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Measurement Steps

Adjust the thermistor probe in the cell lid so that one of the thermistors can be loaded only with solvent, while the second can receive either solvent or lignin solutions. [Pg.513]

Insert the vapor wicks in the glass solvent reservoir and introduce the solvent into the cell. [Pg.513]

Set the operating temperature the desired cell temperature should be in a range extending up to about 5 °C below the boiling temperature in order to prevent decomposition of the solvent or the sample. Table 8.3.1 lists the temperature generally employed with the usual lignin solvents. [Pg.513]

Prepare the syringes two syringes are filled with solvent and the others with sample solutions (lignins or calibrating compound). All are inserted into the head. [Pg.513]

Set the bridge to zero the zero balance is adjusted with solvent on both thermistors by means of a potentiometer. For good reproducibility, the drop size should remain as uniform as possible. [Pg.513]


That means, the derivation of the measured step response h(x) along the path x delivers the impulse response function g(x) of the system. [Pg.366]

Rheometric Scientific markets several devices designed for characterizing viscoelastic fluids. These instmments measure the response of a Hquid to sinusoidal oscillatory motion to determine dynamic viscosity as well as storage and loss moduH. The Rheometric Scientific line includes a fluids spectrometer (RFS-II), a dynamic spectrometer (RDS-7700 series II), and a mechanical spectrometer (RMS-800). The fluids spectrometer is designed for fairly low viscosity materials. The dynamic spectrometer can be used to test soHds, melts, and Hquids at frequencies from 10 to 500 rad/s and as a function of strain ampHtude and temperature. It is a stripped down version of the extremely versatile mechanical spectrometer, which is both a dynamic viscometer and a dynamic mechanical testing device. The RMS-800 can carry out measurements under rotational shear, oscillatory shear, torsional motion, and tension compression, as well as normal stress measurements. Step strain, creep, and creep recovery modes are also available. It is used on a wide range of materials, including adhesives, pastes, mbber, and plastics. [Pg.202]

On silicon carbide, it is easier to see and measure step heights than in crystals like beryl, because SiC has polytypes, first discovered by the German crystallog-rapher Baumhauer (1912). The crystal structure is built up of a succession of close-packed layers of identical structure, but stacked on top of each other in alternative ways (Figure 3.24). The simplest kind of SiC simply repeats steps ABCABC, etc., and the step height corresponds to three layers only. Many other stacking sequences... [Pg.119]

Essentially, stripping analysis is a two-step technique. The first, or deposition, step involves die electrolytic deposition of a small portion of the metal ions hi solution into die mercury electrode to preconcentrate the metals. This is followed by die shipping step (the measurement step), which involves die dissolution (shipping) of die deposit. Different versions of stripping analysis can be employed, depending upon die nature of the deposition and measurement steps. [Pg.76]

Several solid surfaces, such as filter paper, sodium acetate, and silica gel chromatoplates with a polyacrylate binder, have been used in solid-surface luminescence work (1,2). Experimentally it is relatively easy to prepare samples for analysis. With filter paper, for example, a small volume of sample solution is spotted onto the surface, the filter paper is dried, and then the measurement is made. In many cases, an inert gas is passed over the surface during the measurement step to enhance the RTF signal. For powdered samples, the sample preparation procedure is somewhat more involved. Commercial instruments can be readily used to measure the luminescence signals, and a variety of research instruments have been developed to obtain the solid-surface luminescence data (1,2). [Pg.157]

Following RM certificate instructions for material usage and handling, incorporate the RM into the scheme of analysis at the earliest stage possible, i.e. prior to the beginning of sample decomposition. Take it through the entire analytical procedure at the same time and under the identical conditions as the actual analytical samples in order to correctly monitor all the sample manipulation and measurement steps. [Pg.217]

Finally, a more subtle distinction lies in the manner in which the measurement step is carried out. This is accomplished in chromatographic methods by the... [Pg.720]

Figure 23 Calculation of the shape of the actively compensated pulse can be carried out on the software. (A) shows the real (red line) and the imaginary (green line) component of an example of the target pulse shape t>,(f). Its leading and the trailing edges have a cosine shape with a transition time of 1.25 xs in 50 steps, and the width of the plateau is 5 ps. (B) Laplace transformation B(s) multiplied by the Laplace transformed step function U(s). (C) It was then divided by the Laplace transformation Y(s) of the measured step response y(t) of the proton channel of a 3.2-mm Varian T3 probe tuned at 400.244 MHz to obtain V(s). (D) Finally, inverse Laplace transformation was performed on V(s) to obtain the compensated pulse that results in the RF pulse with the target shape. Time resolution was 25 ns, and o = 20 was used for the Laplace and inverse Laplace transformations. Figure 23 Calculation of the shape of the actively compensated pulse can be carried out on the software. (A) shows the real (red line) and the imaginary (green line) component of an example of the target pulse shape t>,(f). Its leading and the trailing edges have a cosine shape with a transition time of 1.25 xs in 50 steps, and the width of the plateau is 5 ps. (B) Laplace transformation B(s) multiplied by the Laplace transformed step function U(s). (C) It was then divided by the Laplace transformation Y(s) of the measured step response y(t) of the proton channel of a 3.2-mm Varian T3 probe tuned at 400.244 MHz to obtain V(s). (D) Finally, inverse Laplace transformation was performed on V(s) to obtain the compensated pulse that results in the RF pulse with the target shape. Time resolution was 25 ns, and o = 20 was used for the Laplace and inverse Laplace transformations.
In this paper we will first describe a fast-response infrared reactor system which is capable of operating at high temperatures and pressures. We will discuss the reactor cell, the feed system which allows concentration step changes or cycling, and the modifications necessary for converting a commercial infrared spectrophotometer to a high-speed instrument. This modified infrared spectroscopic reactor system was then used to study the dynamics of CO adsorption and desorption over a Pt-alumina catalyst at 723 K (450°C). The measured step responses were analyzed using a transient model which accounts for the kinetics of CO adsorption and desorption, extra- and intrapellet diffusion resistances, surface accumulation of CO, and the dynamics of the infrared cell. Finally, we will briefly discuss some of the transient response (i.e., step and cycled) characteristics of the catalyst under reaction conditions (i.e.,... [Pg.80]

