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Thermal conductivity Figure , 277

Thermal Conductivity Detector One of the earliest gas chromatography detectors, which is still widely used, is based on the mobile phase s thermal conductivity (Figure 12.21). As the mobile phase exits the column, it passes over a tungsten-rhenium wire filament. The filament s electrical resistance depends on its temperature, which, in turn, depends on the thermal conductivity of the mobile phase. Because of its high thermal conductivity, helium is the mobile phase of choice when using a thermal conductivity detector (TCD). [Pg.569]

Thermal Conductivity. Figure 1 shows the temperature dependence of a range of materials, and it can be seen that the values of thermal conductivities of materials vary widely. Typical values are as follows ... [Pg.97]

Fig. 1.8. Schematic illustration of the ways in which microscopic calculations may be exploited to model macroscopic material properties. The first example (frames (a) and (b)) illustrates the use of microscopic calculations to examine surface diffusion, while the second example (frames (c) and (d)) illustrates the analysis of phonons in Ge as the basis of an analysis of thermal conductivity. Figures adapted from (a) Kaxiras and Erlebacher (1994), (b) Gjostein (1972), (c) and (d) Omini and Sparavigna (1997). Fig. 1.8. Schematic illustration of the ways in which microscopic calculations may be exploited to model macroscopic material properties. The first example (frames (a) and (b)) illustrates the use of microscopic calculations to examine surface diffusion, while the second example (frames (c) and (d)) illustrates the analysis of phonons in Ge as the basis of an analysis of thermal conductivity. Figures adapted from (a) Kaxiras and Erlebacher (1994), (b) Gjostein (1972), (c) and (d) Omini and Sparavigna (1997).
In order to answer this, Carborundum needed to understand the role of oxygen in changing the thermal conductivity. Our Cleveland Research Centre provided this understanding by harnessing a battery of techniques, particularly a photo-luminescence measurement which showed a strong correlation between the position of the luminescence peak and the level of thermal conductivity (Figure 5) this technique also had the advantage of rapid measurement without need for special sample preparation. [Pg.25]

The CHX is installed in an air loop to obtain its thermal conductance. Figure 7 shows a flow sheet of the air test loop. A compressor transfers low temperature air into the CHX. After that, it is heated up to the maximum 120°C in an electric heater and flows back to the CHX. The heat is transferred from high to low temperature air in the CHX. An exhausted air from the CHX is released to the atmosphere. Four K-type thennocouples are installed at each inlet and outlet nozzle of the CHX, and the flow rate of air is measured by a vortex flowmeter. As a result, the thermal conductance is calculated by an inlet and outlet temperatures, flow rate and specific heat of air. [Pg.174]

Knowing the thermal conductivity (Figure 10.12) of the insulation material at the mean temperature, the quantity of heat passing through a refractory wall is... [Pg.388]

Materials used to make nozzles. The main features required of materials used for nozzles are a high level of mechanical strength and a high thermal conductivity (Figure 4.4), and in some applications they must also he highly ahrasion-resistant and have special resistance to chemicals. [Pg.80]

The effect of stoichiometry on the strand surface temperature is shown in Figure 6.8. It shows a temperature decrease with an increase in Mg content. This can be related to increased composite thermal conductivity (Figure 6.9), which effects faster dissipation of heat. At stoichiometries about 60 wt% Mg and above, the surface temperature scatters around the fusion temperature of magnesium (660 °C). [Pg.75]

Yeh et al. (2009) investigated the effect of nanoclay on the dielectric and thermal transport properties of PMMA nanocomposite foams. As shown in Figure 1.18, the nanocomposite foams showed lower dielectric constants than the neat PMMA foam. And the effect is more prominent when the clay nanoparticles were better dispersed (CCLMA clay) and when the clay concentration was increased. The effect on thermal conductivity (Figure 1.19) was slightly more complicated. While the nanocomposite foams with better dispersion, that is, CCLMA nanocomposites with an exfoliated-intercalated mixed morphology, showed a deaease in thermal conductivity, the thermal conductivity of the intercalated ACLMA nanocomposite foam was higher than that of neat PMMA foam. They have also prepared PMMA M WCNT nanocomposite foams and measured their insulation property. Interestingly, they noticed a decrease in both dielectric constant (22.6%) and thermal conductivity (19.7%) in the nanocomposite foams with 0.3 wt% carboxyl-multi-walled carbon nanotubes (c-MWNTs). [Pg.25]

The temperature dependence of the thermal conductivity isolates different mechanisms affecting the thermal conductivity. Figure 8.9 shows thermal conductivity of three materials... [Pg.319]

Insulation materials comprising multiple reflective shields separated by various spacer materials have been tested to determine the apparent thermal conductivity. Figure 3 shows a few of the shield materials and spacer materials tested or to be tested. The shields consist of reflective materials with and without secondary materials. The bonding of the reflective material to another material makes possible easy handling of very thin foil in large-scale applications. Of the spacer materials shown, tests have been conducted on the powders, glass fibers, glass fiber papers, and asbestos paper. Results of these tests are shown in Table I. [Pg.221]


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