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Conductivities temperature characteristics

Figure 4.5 Comparison of conductivity-temperature characteristics for various cathode materials produced by FSS and conventional methods. Cobaltites and ferrites ... Figure 4.5 Comparison of conductivity-temperature characteristics for various cathode materials produced by FSS and conventional methods. Cobaltites and ferrites ...
Ando K. Matsumoto T. Nagahama T. Ueki I. Takatsuki Y. and Kuroda Y. (2005). Drift characteristics of a moored conductivity-temperature sensor and correction of salinity data. J. Atmos. Oceanic Technol., 22, 282-291. [Pg.516]

Fluid characteristics w velocity, r viscosity, p density, X thermal conductivity. Column characteristics d diameter, H height. At differential temperature between the air and the column surface. [Pg.531]

Cut points specify the beginning and end of the collection of a fraction. Cut points can be based on time, although in practice time is not the most stable parameter, due to possible fluctuations in the flow rate. They can be based on threshold values of the UV-detector signal or on volume of eluent through a mass flowmeter. Cut point locations can also be a combination of a characteristic feature on the chromatogram and volume. Cut point locations for valve switching may also be based on the response of less traditional detection instrumentation such as the on- line measurement of density, conductivity, temperature, spedflc ion detection, near infrared, or refractive index. [Pg.854]

Figures 8.5 and 8.6 show the voltage dependence of the corrected capacitance Q and corrected conductance G,. characteristics at 1 MHz before and after 50 MeV Li + ion irradiation for different fluences at room temperature. The peaks seen in the Figure 8.7 correspond to the depletion area of the device. The value of interface traps density (Dj is determined from this peak value. This peak was observed for samples. From C-V and G-V measurements in the accumulation region, the oxide capacitance Cox was calculated using Equation 8.5 (Nicollian and Brews 1982) ... Figures 8.5 and 8.6 show the voltage dependence of the corrected capacitance Q and corrected conductance G,. characteristics at 1 MHz before and after 50 MeV Li + ion irradiation for different fluences at room temperature. The peaks seen in the Figure 8.7 correspond to the depletion area of the device. The value of interface traps density (Dj is determined from this peak value. This peak was observed for samples. From C-V and G-V measurements in the accumulation region, the oxide capacitance Cox was calculated using Equation 8.5 (Nicollian and Brews 1982) ...
Characteristic time required to establish a conductive temperature profile... [Pg.1029]

The process transfer curve indicates the power-temperature characteristic of the actuai system, i.e., the extruder and its surroundings. This curve indicates how much power is required to maintain a certain temperature level on the machine. The higher the temperature ievei that needs to be maintained, the more power will be required. For most machines, the reiationship between temperature and power requirement wiii be approximateiy iinear. The power requirement is determined by the heat iosses in the system by conduction, convection, and radiation. By improving the thermai insuiation of the extruder, the heat losses can be reduced. This will directly affect the process transfer curve adding insulation will reduce the power requirements at a certain temperature, resulting in a reduced slope of the process transfer curve. Obviously, this will also improve the energy efficiency of the entire process. [Pg.122]

The unsynchronized resonance of the bonds corresponds to the transfer of electric charge (electrons) that leads to high electric conductivity. This conductivity is characteristic of the structure of the metal, and hence takes place most readily at very low temperatures, when the atoms are quite regularly arranged in the crystal. At higher temperatures the thermal oscillation of the atoms introduces some disorder in their arrangement, which interferes with the resonance of the bonds, and hence causes a decrease in conductivity (negative temperature coefficient). [Pg.569]

Very often thermogravimetric curves are characteristic for particular polymers and can therefore be used for their identification. Because of the poor heat conductivity, temperature gradients occur within samples at high heating rates. To obtain reproducible results, a standardisation of heating rate should be used, e.g., 10 °C/min, when comparing an unknown polymer with a set of reference polymers. [Pg.209]


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