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Temperature general effects

The equations presented herein do not include any viscosity correction to reflect the difference between the viscosity at the wall temperature and the bulk fluid temperature. This effect is generally negligible, except at low temperatures for organic fluids having viscosities that are strongly temperature dependent. For such conditions, the values tabulated in Table 2 should be appropriately modified. [Pg.508]

Vapor Toxicity. Laboratory exposure data indicate that vapor inhalation of alkan olamines presents low hazards at ordinary temperatures (generally, alkan olamines have low vapor pressures). Heated material may cause generation of sufficient vapors to cause adverse effects, including eye and nose irritation. If inhalation exposure is likely, approved respirators are suggested. Monoethan olamine and diethanolamine have OSHA TLVs of 3 ppm. [Pg.9]

The net effect is that tackifiers raise the 7g of the blend, but because they are very low molecular weight, their only contribution to the modulus is to dilute the elastic network, thereby reducing the modulus. It is worth noting that if the rheological modifier had a 7g less than the elastomer (as for example, an added compatible oil), the blend would be plasticized, i.e. while the modulus would be reduced due to network dilution, the T also would be reduced and a PSA would not result. This general effect of tackification of an elastomer is shown in the modulus-temperature plot in Fig. 4, after the manner of Class and Chu. Chu [10] points out that the first step in formulating a PSA would be to use Eqs. 1 and 2 to formulate to a 7g/modulus window that approximates the desired PSA characteristics. Windows of 7g/modulus for a variety of PSA applications have been put forward by Carper [35]. [Pg.477]

These quantum effects, though they do not generally affect significantly the magnitude of the resistivity, introduce new features in the low temperature transport effects [8]. So, in addition to the semiclassical ideal and residual resistivities discussed above, we must take into account the contributions due to quantum localisation and interaction effects. These localisation effects were found to confirm the 2D character of conduction in MWCNT. In the same way, experiments performed at the mesoscopic scale revealed quantum oscillations of the electrical conductance as a function of magnetic field, the so-called universal conductance fluctuations (Sec. 5.2). [Pg.111]

Relatively little information is available on the influence of initial pressure and initial temperature on detonation limits, in confined situations. The general effect of an increase in inidal pressure is to widen the detonations limits, and the same applies to an increase in the initial temperature. The widening is more marked for die upper limit. [Pg.71]

Tests in a Clj + Oj mixture at 427°C have shown that the worst elements for promoting susceptibility are Al, Sn, Cu, V, Cr, Mn, Fe and Ni, while the least harmful are Zr, Ta and Mo. a-phase alloys are generally more susceptible than )3-phase alloys. Heat treatment has not been examined extensively, but some heat treatments render some a-alloys more susceptible or change the mode of fracture. The general effect will depend upon the alloy and the heat-treatment cycle. Subsequent cold work can sometimes considerably lower susceptibility. Failure times decrease as either the testing temperature or initial stress value is raised. [Pg.1261]

Effect of Temperature. Generally, isotropic deposits are obtained at higher temperatures (>1400°C) and laminar and columnar deposits at lower temperatures. [Pg.192]

Hydrilla explant bioassays. The general effects of temperature on production and elongation of new shoots on 2-node hydrilla explants is shown in Figure 3. No shoots were produced at 15 C, but at 36 C ca. 50% of the explants had new shoots averaging 7 cm in length within 7 days. In most cases, only one new shoot was produced per explant, but occasionally, two shoots were produced (either one at each node or two at one node). [Pg.357]

In general, solubility is mainly a function of temperature, generally increasing with increasing temperature. Pressure has a negligible effect on solubility. [Pg.204]

Equation 8.3.4 is completely general and independent of whether the reaction occurs at constant density (dA = 0) and of whether the feed stream and the reactor contents have identical temperatures. The effective reactor volume is independent of the particular geometry giving rise to this volume. All that is required is that the contents be well mixed. [Pg.272]

Fig. 3.6. Specific heats of MnC03 and CaC03 illustrate the general effect of a magnetic transition. Data from [30], The Neel temperature for MnC03 is 29.4 K [30]. Fig. 3.6. Specific heats of MnC03 and CaC03 illustrate the general effect of a magnetic transition. Data from [30], The Neel temperature for MnC03 is 29.4 K [30].
Additional considerations in the design and operation of a remote hydrogen plasma system include the following (1) convective heat transfer between the downstream gas and the specimen can introduce a significant difference between the heater temperature and the specimen surface temperature (this effect is generally not as severe as for direct immersion in... [Pg.130]

Two forms of flameless atomizer are in use, i.e. the graphite tube or L Vov furnace and the carbon rod or filament. Of these the first has proved to be the most generally effective and popular. It is widely used in a variety of modifications. In both cases, the temperature is raised rapidly to about 2500 K by the passage of a heavy current for a period of 1-2 minutes. Tube furnaces, which are usually 5 or 10 cm x 3 mm, may be flushed through with argon before vaporizing the sample so as to prevent the formation of... [Pg.328]


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See also in sourсe #XX -- [ Pg.7 ]




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General effects

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