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Local temperature

This justifies all the work undertaken to arrive at fuel denitrification which, as is well known, is difficult and costly. Moreover, technological improvements can bring considerable progress to this field. That is the case with low NO burners developed at IFF. These consist of producing separated flame jets that enable lower combustion temperatures, local oxygen concentrations to be less high and a lowered fuel s nitrogen contribution to NOj. formation. In a well defined industrial installation, the burner said to be of the low NO type can attain a level of 350 mg/Nm, instead of the 600 mg/Nm with a conventional burner. [Pg.269]

Item 7 Describe ihe suspected adverse event. Such things as temperature, local and general signs and symptoms, time course, duration of symptoms diagnosis, treatment and recovery should be noted. [Pg.670]

Land formed very early due to eruptions from the hot mantle, which here and there upset equilibria and temperature locally for relatively short periods. Owing to the motion of the Earth, the Sun s radiation fell, and still falls (unevenly) on Earth causing air circulation which carries rain water and which, on precipitation, erodes the land so that fine deposits developed close to the sea. At the same time, there is the slower movements of the underlying mantle giving rise to both chemical and physical changes. [Pg.32]

The second example used visible light absorption that increased the temperature locally within the thermosensitive gel [39]. The gel consisted of a covalently cross-linked copolymer network of N-isopropylacrylamide and chloro-phyllin, a combination of a thermo-sensitive gel and a chromophore. In the absence of light, the gel volume changed sharply but continuously as the temperature was varied. Upon illumination the transition temperature was lowered, and beyond a certain irradiation threshold the volume transition became discontinuous. The phase transition was presumably induced by local heating of polymer chains due to the absorption and subsequent thermal dissipation of light energy by the chromophore. The details will be discussed in a later section. [Pg.53]

The 116-pm focused beam raised the temperature locally up to 70 °C. An X-Y-Z moving stage permitted the creation of arrays of dots of 350 pm diameter. [Pg.91]

Bottom This chip is cultivated at 40 °C, just below the upper temperature limit for fibroblasts. The electric field again raises the temperature locally, creating a zone where cells cannot grow... [Pg.107]

Even relatively low concentrations of noncondensible gases can substantially reduce the condensation rate. The main reason for this is that as vapor condenses, noncondensible gases get carried with the vapor toward the surface of the film. Since the film is impermeable, the concentration and partial pressure of noncondensible gases build up near the film to levels much higher than those far from the film. Since tdbe total pressure is constant, the noncondensible gases suppress the partial pressure of the vapor at thd edge of the film. This reduces the saturation temperature locally at the film/vapor interface as illustrated in Fig. 11.19. In turn, the reduction in the driving temperature difference leads to a reduction in the heat transfer and condensation... [Pg.585]

A number of important questions, however, still remain open. The first is which ion displacements Pb or Nb/Mg/Sc are responsible for the formation of polar regions What is the nature of non-polar matrix into which polar clusters are assumed to be embedded Are the polar clusters and the non-polar matrix dynamic or static entities Another still open important problem in PMN relaxor is related to microscopic inhomogeneities in the site occupancy of the Mg2-1" and Nb5+ cations and their role in the formation of the polar regions. An existence of a 1 1 Mg/Nb ordered microregions is still discussed in literature. Since the 1 1 Sc/ Nb chemical order in PbSci/2Nbi/203 really exists, a comparative study of the high-temperature local structure of these two relaxors is of interest. [Pg.159]

According to the basic statement of the models we are going to summarize, the metal is conceived as a network of cations immersed in a cloud of free electrons in a crystalline structure. The transport of the ions controls the growth of the new phase (Figure 8.2). The ionic transport will depend on the nature of the system and on experimental conditions, such as temperature, local electric field, local concentration excess, etc. To better understand the continuous-film models, the main ionic transport mechanisms in crystalline solids are presented [1] as follows. [Pg.192]

The data of Schegolev and Zolotukhin on conductivity of Adz /TCNQ/2 are shown in Fig. 8. Their data on dielectric permeability are shown in Fig. 9. For Adz/TCNQ/2 the low temperature localization length 17 2 has been found... [Pg.273]

Higher temperature may result in a weaker Rehbinder effect as well. This occurs due to the facilitation of a plastic flow at elevated temperatures. Thermal fluctuations result in the relaxation of deformational microheterogeneities. As a result, at elevated temperatures local concentrations of stresses are too low to initiate the formation of primary microcracks. An increase in temperature thus often leads to a transition from brittle fracture in the presence of adsorption-active medium to plastic deformation. The decrease in the rate of deformation of a solid has an analogous effect slow deformation also results in an increased probability of the thermally activated relaxation of locally concentrated deformations and stresses. [Pg.719]

Calf thymus DNA/intercalated Temperature- Local motions < 7 ns above 220 K DNA rigid at low temp. 231... [Pg.198]


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Arrhenius relation local temperatures

Electron localization, high temperature

Electron localization, high temperature structure

Local Temperature Models

Local analyses temperature

Local high temperature

Local, environment temperature

Localization temperature

Localization temperature

Localized high temperatures

Locally excited state temperature dependence

Measurement of Local Temperature for Several Organic Solvents

Microcanonical temperature local temperatures

Shear localization temperature rise

Temperature dependence local temperatures

Temperature elevation from localized

Temperature measurement local

Temperature rises associated with shear localization

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