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Measurement coating resistance

In electrochemical protection the necessary range of protection current is achieved by an appropriate arrangement of the electrodes. It follows that measures which raise the polarization resistance are beneficial. Coated objects have a coating resistance (see Section 5.2), which can be utilized in much the same way as the polarization resistance in Eq. (2-45). Therefore, the range in the medium can be extended almost at will by coatings for extended objects, even at low conductivity. However, the range is then limited by current supply to the object to be protected (see Section 24.4). [Pg.51]

Soil resistivity measurements can be affected by uncoated metal objects in the soil. Values that are too low are occasionally obtained in built-up urban areas and in streets. Measurements parallel to a well-coated pipeline or to plastic-coated cables give no noticeable differences. With measurements in towns it is recommended, if... [Pg.117]

The variation in the on and off potentials or the potential difference along the pipeline will usually indicate faults that prevent the attainment of complete cathodic protection. The protection current requirement of the pipeline may be estimated from experience if the age and type of pipeline is known (see Fig. 5-3). Figure 3-20 shows the variation in the on and off potentials of a 9-km pipeline section DN 800 with 10-mm wall thickness. At the end of the pipeline, at 31.84 km, an insulating unit is built in. The cathodic protection station is situated at 22.99 km. Between this and the end of the pipeline there are four pipe current measuring points. The applied protection current densities and coating resistances of individual pipeline sections are calculated from Eqs. (3-40) and (3-41). In the upper diagram the values of... [Pg.119]

Tank/soil potential measurements cannot be made on objects to be protected with very high coating resistances which are found in rare cases of defect-free coating, and particularly with resin coatings. Off potentials change relatively quickly with time, similar to the discharge of a capacitor, and show erroneous values that are too positive [8]. This is the case with coating resistances of 10 Q m. If there are defects, the resistance is clearly much lower. The advice in Section 3.3.2.2 is then applicable for potential measurement. [Pg.295]

Impedance spectroscopy This technique is essentially the extension of polarization resistance measurements into low-conductivity environments, including those listed above. The technique can also be used to monitor atmospheric corrosion, corrosion under thin films of condensed liquid and the breakdown of protective paint coatings. Additionally, the method provides mechanistic data concerning the corrosion processes, which are taking place. [Pg.911]

If protection by paints or varnish films is due to their ability to restrict the penetration of corrosive ions, then it follows that resistance measurements should form the basis of the prediction of their behaviour. In 1948 Bacon eta/. measured the resistance of over 300 paint systems immersed in seawater using a d.c. technique, and concluded that for good performance coatings should have a resistance in excess of 10 0cm Coatings having resistances in the range 10 -10 0cm were found to be unreliable, and those of lower resistance behaved poorly. [Pg.605]

The hardness and abrasion resistance of anodic coatings have never been easy properties to measure, but the development of a British Standard on hard anodising has made this essential. Film hardness is best measured by making microhardness indents on a cross-section of a film , but a minimum film thickness of 25 tm is required. For abrasion resistance measurements, a test based on a loaded abrasive wheel , which moves backwards and forwards over the film surface, has improved the sensitivity of such measurements. [Pg.703]

The values of the three electrochemical measurements, potential, resistance, and current were measured for the four coatings over time. The resultant time series for each measurement and coating combination were analyzed by the Box-Jenkins ARIMA procedure. Application of the ARIMA model will be demonstrated for the poly(urethane) coating. Similar prediction results were obtained for all coatings and measurements, however, not all systems were modeled by the same order of ARIMA process. [Pg.92]

Fig. 5.2 Variation of conductivity with mol% Ru02 in the coating. The measurement technique and the final firing temperatures are noted below. The symbols are = 350-600°C/ direct resistance measurement (Ref. [3]) O = 450°C/a.c. impedance (Ref. [4]) A = 400°C/ direct resistivity measurement (Ref. [5]). Fig. 5.2 Variation of conductivity with mol% Ru02 in the coating. The measurement technique and the final firing temperatures are noted below. The symbols are = 350-600°C/ direct resistance measurement (Ref. [3]) O = 450°C/a.c. impedance (Ref. [4]) A = 400°C/ direct resistivity measurement (Ref. [5]).
DC techniques Include measurement of DC resistance, determination of polarization behavior, and measurement of polarization resistance. Coating resistance has been correlated with corrosion performance by a number of workers. As svunmarlzed by Leldhelser ( ), the results of several independent investigations suggest that coating resistance below about 10 ohm/cm Is associated with the formation of visible under-film corrosion. Parallel DC resistance measurements on thin film metal substrates have been used to study the deterioration of coated metals the technique successfully detected the effects of water after migration to the coating/metal interface (351. [Pg.7]

