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Thermal sampling

A single relaxation process is normally assumed when analyzing the shape of the TSC curve, and the activation energy can be estimated using the [Pg.28]


Table V shows the differences in the freeze-thaw durability of concrete-polymer specimens receiving radiation and thermal treatment. The data indicate that the thermally treated specimens have either the same or slightly better durability than the radiation treated material. The higher durability, however, may be related to the higher polymer loading present in the thermal samples for this series of tests. Table V shows the differences in the freeze-thaw durability of concrete-polymer specimens receiving radiation and thermal treatment. The data indicate that the thermally treated specimens have either the same or slightly better durability than the radiation treated material. The higher durability, however, may be related to the higher polymer loading present in the thermal samples for this series of tests.
For a Langmuir-Hinshelwood reaction in which both reactants are thermally equilibrated on the surface, reaction is initiated by thermal activation of the adsorbate. This thermal sampling can be turned to advantage by invoking detailed balance to equate the rates of adsorption and desorption for a surface at equilibrium [66, 67]. This allows us to relate the final state distributions measured for desorption to the detailed sticking probability for each product quantum state (v, J). This approach has been applied very successfully to hydrogen adsorption/desorption [4, 68] but its use has not been widely explored for reactions of heavier molecules. [Pg.150]

Now, the argument just presented relies on the unproven assumption that rotational quantum beats arising from a thermal sample of isolated molecules will wash each other out. Recently, we examined this assumption by directly simulating the decays associated with thermally averaged rotational beats.47 (Our initial motivation for this work was to try to explain the picosecond pump-probe results of Refs. 51 and 52, which results showed the existence of polarization-dependent early time transients in the decays of t-stilbene.) These theoretical simulations and subsequent picosecond-beam experiments47-50 have revealed that the manifestations of rotational coherence in thermally averaged decays can, in fact, be observed. In this section, we briefly review these results and examine some of their implications with regard to time-resolved studies of IVR. [Pg.345]

In a thermal sample at a temperature 7) the canonical distribution of K levels in the ground state will be... [Pg.233]

An instrument that uses thermal sample decomposition followed by gold amalgamation and CVAAS was specified in EPA Method 7473 [8]. A few commercial instruments based upon this technique have been used to analyze crude oil samples [9,10]. [Pg.197]

Figure 22. Experimental schemes presenting the thermo-electric procedure for global (left) and thermal sampling (right) experiments. The time interval during which the constant voltage is applied is indicated by the horizontal line. The insets shows the temperature dependence of the polarization of tiie sample during the... Figure 22. Experimental schemes presenting the thermo-electric procedure for global (left) and thermal sampling (right) experiments. The time interval during which the constant voltage is applied is indicated by the horizontal line. The insets shows the temperature dependence of the polarization of tiie sample during the...
The thermal sampling technique, TS, allows narrow segments of the complex thermocurrent to be polarised and, thus, it enables complex global peaks to be resolved into their individual components. The thermo-electric treatment of the sample during a TS experiment is schematically shown in Figure 22 (right). The electric field, Eq, is applied at Tp during tp and the sample is cooled (at a rate Pi), in the presence of the field, to a temperature where 7 - is typically 2-3 C. [Pg.255]

Complementary experiments may be also obtained by TSDC. This technique provides a simple way to probe the mobility of dipoles and electric charges over a large temperature range. The use of thermal sampling methodologies enables a better insight on the complexity in relaxation characterised by broad time distributions to be obtained... [Pg.260]

Thomas P. Wampler has been actively engaged in the field of analytical pyrolysis for 25 years. He is director of science and technology at CDS Analytical, Inc., in Oxford, Pennsylvania. He is the author or coauthor of numerous professional papers on the use of analytical pyrolysis and other thermal sampling techniques. He received aB.S. degree (1970) in chemistry andaMJid. degree (1973) in natural science from the University of Delaware, Newark. [Pg.297]

A study of microwave curing (70) effectiveness was made with a magnetron at 28 W power and a frequency of 2.45 Ghz in an 18 cm diameter cylindrical tunable cavity. With this system, samples can be cured in 10 min to approximately 99% conversion as measured by DSC. By way of comparison, for thermal samples, heating at 195 °C for two hours and postcure at 240 °C for one hour was required for cure to this extent. [Pg.562]

Poling and heating profiles used to measure thermally stimulated current. (1) Standard measurement, (11) partial heating method or peak cleaning method (111) thermal sampling method... [Pg.149]

The second method is referred to as thermal sampling or thermal windowing [2.3] (Figure 6.29(111)). [Pg.150]

Figure 2.26 Temperature and applied field diagram for the thermal sampling method... Figure 2.26 Temperature and applied field diagram for the thermal sampling method...
It is not surprising that most results in atomic spectroscopy were obtained on singly charged ions which are difficult to prepare for the usual Doppler-free techniques on thermal samples. On the other hand, the fast-beam technique has certain advantages also on neutral atoms, such as the availability of metastable beams, the sensitivity, and the Doppler-tuning. [Pg.97]

Figure 6.17. (a) Illustration of principle of the thermal sampling procedure. By varying the value of by a constant step along the axis (i.e., by shifting the polarization window Tp-Td from 2° to 5°), peaks with a narrow t distribution are recorded, (b) Schematic Arrhenius diagram of isolated processes that exhibit a compensation law behavior, (c) Schematic compensation diagram. [Pg.546]

It is obvious from the very small relaxation rate coefficient, k oi = (3.6 di 0.8) X cm s , that one has to take very large He densities for getting a thermalized sample of Ar+ with He as buffer gas. The deduced radiative relaxation rate fcrad = (0.06 0.04) s , corresponding to a radiative lifetime of 17 s, is in good agreement with a lifetime of 19.0 s calculated for the magnetic dipole transition. [Pg.323]


See other pages where Thermal sampling is mentioned: [Pg.191]    [Pg.216]    [Pg.249]    [Pg.250]    [Pg.173]    [Pg.177]    [Pg.98]    [Pg.173]    [Pg.177]    [Pg.343]    [Pg.256]    [Pg.275]    [Pg.199]    [Pg.345]    [Pg.188]    [Pg.110]    [Pg.126]    [Pg.162]    [Pg.343]    [Pg.615]    [Pg.833]    [Pg.834]    [Pg.837]    [Pg.28]    [Pg.29]    [Pg.528]    [Pg.543]    [Pg.564]    [Pg.565]    [Pg.598]   
See also in sourсe #XX -- [ Pg.615 ]

See also in sourсe #XX -- [ Pg.528 , Pg.543 , Pg.546 ]




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