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Calibration dynamic methods

Analogously to the dynamic method, the energy equivalent of the calorimeter, k.Q, can be obtained by performing calibration experiments in the isothermal mode of operation, using electrically generated heat or the fusion of substances with well-known A us//. Recommendations for the calibration of the temperature scale of DSC instruments for isothermal operation have also been published [254,270]. [Pg.189]

In the dynamic method the powder is flushed with an inert gas during degassing, nitrogen is then adsorbed on the powder in a carrier of helium gas at Known relative pressure while the powder is in a container surrounded by liquid nitrogen. The changing concentration of nitrogen is measured by a calibrated conductivity cell so that the amount adsorbed can be determined. [Pg.1587]

Fig. 3. Data analysis performed by using MicroVigene (VigeneTech, Billerica, MA, USA) software program. Spot finding, regional and local background subtraction, and linear dynamic range finding are performed by the software program. Combined with the calibrator, this method provides for a reproducible and quantifiable value for every sample. Fig. 3. Data analysis performed by using MicroVigene (VigeneTech, Billerica, MA, USA) software program. Spot finding, regional and local background subtraction, and linear dynamic range finding are performed by the software program. Combined with the calibrator, this method provides for a reproducible and quantifiable value for every sample.
The so-called Shore hardnesses are measured differently for metals and plastics. With hard materials (metals), a scleroscope is used to measure the rebound of a small steel ball. This Shore hardness is thus measured by a dynamic method, which yields the rebound hardness (the impact elasticity of the rubber industry). Soft plastics, on the other hand, are tested with a Shore durometer. This measures the resistance to the penetration of the point of a cone through the contraction of a calibrated spring. The durometer thus works according to a static method, and yields the true Shore hardness as understood by the rubber industry. Like the Rockwell hardness, the Shore hardness is given in scale divisions. [Pg.457]

The T calibration curves therefore are valid only for fast transitions. Corrections by extrapolation towards 6=0 for sluggish transitions are less accurate and depend on the transition speeds. In the opinion of the authors it does not pay to derive calibration curves for sluggish transitions. In these cases accurate temperature determinations are less accurate if not impossible at all by using dynamic methods. [Pg.78]

As an example, the separation of a mixture of three polymers, PS, poly-n-butyl methacrylate and their copolymer, is shown in Figure 5.12. The slice from system 1 was injected into system 2, and the molecules in the slice were separated according to their composition. The effect of n-heptane content in the THF was critical. When the n-heptane content was 63.8%, three components, PBMA, P(S-MMA) and PS, were completely separated in this order, although PBMA and P(S-MMA) were not separated if the n-heptane content was 60%. These molecules have the same hydrodynamic volume in THF, but a different composition. A dynamic method of calibrating for composition utilizing a rapid scanning UV detector was developed and... [Pg.125]

Besides the determination of the time constant value, veiy important information is provided by observation of the course of the changes A(t) for the calorimeter as a thermally inertial object. When the changes Ind =f(t) are nonlinear during the initial period of the cooling or heating process, it is necessary to analyze whether application of the simple body heat balance equation to the calculations is correct. A nonlinear course of lad = f(t) means that the function A(t) f(t) is multiexponential. More precise equations expressing the relation between P(t) and T(t) should then be used. The calibration procedure presented here is not the only one used in the dynamic method. The literature on this subject... [Pg.113]

Table 1 Weight-average molecular weights obtained by GPC with PS calibration, light-scattering (static method) and GPC with light-scattering detector (dynamic method). Table 1 Weight-average molecular weights obtained by GPC with PS calibration, light-scattering (static method) and GPC with light-scattering detector (dynamic method).
In order to derive structural information from infrared frequencies, input is required from quantum chemical calculations at computational levels which match the experimental resolution. Experimentally, gas-phase conditions imply extremely low sample densities, requiring special techniques in order to acquire infrared data. Some of those techniques involve double resonance approaches which provide unique opportunities for isomer selective IR spectroscopy. This facet is among the advantages of gas-phase experiments, making it possible to follow certain properties, such as excited state dynamics, as a function of molecular structure. At the same time, the availability of gas-phase data provides opportunities to calibrate computational methods, force fields, and functionals. [Pg.272]

The linear dynamic range of this method is 0.1 p.gl to 100 J.gl i The method detection limit (MDE) depends on selected operating conditions and a calibration range. It is important to use high purity reagents in all determinations. [Pg.211]

A final practical note involves instrument intensity measurement calibrations. The intensity measurement is self-calibrating relative to the incident beam from the source. However, measurements typically have a dynamic range of 10 -10 , and care must be taken to insure the detection system is linear. A method of calibrating the scatterometer is to characterize a diffuse reflector having a known scattering characteristic. For example, a surface coated with BaS04 makes a nearly Lambertian scatterer, which has a BRDF of 1/Jt at all angles. [Pg.719]

In SEC, universal calibration is often utilized to characterize a molecular weight distribution. For a universal calibration curve, one must determine the product of log(intrinsic viscosity molecular weight), or log([7j] M). The universal calibration method originally described by Benoit et al. (9) employs the hydro-dynamic radius or volume, the product of [tj] M as the separation parameter. The calibration curves for a variety of polymers will converge toward a single curve when plotted as log([7j] M) versus elution volume (VJ, rather than plotted the conventional way as log(M) versus V, (5). Universal calibration behavior is highly dependent on the absence of any secondary separation effects. Most failures of universal calibration are normally due to the absence of a pure size exclusion mechanism. [Pg.565]

A common problem for both methods lies in the use of potentials that do not possess the correct net attractiveness. This can have the consequence that continuum feamres appear shifted in energy. In particular, there is evidence that the LB94 exchange-correlation potential currently used for the B-spline calculations, although possessing the correct asymptotic behavior for ion plus electron, is too attractive, and near threshold features can then disappear below the ionization threshold. An empirical correction can be made, offsetting the energy scale, but this can mean that dynamics within a few electronvolts of threshold get an inadequate description or are lost. There is limited scope to tune the Xa potential, principally by adjustment of the assumed a parameter, but for the B-spline method a preferable alternative for the future may well be use of the SAOP functional that also has correct asymptotic behavior, but appears to be better calibrated for such problems [79]. [Pg.297]

Sample preparation, injection, calibration, and data collection, must be automated for process analysis. Methods used for flow injection analysis (FLA) are also useful for reliable sampling for process LC systems.1 Dynamic dilution is a technique that is used extensively in FIA.13 In this technique, sample from a loop or slot of a valve is diluted as it is transferred to a HPLC injection valve for analysis. As the diluted sample plug passes through the HPLC valve it is switched and the sample is injected onto the HPLC column for separation. The sample transfer time typically is determined with a refractive index detector and valve switching, which can be controlled by an integrator or computer. The transfer time is very reproducible. Calibration is typically done by external standardization using normalization by response factor. Internal standardization has also been used. To detect upsets or for process optimization, absolute numbers are not always needed. An alternative to... [Pg.76]


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See also in sourсe #XX -- [ Pg.117 , Pg.118 ]




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