A micro computer system allowed voltage and current measurements to be synchronised plus data logging and averaging of measurements. Alongside each "measurement" foil was a "control" foil, coated with paint plus a protective epoxy coating, which did not corrode and allowed resistance measurements to be normalised. [Pg.21]

The impact resistance of the pseudo-IPN coatings was measured on a Gardner-SPI modified Variable Height Impact Tester using both the direct and the indirect techniques. [Pg.314]

During the entire coating process the coating thickness is continuously monitored with an optical measuring system or by means of electrical resistance measurement devices. The measured values are compared with the coating thickness setpoints in the system and the evaporator power is thus automatically controlled. [Pg.136]

For coatings with no pitting, the generalized model must be amended to account for that fact that all current must flow through the barrier coating. The coating resistivity, Rt, is on the order of 100 to 1000 MQ cm2 and behaves essentially as an open circuit under near-DC conditions (f = 0). The EIS response over the typically measured frequency domain is that of a constant phase element (CPE) in series with a solution resistance (Fig. 22b). [Pg.292]

Fig. 10 Schematic diagram of gold sputter coating on a CaO coating for electrical resistivity measurements. Fig. 10 Schematic diagram of gold sputter coating on a CaO coating for electrical resistivity measurements.
Analysis of the results allowed conclusions to be drawn from the high-resistance measurements of the coatings. The mean volumetric electrical resistance of the samples tested was pv = 109-1010 ohm.cm. [Pg.186]

Tensile stress is used to characterize cohesiveness between particles, or in a certain powder cake, coating resistance in an encapsulated powder. Shear stress refers to the stress component tangential to the plane on which forces act and is mainly used to determine frictional properties (e.g., angle of internal friction) between particles under a pressure load. Furthermore, because individual particles predominantly slide across each other in a shearing action during flow, shear stress measurement allows determination of flow properties. [Pg.237]

DC electrical resistivity measurements were carried out using LCR Macroni bridge with two probe conductivity arrangement. The end faces of each pellet were coated with a thin layer of conducting silver paste which was activated in an oven for 5h. Resistivity was measured from room temperature to 773 K. An electric field of 20 V cm" was applied across the pellet for these measurements. [Pg.992]

Schematic diagrams of commercial tin oxide sensors by Figaro Engineering Inc. are shown in figure 14.2. The sensor of figure 14.2(c) consists of a small ceramic tube coated with tin (IV) oxide and a suitable catalyst. A heater coil maintains the tin oxide temperature (between 200 and 500 °C). The signal is the resistance measurement between the two electrodes at opposite ends of the tube. The assembly is packaged in a protective housing with an open area (covered by wire mesh) to allow gases to enter. Schematic diagrams of commercial tin oxide sensors by Figaro Engineering Inc. are shown in figure 14.2. The sensor of figure 14.2(c) consists of a small ceramic tube coated with tin (IV) oxide and a suitable catalyst. A heater coil maintains the tin oxide temperature (between 200 and 500 °C). The signal is the resistance measurement between the two electrodes at opposite ends of the tube. The assembly is packaged in a protective housing with an open area (covered by wire mesh) to allow gases to enter.
Coatings of Eudragit RL100 were shown to offer only minimum diffusional resistance to cyanomethemoglobin which was released from lysed red blood cells. Encapsulated red blood cells remained viable after coating, as measured by... [Pg.193]


See other pages where Measurement coating resistance is mentioned: [Pg.110]    [Pg.110]    [Pg.110]    [Pg.110]    [Pg.112]    [Pg.120]    [Pg.287]    [Pg.298]    [Pg.336]    [Pg.529]    [Pg.383]    [Pg.149]    [Pg.1217]    [Pg.115]    [Pg.284]    [Pg.308]    [Pg.324]    [Pg.290]    [Pg.314]    [Pg.330]    [Pg.86]    [Pg.412]    [Pg.135]    [Pg.424]    [Pg.606]    [Pg.51]    [Pg.360]   
See also in sourсe #XX -- [ Pg.110 , Pg.112 ]

See also in sourсe #XX -- [ Pg.110 , Pg.112 ]




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