The basic calibration of a method only covers the final measurement step without any preceding sample preparation. Pure analytical standard solutions are used here. Of course this does not cover the whole analytical process. So method characteristics for the basic calibration are not transferable to the whole analytical process. During validation the influence of other matrix constituents has to be investigated. [Pg.187]

With the Basic Caiibration oniy the measurement step itseif is caiibrated... [Pg.187]

Most analytical procedures do not consist of a physical measurement step only, but may inelude ehemical sample preparation steps. In addition there might be some substanees present that interfere with our measurements and other constituents (the matrix) may influence the sensitivity of the method. [Pg.194]

If all the samples that ate analysed have the same matrix, the sample preparation should be included in the control procedure. If the matrix changes very often, it could be useful to hmit the procedure to the measurement step only. [Pg.287]

The relative lifetimes of the two terraee types at any one saddle point location has been measured[31] to differ by a factor of 6 at 1060C. The change in terrace type occurs by the bridging of the short dimension by step fluctuations. Since the probability of a fluctuation of a particular amplitude depends linearly on the step stiffness[8] the observed lifetime ratio is consistent with measured step stiffnesses[37] and the geometrical picture given above[38]. [Pg.35]

Successful development and implementation of various chemical sensors for ocean measurements (based on optical, electrochemical, or mass transducers) requires concomitant advances in the design or discovery of organic or inorganic molecules that interact selectively with the important ocean analytes. These developments are particularly important for in situ sensors where no separation of ocean components or addition of external reagents occurs before or during the measurement step. [Pg.69]

For accurate quantification, it is essential that the glucose standard be equilibrated to room temperature before an aliquot is taken for measurement (step 16), and that aliquots be taken using the most accurate pipetting techniques. For further details, see Critical Parameters and Troubleshooting for discussions on glucose standards and pipetting technique. [Pg.748]

High-performance LC is widely used, offline or online, in the determination of pesticides, either as a final measurement step or as a separation technique. The increase in the use of HPLC is mainly the result, on the one hand, of its suitability for determining thermally labile and polar pesticides that require derivatization prior to GC, and, on the other, of its compatibility with online precolumn extraction and cleanup and with MS systems (19). [Pg.718]

As already indicated, catalytic titrations are carried out by monitoring conversion of a model reactant while the surface concentration of adsorbed reagent (usually an amine) is increased in measured steps. Conversion of the reactant is determined by means of a pulse reactor or a conventional flow reactor, depending on the needs of the investigator. In order to obtain the most meaningful titration results, we make the following recommendations. [Pg.119]

For the simultaneous detection of sodium dithionite, sulphite and indigo, a multistep amperometric method was worked out and optimised, as outlined in Table 6.4. It is clear that after each measuring step, the electrode surface should be cleaned to remove indigo that is oxidised at all applied... [Pg.190]

The stripping voltammogram, recorded during this measurement step, consists of multiple current peaks, corresponding to the reoxidation of the amalgamated metals, and their stripping out of the electrode. Such output provides the qualitative and quantitative information through measurements of the peak potential and current,... [Pg.133]

Fig. 23.5. Schematic representation of the MIP-SPCE sensor device and the measurement steps. NIP non-imprinted polymer (control). Reproduced from Ref. [160] by permission of Wiley-VCH Verlag GmbH Co. Fig. 23.5. Schematic representation of the MIP-SPCE sensor device and the measurement steps. NIP non-imprinted polymer (control). Reproduced from Ref. [160] by permission of Wiley-VCH Verlag GmbH Co.
A software tool for the handheld LAPS set-up can be created by, e.g., the programming language Lab VIEW from National Instruments. The software should provide all necessary measurement steps that are required during a complete measurement cycle ... [Pg.1007]

Batch-mode operation, with a detection limit of around 5ng/mL, is suitable for oestrus prediction and by using chronoamperometry as the measurement step, gives a result in around 40 min with simple instrumentation. The chronoamperometric approach does have the disadvantage of requiring the use of a blank measurement to cater for... [Pg.1191]

The final measurement step can be done in a number of ways. [Pg.371]

Martinotti, W., Queirazza, G., Guarinoni, A. and Mori, G. (1995) In-flow speciation of copper, zinc, lead and cadmium in fresh waters by square wave anodic stripping voltammetry Part II. Optimization of measurement step. Anal. Chim. Acta, 305, 183-191. [Pg.228]

Analysis is a lot more complex than the measurement process alone. The measurement step is often the best understood step in the overall analytical process. Error sources are largely situated outside the direct measurement step (Examples 2-4). [Pg.42]


See other pages where Measurement Steps is mentioned: [Pg.366]    [Pg.261]    [Pg.720]    [Pg.119]    [Pg.291]    [Pg.171]    [Pg.718]    [Pg.674]    [Pg.265]    [Pg.418]    [Pg.145]    [Pg.261]    [Pg.229]    [Pg.92]    [Pg.273]    [Pg.523]    [Pg.524]    [Pg.540]    [Pg.895]    [Pg.363]    [Pg.33]    [Pg.432]    [Pg.82]   


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