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Thermal mechanical measurement

All VGCF was graphitized prior to composite consolidation. Composites were molded in steel molds lined with fiberglass reinforced, non-porous Teflon release sheets. The finished composite panels were trimmed of resin flash and weighed to determine the fiber fraction. Thermal conductivity and thermal expansion measurements of the various polymer matrix composites are given in Table 6. Table 7 gives results from mechanical property measurements. [Pg.151]

Thermal-mechanical analysis (TMA) has proven a more reproducible measure of melt integrity [20]. The TMA test involves measuring the shape change of a separator under load while the temperature is linearly increased. Typically, separators show some shrinkage, then start to elongate, and finally break (see Fig. 5). [Pg.561]

Correlations between surface species and emitted secondary ions are based on characterization of the surface adlayer by adsorption and thermal desorption measurements. It is shown that the secondary ion ratios RuC+/Ru+ and R CTVRuJ can be quantitatively related to the amount of nondesorbable surface carbon formed by the dissociative adsorption of ethylene. In addition, emitted hydrocarbon-containing secondary ions can be directly related to hydrocarbon species on the surface, thus allowing a relatively detailed analysis of the hydrocarbon species present. The latter results are consistent with ejection mechanisms involving intact emission and simple fragmentation of parent hydrocarbon species. [Pg.27]

The working principle of the thermocouple was discovered (1823) by Seebeck who observed that if wires of two different metals were joined to form a continuous circuit, a current flowed in the circuit when the two junctions were at different temperatures. In order to make a measurement, one junction (the reference junction) is maintained at a constant temperature (typically at 0°C) and the electromotive force produced when the other junction is at the test temperature is measured, or recorded, by a suitable instrument (or used as the input of a controller ). In order to choose the right kind of thermocouple among the many types available, the temperature range to be studied must be considered, as well as several requirements regarding sensitivity, calibration stability, chemical, thermal, mechanical inertia, etc. [Pg.548]

The major factor influencing the thermal and mechanical properties is the composition differences between the polymers. Gel permeation chromatography measurements have shown that the molecular weight averages and molecular weight distributions are not significantly different for the samples which have been studied and are therefore not seen as important as far as Tg and mechanical measurements are concerned. [Pg.336]

We now turn to a correlation of the DMTA results with DSC measurements. In Figure 10 the extent of C=C double bond conversion, as measured with DSC, is plotted versus exposure time. Also plotted is the amount of monomer extracted afterwards from the DSC samples. It can be seen that for exposure times longer than 6 s the rate of polymerization decreases suddenly to a much lower value, but not to zero. At the same time the free monomer is exhausted so further reaction necessarily means further crosslinking by reaction of pendent double bonds. According to our mechanical measurements thermal aftercuring also ceases to have an observable effect on E (Figure 9a and b). [Pg.423]

The measurements of Young s modulus in dependence of the temperature (dynamic-mechanical measurements, see Sect. 2.3.5.2) and the differential thermal analysis (DTA or DSC) are the most frequently used methods for determination of the glass transition temperature. In Table 2.10 are listed and values for several amorphous and crystalline polymers. [Pg.120]

It is noteworthy that nonlinearity of the absorption, required for 3D microfabrication can be provided via thermal mechanisms [53,54]. In the case of tightly focused laser pulses, linear absorption is most efficient at the focus, where local heating can create the conditions required for polymerization. Usually the absorption increases with temperature and thermal polymerization may become dominant at the focus. It is usually difficult to confirm the TPA mechanism from the direct transmission measurements due to the nar-... [Pg.174]

The glass transition temperature can be measured in a variety of ways (DSC, dynamic mechanical analysis, thermal mechanical analysis), not all of which yield the same value [3,8,9,24,29], This results from the kinetic, rather than thermodynamic, nature of the transition [40,41], Tg depends on the heating rate of the experiment and the thermal history of the specimen [3,8,9], Also, any molecular parameter affecting chain mobility effects the T% [3,8], Table 16.2 provides a summary of molecular parameters that influence the T. From the point of view of DSC measurements, an increase in heat capacity occurs at Tg due to the onset of these additional molecular motions, which shows up as an endothermic response with a shift in the baseline [9,24]. [Pg.123]

In order to deduce the product P(0)R(0) in these experiments from a simple inversion of V z), it is necessary to measure it as a complex-valued function, i.e. with both amplitude and phase information. This can be done, though the requirements for thermal, mechanical, and electronic stability should not be underestimated. If the phase information is not available, then it must be reconstructed. [Pg.128]

Results. In a typical experiment on the explosion of a mixture of 23.5% CO with air at p0 = 5 kg/cm2 we obtained 0.33% NO. The computed explosion temperature Tm = 2560°K and [NO] = 0.99%. However, experimentally we observed a maximum pressure of 2.5 kg/cm2 which corresponds to an explosion temperature T = 1670°K the equilibrium content of nitric oxide at 1670°K equals [NO] = 0.11%. It might appear that a triple yield of nitric oxide compared to the equilibrium value at the measured temperature even in one experiment would prove the existence of a non-thermal mechanism regardless of any other findings. Hausser [8] drew just such a conclusion from similar data. However, as we shall see later, it is incorrect. [Pg.374]

Exergy (availability) is a property of a material system that measures the maximum work which can be obtained when the system is brought to the reference or dead state that is thermally, mechanically and chemically in equilibrium with the surroundings. As the dead state changes, so does the numerical value of the exergy (availability). In other words, the value of the exergy depends on the choice of the surroundings, which is defined to be the dead state. [Pg.352]


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