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Measurement geometry effects

Such effects principally cannot be observed in multi band detectors such as a UV diode array detector or a Fourier transform infrared (FTIR) detector because all wavelengths are measured under the same geometry. For all other types of detectors, in principle, it is not possible to totally remove these effects of the laminar flow. Experiments and theoretical calculations show (8) that these disturbances can only be diminished by lowering the concentration gradient per volume unit in the effluent, which means that larger column diameters are essential for multiple detection or that narrow-bore columns are unsuitable for detector combinations. Disregarding these limitations can lead to serious misinterpretations of GPC results of multiple detector measurements. Such effects are a justification for thick columns of 8-10 mm diameter. [Pg.441]

Fig. 3.19 Schematic illustration of the measurement geometry for Mossbauer spectrometers. In transmission geometry, the absorber (sample) is between the nuclear source of 14.4 keV y-rays (normally Co/Rh) and the detector. The peaks are negative features and the absorber should be thin with respect to absorption of the y-rays to minimize nonlinear effects. In emission (backscatter) Mossbauer spectroscopy, the radiation source and detector are on the same side of the sample. The peaks are positive features, corresponding to recoilless emission of 14.4 keV y-rays and conversion X-rays and electrons. For both measurement geometries Mossbauer spectra are counts per channel as a function of the Doppler velocity (normally in units of mm s relative to the mid-point of the spectrum of a-Fe in the case of Fe Mossbauer spectroscopy). MIMOS II operates in backscattering geometry circle), but the internal reference channel works in transmission mode... Fig. 3.19 Schematic illustration of the measurement geometry for Mossbauer spectrometers. In transmission geometry, the absorber (sample) is between the nuclear source of 14.4 keV y-rays (normally Co/Rh) and the detector. The peaks are negative features and the absorber should be thin with respect to absorption of the y-rays to minimize nonlinear effects. In emission (backscatter) Mossbauer spectroscopy, the radiation source and detector are on the same side of the sample. The peaks are positive features, corresponding to recoilless emission of 14.4 keV y-rays and conversion X-rays and electrons. For both measurement geometries Mossbauer spectra are counts per channel as a function of the Doppler velocity (normally in units of mm s relative to the mid-point of the spectrum of a-Fe in the case of Fe Mossbauer spectroscopy). MIMOS II operates in backscattering geometry circle), but the internal reference channel works in transmission mode...
Coefficient of variation for dust (dry assay) and dust (wet assay) was 8.5 and 8.7%, respectively. The range of trash contents is about 50 compared to about four for dust content. As explained by Montalvo (12). differences in dust content by the dry and wet assay methods are a result of a geometry effect associated with the former technique and the variation of adhesion force of dust on cotton with environment. Only one airborne dust measurement was taken on five of the six cottons. [Pg.73]

For large n, almost all volume of the simplex is concentrated in a small neighborhood of its center and this effect is an example of measure concentration effects that play important role in modem geometry and analysis (Gromov, 1999). All Si are identically distributed, and for normalized variable s — Si/ b — a)... [Pg.117]

The raw data from a tensile test are the load versus elongation measurements made by the load cell and the extensometer, respectively. To eliminate sample geometry effects, the extension is divided by the initial length to obtain the dimensionless strain (which is occasionally multiplied by 100 and reported as % elongation for samples... [Pg.408]

Four-Probe Method. If two electrodes are used to probe the resistance of a sample, as shown in Fig. 8.1a, then the resistances of the wires and contacts on both sides are additive and may mask the intrinsic resistance of the sample itself (divorced from the contact resistances). If the sample is long enough, then the four-probe method described in Fig. 8.1c will eliminate the contact resistances A constant current I is passed between electrodes 1 and 4, and the voltage drop V across electrodes 2 and 3 is measured the resistance, after due corrections for geometry effects, is given by Ohm s law. [Pg.446]

Capillary rheometers measure the effect of pressure on volumetric flow through a cylindrical capillary. They are popular in practical work because shear rate and flow geometry are similar to conditions in extrusion and injection molding. They cover a wide range of shear... [Pg.668]

