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Experimental procedure density measurements

The problem of an exact definition of hardness, and a valid experimental procedure to measure it, was solved for me in 1983. Bob Parr, the well-known theoretician, spent a sabbatical quarter in Santa Barbara. He had already used density functional theory to define the electronic chemical potential,... [Pg.309]

The sohd line in Figure 3 represents the potential vs the measured (or the appHed) current density. Measured or appHed current is the current actually measured in an external circuit ie, the amount of external current that must be appHed to the electrode in order to move the potential to each desired point. The corrosion potential and corrosion current density can also be deterrnined from the potential vs measured current behavior, which is referred to as polarization curve rather than an Evans diagram, by extrapolation of either or both the anodic or cathodic portion of the curve. This latter procedure does not require specific knowledge of the equiHbrium potentials, exchange current densities, and Tafel slope values of the specific reactions involved. Thus Evans diagrams, constmcted from information contained in the Hterature, and polarization curves, generated by experimentation, can be used to predict and analyze uniform and other forms of corrosion. Further treatment of these subjects can be found elsewhere (1—3,6,18). [Pg.277]

It is appropriate at this point to briefly discuss the experimental procedures used to determine polymerization rates for both step and radical chain polymerizations. Rp can be experimentally followed by measuring the change in any property that differs for the monomer(s) and polymer, for example, solubility, density, refractive index, and spectral absorption [Collins et al., 1973 Giz et al., 2001 McCaffery, 1970 Stickler, 1987 Yamazoe et al., 2001]. Some techniques are equally useful for step and chain polymerizations, while others are more appropriate for only one or the other. Techniques useful for radical chain polymerizations are generally applicable to ionic chain polymerizations. The utility of any particular technique also depends on its precision and accuracy at low, medium, and high percentages of conversion. Some of the techniques have the inherent advantage of not needing to stop the polymerization to determine the percent conversion, that is, conversion can be followed versus time on the same reaction sample. [Pg.208]

Figure 10.1. Experimental procedure for the determination of the colloidal index (Cl). The Cl or the silt density index (SDI) test is used to predict and prevent particulate fouling on the membrane surface. It measures the time required to filter a fixed volume of water through a standard 0.45- xm pore-size microfiltration membrane with a pressure of 2.07 bar. The difference between the initial time and the time of a second measurement after normally 15 minutes (after silt was built up) represents the Cl or SDI value. Figure 10.1. Experimental procedure for the determination of the colloidal index (Cl). The Cl or the silt density index (SDI) test is used to predict and prevent particulate fouling on the membrane surface. It measures the time required to filter a fixed volume of water through a standard 0.45- xm pore-size microfiltration membrane with a pressure of 2.07 bar. The difference between the initial time and the time of a second measurement after normally 15 minutes (after silt was built up) represents the Cl or SDI value.
The general statement that connects quantum theory to experimental observations such as optical activity can be put as follows. We subject the material medium to some experimental procedure using a probe light beam, and observe a certain outcome after the probe has passed through the system, for example by analysing the scattered light. If we define the density matrix tot for the combined system of material medium + probe, and characterize the measurement by some operator, then the probability that the specified outcome of the measurement is observed, is given by,... [Pg.15]

The experimental procedure was described in a previous publication[2]. Data sets were measured for the following systems n-Butane + Tetrapentacontane, n-Butane + Hexacontane, LPG(n-Butane rich) + Hexacontane and LPG(Propane rich) + Tetrapentacontane. The first three data sets were reported previously[2,3]. The vapour-liquid equilibria and density data for the system LPG + Tetrapentacontane is shown in figures 2 and 3 respectively. The composition of the propane rich LPG used in the LPG + Tetrapentacontane measurements, as determined with capillary GC with an FID detector, is shown in table 1. [Pg.284]

Bromides and Iodides. The absorption spectra of the gaseous rare-earth halides were measured with a Cary 14 H spectrophotometer. The experimental procedure has been described previously 11). In this study a double furnace was used, allowing the rare-earth halide vapor to be heated to a higher temperature than the solid or liquid and allowing a baseline determination at the temperature of interest. In addition, a 0 0.1 full scale optical density slidewire was employed with the Cary... [Pg.119]

Quantitative y-ray spectrum analysis of environmental samples such as soil, water or ash of food requires the peak efficiency for volume sample. A Marinelli beaker is often used as a container for a large quantity of sample such as water or soil. As the volume of sample to be measured is usually fixed, the absolute peak efficiency is dependent on energy only, but affected by self-absorption which depends on density of matrix and the elemental composition. The method to be used for determination of the peak efficiency is based on experimental procedures involving the following steps ... [Pg.174]

When the PEELS measurement was conducted, an abrupt drop in density was observed at the interface between the matrix and the craze bands (Figure 4). In addition, a drop of approximately 50% in density was found at the base of the already unloaded craze band. This observation implies that an extension ratio of at least 2 exists for the craze fibrils. This phenomenon is not uncommon for thermoplastic crazes (5, 10). To ensure that the PEELS method gives reasonable results, the density of the craze band inside a polystyrene tensile specimen was measured (Figure 5) using the same sample-preparation procedures described in the section Experimental Details. The measured density of the craze band in the unloaded polystyrene was found to be about 0.62 g/cm3, which is in good agreement with the number reported in the literature (5,10, 24). [Pg.175]

The previous concepts may be summarized by briefly reviewing the experimental procedures for determining the kinetic parameters, i0, Pox, and Pred. If a single half-cell reaction is involved, the equilibrium half-cell potential will be measured against some reference electrode. If the electrode is now connected to a potentiostat and the potential increased in the positive or oxidation direction, the upper solid curve of Fig. 3.11 will be plotted. If the potential is decreased, the lower solid curve will be plotted. The higher current-density linear sections of each curve are then extrapolated through the value of the equilibrium poten-... [Pg.107]

Outline an experimental procedure and a method of data analysis that will enable one to determine the constants Kj)S, K and k of Illustration 8.4 with a minimum of experimental effort. Assume that D t) measurements were taken at equal time increments (i.e., 0.1, 0.2, 0.3- -h.) Benzene is to be nitrated in a batch reactor with acid composed of 15mol% HNO3, 25mol% H2SO4, and 60mol% H2O. The amount of this acid is to be 10% in excess of the theoretical amount required for 100% conversion, although only 96% conversion is required. The reaction temperature is 40°C, at which the densities are 0.87, 1.20 and 1.60 g/ cm for benzene, nitrobenzene, and the acid mixture, respectively. [Pg.663]

The lattice parameters of the hexagonal p-SiAlON phase were calculated from the XRD peaks ofthe products by employing the least-squares method. The lattice parameter a was calculated from (100), (110), (20 0), (2 10), (3 0 0), and (310) peaks of P-SiAlON, and the lattice parameter c was calculated from the (101) peak using the calculated a value. The bulk density of the spark-plasma-sintered (SPSed) specimens was measured according to the Archimedean principle, using distilled water as the medium. The detailed experimental procedure was published in paper [11]. [Pg.103]


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