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Measuring Polarization

Measurement of corrosion rate is essential for the purpose of material selection. The compatibility of a metal to its environment is a prime requirement for its reliable performance. Corrosion rate measurement may become necessary for the evaluation and selection of materials for a specific environment or a given definite application, or for the evaluation of new or old metals or alloys to determine the environments in which they are suitable. Often the corrosive environment is treated to make it less aggressive, and corrosion rate measurement of a specific material in the untreated and treated environments will reflect the efficacy of the treatment. Corrosion rate measurement is also essential in the study of the mechanisms of corrosion. [Pg.31]

Most often, it is the anodic polarization behavior that is useful in understanding alloy systems in various environments. Anodic polarization tests can be conducted with relatively simple equipment and the scans themselves can be done in a short time. They are extremely useful in [Pg.32]

Active-passive behavior is dependent on the material-corrodent combination and is a fimction of the anodic or cathodic polarization effects that occur in that specific combination. In most situations where active-passive behavior occurs, there is a thin layer at the metal surface that is more resistant to the environment than the imderlying metal. In stainless steels, this layer is composed of various chromium and/or nickel oxides that exhibit substantially different electrochemical characteristics than the underlying alloy. If this resistant, or passive, layer is damaged while in the aggressive environment, active corrosion of the freshly exposed surface will occur. The damage to this layer can be either mechanical or electrochemical in nature. [Pg.33]

The behavior of iron in nitric acid underscores the importance of recognizing the nature of passivity. Iron is resistant to corrosion in nitric acid at concentrations around 70%. Once passivated under these conditions it can also exhibit low rates of corrosion as the nitric acid is diluted. However, if the passive film is disturbed, rapid corrosion will begin and repassivation will not be possible until the nitric acid concentration is raised to a sufficient level. [Pg.33]

Fundamentals of Metallic Corrosion Atmospheric and Media Corrosion of Metals [Pg.34]


Although the effects of dielectric constant change and strain have a strong effect on the current during wave transit time, the current at a time about j transit time is close to the value for the linear relation. Thus, based on Eq. 5.7, the wavespeed can be computed from the measured current and the measured polarization data. The approximate agreement between currents calculated from the polarization data and the wavespeed data confirms that the wavespeed values currently available are reasonable. [Pg.112]

Ratio measurement, polarity check and phase relationship ... [Pg.215]

The case of several populations of fluorophores having their own fluorescence decay i (t) and time constants characterizing r (t) deserves particular attention. In Section 5.3, it was concluded that an apparent or a technical emission anisotropy r(t) can be obtained by considering that the measured polarized components, I(t) and I (t), are the sums of the individual components (i.e. of each population) and by using Eq. (6.43). Hence... [Pg.191]

X cos 30° A is the inter-row distance of the commensurate Xe structure in the same direction. From the measured polar and azimuthal peak widths in Fig. 32 we can also estimate average domain sizes of the incommensurate layer. For the FK direction, i.e. parallel to the walls, we obtain 350 A and for the perpendicular TM direction 50 A. [Pg.257]

The open circuit potential represents the potential of the system taken after approximately a 10 minute equilibration period. In addition to open circuit potential measurements, polarization curves were run for each sample. It was hoped a correlation could be seen between the visual assessment of corrosion and polarization. Unfortunately, only open circuit potentials could be correlated with performance. Therefore, no attempts were made to correlate the corrosion current density or the shapes of the polarization curves with performance. [Pg.54]

The UV spectra of the coloured aryl-substituted alkylidenecycloproparenes show long-wavelength absorption maxima, the positions of which are solvent dependent and in accord with the measured polarities (Table 4, Section II.G)153-157-158,294 297. Removal of the... [Pg.759]

The structure of hard gels is best elucidated using SAXS or SANS because the periods of the ordered structures are on the scale 10-100nm. In addition to tube inversion and rolling ball viscometry, which are sensitive to yield stress, the formation of a hard gel can be identified by other techniques. These include DSC (gelation is an endothermic process), NMR (via transverse relaxation time, T2, measurements), polarized light microscopy and rheometry. [Pg.224]