From this discussion it follows that all conclusions drawn for isotropic catalyst pellets hold for anisotropic catalyst pellets as well. In fact, with a single catalyst geometry, it is not possible to distinguish between isotropic and anisotropic pellets. The effect of anisotropy is lumped in with the effective diffusion coefficient. If the catalyst pellet is isotropic, then from Equation 7.128 it follows that we measure the effective diffusion coefficient D / = D J = D. For anisotropic pellets, we measure for pellets with a large height (0 large) and D H for flat pellets (0 small). For intermediate values of 0 the value of DeA is between De/iR and D H. [Pg.172]

It should be realized that hydrodynamic techniques measure an effective thickness obtained by comparing the tangential flow along a polymer-covered surface with that along a bare surface. The effective thickness thus found is usually called the hydrodynamic layer thickness. The exact shape of the flow velocity profile is Important, and this depends on the shape of the surface in question, and on its orientation with respect to the flow field. Detailed data Interpretation is therefore only possible if simple geometries are chosen such as smooth cylindrical channels or spherical colloidal particles. [Pg.672]

Figure 1. Particleboard elution by dry nitrogen sample geometry effects (o shredded 1.0 NCM. A A 25x25x16 mm 0.5 NCM duplicate runs. P = Perforator value in mg/100 g dry board/measured on starting material at " 6 pet moisture content.) (ML85 5428)... Figure 1. Particleboard elution by dry nitrogen sample geometry effects (o shredded 1.0 NCM. A A 25x25x16 mm 0.5 NCM duplicate runs. P = Perforator value in mg/100 g dry board/measured on starting material at " 6 pet moisture content.) (ML85 5428)...
The most common geometry used for the determination of the cure viscosity is that of the parallel-plate rheometer (Martin et al. 1989, Hale et al. 1989, Sundstrom and Burkett, 1981, Kojima et al. 1986, Pahl and Hesekamp, 1993, Ryan and Kamal, 1976, Ng and Manas-Zloczower, 1993, Nguyen, 1993, Peters et al. 1993, Kenny et al. 1991, Choi and Lin, 1991, Halley et al. 1994). This rheometer may be operated at low shear rates under isothermal and non-isothermal conditions. Alternative measurements have been used to measure the effects of cure on the viscosity, and these are summarized in Table 4.6. [Pg.343]

Studies Based on Molecular Mechanics Theory. - Amino-imino tautomerism in thiazolium-substituted alkylidene-l,l-bisphosphonic acids (11) has been studied by spectroscopy and pKa measurements. The effects of pH, steric and electronic effects on the conversion of amino to imino tautomers (and on the spectra) have been confirmed by molecular mechanics calculations of their optimised molecular geometries and PPP spectra. ... [Pg.330]

Moreover, the calculation of 7 " can be partitioned into several contributions for studies in vacuo the partition is generally done in terms of electronic and vibrational contributions. Here we consider it convenient to make reference to the in vacuo case, adding a further term, the geometry relaxation contribution, measuring the effects on the electronic polarizability due to the changes in the equilibrium geometry induced by the solvent. [Pg.250]

Figure 3.16. Electroclinic effect in ferroelectric LCEs (a) Chemical structure of sample, (b) Measurement geometry the beam in the interferometer passes twice through the film to measure the electrically induced thickness modulation, (c) The viewing angle is turned by 90° around the layer normal compared with that in (b). Source Lehmann et al., 2001. Figure 3.16. Electroclinic effect in ferroelectric LCEs (a) Chemical structure of sample, (b) Measurement geometry the beam in the interferometer passes twice through the film to measure the electrically induced thickness modulation, (c) The viewing angle is turned by 90° around the layer normal compared with that in (b). Source Lehmann et al., 2001.
The main sources of error in the concentric cylinder type measuring geometry arise from end effects (see above), wall shp, inertia and secondary flows, viscous heating effects and eccentricities due to misahgnment of the geometry [Macosko, 1994],... [Pg.44]


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See also in sourсe #XX -- [ Pg.267 ]




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