that an optimum can be reached between 0.5 and 1.0 J/cm for = 308 nm and between 5 and 10 J/cm for = 325 nm. For TS6 the penetration depth at 308 nm is about 110 pm, whereas at 325 nm it is about 420 pm. This difference and in addition a presumably lower quantum yield at 325 nm results in much slower growth curves for this wavelength. The decrease in efficiency is not only an effect of coupling back intensity from first to zeroth order, but also produced by an increase of absorption. Sample quality and thickness can influence these curves. A destruction of the surface is only observed if the optimal exposure is exceeded by a factor 2 to 3. This is due to the lattice mismatch of monomer and polymer stacking distance. [Pg.149]


See other pages where Sample absorption is mentioned: [Pg.388]    [Pg.148]    [Pg.31]    [Pg.49]    [Pg.6524]    [Pg.181]    [Pg.291]    [Pg.245]    [Pg.6523]    [Pg.396]    [Pg.772]    [Pg.321]    [Pg.53]    [Pg.94]    [Pg.440]    [Pg.241]    [Pg.241]    [Pg.178]    [Pg.957]    [Pg.1064]    [Pg.172]    [Pg.4]    [Pg.193]   
See also in sourсe #XX -- [ Pg.379 ]




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Absorption by a sample

Absorption of moisture by the sample

Absorption within sample, correction

Atomic absorption spectrometry liquid samples

Atomic absorption spectrometry sample preparation

Atomic absorption spectrometry sample vaporization

Atomic absorption spectrometry solid samples

Atomic absorption spectrometry solid sampling

Calculations Absorption Factor, Optimum Sample Thickness

Experiment 29 Quantitative Flame Atomic Absorption Analysis of a Prepared Sample

Experiment 31 The Analysis of Soil Samples for Iron Using Atomic Absorption

Near infrared absorption spectroscopy sampling

Reflection---Absorption Sampling Technique

Sample atomic absorption spectrometry

Sample flame atomic absorption spectrometry

Sample preservation absorption

Slurry sampling-electrothermal atomic absorption spectrometry

Solid sampling Zeeman atomic absorption spectrometry

Thick samples, nonlinear absorption

Thick samples, nonlinear absorption measurements

Thin samples, nonlinear absorption

Wavelength dependence sample absorption

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