Figure 3. An optical arrangement for measuring polarized reflection-absorption spectra of a monolayer or thin film on the surface of a minor S at near grazing incidence. P is a polarizer, Ml, M2, M3 and M4 are mirrors. Figure 3. An optical arrangement for measuring polarized reflection-absorption spectra of a monolayer or thin film on the surface of a minor S at near grazing incidence. P is a polarizer, Ml, M2, M3 and M4 are mirrors.
For ferroelectrics, mainly two possible mechanisms for irreversible processes exist. First, lattice defects which interact with a domain wall and hinder it from returning into its initial position after removing the electric field that initiated the domain wall motion ( pinning ) [16]. Second, the nucleation and growth of new domains which do not disappear after the field is removed again. In ferroelectric materials the matter is further complicated by defect dipoles and free charges that also contribute to the measured polarization and can also interact with domain walls [17]. Reversible contributions in ferroelectrics are due to ionic and electronic... [Pg.32]

Bums, R. G. (1966b) Apparatus for measuring polarized absorption spectra of small crystals. J. Sci. Instruments, 43,58-60. [Pg.483]

A fluorophore free in solution can have a low polarization value, whereas when it is bound to a macromolecule, its polarization increases. The polarization unit is a dimensionless entity, i.e., the value of P does not depend on the intensity of emitted light and the fluorophore concentration. However, this is the theory the reality is quite different. In fact, measuring polarization at high fluorophore concentrations yields erroneous values, and in many cases, instead of reading the correct values of P and A, values that neighbor the limiting values are recorded. [Pg.161]

In vitrified solution and/or when fluorophore molecules do not show any residual motions, the measured polarization is equal to the intrinsic one, P0. This value is obtained at low... [Pg.162]

However, during the excited-state lifetime, energy transfer to neighboring molecules and/or local and global motions of the fluorophores can be observed. These two phenomena induce reorientation of the emission dipole, thereby depolarizing the system. Therefore, the value of the measured polarization P will be lower than intrinsic polarization value PQ (Weber, 1952). [Pg.163]

One should be careful in measuring polarization, since if the sample is not fluorescing too much, errors in reading the intensities could be frequent. Also, depending on the instrument the student is using to perform the measurements, experiments could be easy or very hard to conduct. Therefore, it is important that all students perform each experiment described here so that they can learn how to conduct all experiments, difficult and easy, and also compare all the data obtained together. [Pg.179]

The purpose of these experiments is first to learn how to measure polarization value of a fluorophore and then to see the difference in the information when we perform the experiments at different temperatures and when we work at a fixed temperature but increasing the concentration of sucrose in the medium. [Pg.187]

This set of experiments has focused on the use of two nondestructive electrochemical techniques to measure polarization resistance and thereby estimate the corrosion rate. In addition, the effects of scan rate and uncompensated ohmic resistance were studied. Three main points should have been made by this lab (1) Uncompensated ohmic resistance is always present and must be measured and taken into account before Rp values can be converted into corrosion rates, otherwise an overestimation of Rv will result. This overestimate of Rp leads to an underestimate of corrosion rate, with the severity of this effect dependent upon the ratio Rp/Ra. (2) Finite scan rates result in current shunted through the interfacial capacitance, thereby decreasing the observed impedance and overestimating the corrosion rate. (3) Both of these errors can be taken into account by measuring Ra via EIS or current interruption and by using a low enough scan rate as indicated by an EIS measurement in order to force the interfacial capacitance to take on very large impedance values in comparison to Rp. [Pg.395]

Clarke and Parker54 have reported a thermodynamic study of the tautomerization of 2-(J/V-cyclohexylimino)-l,3-diphenylpropane (47) to its Z- and E-enamine tautomers 48a and 48b in DMSO-d6 solution (Scheme 4). The equilibrium constants and the values of the thermodynamic parameters AH, AG and AS have been determined by variable-temperature NMR measurements. Polar solvents are found to favor enaminization, but have little effect on the E Z isomerization of the enamine tautomers. [Pg.896]

This set of experiments has focused on the use of two nondestructive electrochemical techniques to measure polarization resistance and thereby estimate the corrosion rate. In addition, the effects of scan rate and uncompensated ohmic resistance were studied. Three main points should have been made by this lab ... [Pg.400]

Polarized spectra can be valuable in providing information on the symmetry of a species without requiring a detailed knowledge of their electronic stracture. In crystalline environments, polarized information is inherently available, but its utility is dependent on knowing the orientation(s) of the chromophores with respect to the crystal axes. In general, it is only possible to measure polarized spectra along the symmetry axes of a crystal. These directions may differ from the directions of the transition moments of the chromophores and the spectra that are measured then need to be deconstructed into polarized spectra of the chromophores themselves. ... [Pg.6521]

Bacterial reaction centers crystallize readily, providing high-resolution X-ray data and stmctural information. Photoactivation of these crystals leads to structural changes that can be monitored in time-resolved X-ray experiments. In order to be able interpret these changes, it is important to know the actual extent and kinetics of photoactivation of the crystallized reaction center. It has been possible to measure polarized single crystal data in the near-IR region on crystals of the same size ( 200 J,m) and contained within the same 1 mm capillary tubes as were used in the X-ray experiments. [Pg.6530]

Fig. 2.17. Schematic layout of a microscope spectrophotometer system used to measure polarized absorption spectra of very small mineral crystals. The computer-operated, single-beam instrument shown here comprises a polarizing microscope equipped with a stabilized light source (xenon arc lamp or tungsten lamp cover the range 250-2000 nm), a modulator that chops the light beam with a frequency of 50 Hz (the amplifier for the photodetector signals is modulated with the same phase and frequency), and a Zeiss prism double monochromator. Single crystals as small as 10 ji.m diameter may be measured with this system. A diamond-windowed high-pressure cell can be readily mounted on the microscope scanning table for spectral measurements at very high pressures (after Burns, 1985, reproduced with the publisher s permission). Fig. 2.17. Schematic layout of a microscope spectrophotometer system used to measure polarized absorption spectra of very small mineral crystals. The computer-operated, single-beam instrument shown here comprises a polarizing microscope equipped with a stabilized light source (xenon arc lamp or tungsten lamp cover the range 250-2000 nm), a modulator that chops the light beam with a frequency of 50 Hz (the amplifier for the photodetector signals is modulated with the same phase and frequency), and a Zeiss prism double monochromator. Single crystals as small as 10 ji.m diameter may be measured with this system. A diamond-windowed high-pressure cell can be readily mounted on the microscope scanning table for spectral measurements at very high pressures (after Burns, 1985, reproduced with the publisher s permission).
Time Domain Spectroscopy Basic Theory Experimental Methods Application to Dielectric Measurements Polar Liquids... [Pg.212]

Mennucci presented an approach for such studies. Subsequently, she applied it to two processes, a charge transfer from a donor to an acceptor in a smaller molecule, as well as to the calculation of the time dependence of a Stokes shift which is used spectroscopically to measure polar solvation dynamics. [Pg.73]

Dresser Instmments of Stratford, CT, under the ebro brand has introduced a handheld instmment called the Food Oil Meter (FOM-200). This instmment can repeatedly measure polar compounds within seconds in hot oil to directly monitor oil quality in a fryer. The results obtained from the FOM-200 correlates within +/- 2% of the official lUPAC method 2.507/DFG method III-3b for polar compounds and can store many characteristic oil curves for reference. The instmment is being used by several researchers in their frying studies and fast food franchises to better schedule filtering aids additions and oil replacements in order to improve overall food quality. [Pg.2254]


See other pages where Measuring Polarization is mentioned: [Pg.85]    [Pg.445]    [Pg.10]    [Pg.217]    [Pg.254]    [Pg.132]    [Pg.59]    [Pg.361]    [Pg.89]    [Pg.120]    [Pg.24]    [Pg.186]    [Pg.123]    [Pg.193]    [Pg.260]    [Pg.214]    [Pg.229]    [Pg.14]    [Pg.123]    [Pg.284]    [Pg.200]    [Pg.266]    [Pg.758]    [Pg.238]    [Pg.6528]    [Pg.478]   


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