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Branching temperature

By using silicon wafers (showing a high value of the thermal conductivity) as a substrate and by taking the distance between both branches as small as possible (of course avoiding interaction of the modes traveling through both branches) temperature differences can be reduced. [Pg.272]

A similar temperature analysis is possible for the P-branch transitions to determine the temperature, and usually the R-branch and P-branch temperatures agree. It is from analysis of the relative intensities of transitions that temperatures for the interstellar medium and the photospheres of stars may be determined. [Pg.71]

Figure 4.37. Computed interfaciai tension at the water-decane interface in the presence of CjQ - p SOgNa". Influence of branching. Temperature 25 C. (Redrawn after van Os et al., loc. cit.)... Figure 4.37. Computed interfaciai tension at the water-decane interface in the presence of CjQ - p SOgNa". Influence of branching. Temperature 25 C. (Redrawn after van Os et al., loc. cit.)...
In this section we consider experimental results on the dependence of on molecular weight, polymer chain dimensions and architecture (whether linear or branched), temperature and diluent. We cast our results in forms suggested by theory whenever practicable. The existing theoretical calculations of 7j and comparisons with the empirical relations are reviewed in section 3. [Pg.263]

Kraftt temperature of octadecylalcohol sulfate (methyl branch) Temperature = degrees celslus... [Pg.130]

Beyond propane, it is possible to arrange the carbon atoms in branched chains while maintaining the same number of hydrogen atoms. These alternative arrangements are called isomers, and display slightly different physical properties (e.g. boiling point, density, critical temperature and pressure). Some examples are shown below ... [Pg.91]

Seeley J V, Morris R A, Viggiano A A, Wang FI and Flase W L 1997 Temperature dependencies of the rate constants and branching ratios for the reactions of Cr(Fl20)g 3 with CFIjBr and thermal dissociation rates for CI (CFl3Br) J. Am. Chem. Soc. 119 577-84... [Pg.825]

FIGURE 2 12 Boiling points of unbranched alkanes and their 2 methyl branched iso mers (Temperatures in this text are expressed in de grees Celsius C The SI unit of temperature is the kelvin K To convert degrees Celsius to kelvins add 273 15 )... [Pg.80]

Irregularities such as branch points, comonomer units, and cross-links lead to amorphous polymers. They do not have true melting points but instead have glass transition temperatures at which the rigid and glasslike material becomes a viscous liquid as the temperature is raised. [Pg.1006]

Fig. 4.29 Adsorption isotherms of water vapour on caldte, after being balt-milted for different periods (A, B, C) and on precipitated calcium carbonate (D). Period of milling (A) 1000h (B) ISOh (C) 22h outgassing temperature 2S°C. Isotherms A, B and C (but not D) all showed extensive low-pressure hysteresis, but for clarity the desorption branch is omitted. The amount adsorbed is referred to 1 m of BET-nitrogen area. ... Fig. 4.29 Adsorption isotherms of water vapour on caldte, after being balt-milted for different periods (A, B, C) and on precipitated calcium carbonate (D). Period of milling (A) 1000h (B) ISOh (C) 22h outgassing temperature 2S°C. Isotherms A, B and C (but not D) all showed extensive low-pressure hysteresis, but for clarity the desorption branch is omitted. The amount adsorbed is referred to 1 m of BET-nitrogen area. ...
Type V isotherms of water on carbon display a considerable variety of detail, as may be gathered from the representative examples collected in Fig. 5.14. Hysteresis is invariably present, but in some cases there are well defined loops (Fig. 5.14(b). (t ), (capillary-condensed water. Extreme low-pressure hysteresis, as in Fig. 5.14(c) is very probably due to penetration effects of the kind discussed in Chapter 4. [Pg.266]

We noted above that the presence of monomer with a functionality greater than 2 results in branched polymer chains. This in turn produces a three-dimensional network of polymer under certain circumstances. The solubility and mechanical behavior of such materials depend critically on whether the extent of polymerization is above or below the threshold for the formation of this network. The threshold is described as the gel point, since the reaction mixture sets up or gels at this point. We have previously introduced the term thermosetting to describe these cross-linked polymeric materials. Because their mechanical properties are largely unaffected by temperature variations-in contrast to thermoplastic materials which become more fluid on heating-step-growth polymers that exceed the gel point are widely used as engineering materials. [Pg.314]

The intensity distribution among the rotational transitions is governed by the population distribution among the rotational levels of the initial electronic or vibronic state of the transition. For absorption, the relative populations at a temperature T are given by the Boltzmann distribution law (Equation 5.15) and intensities show a characteristic rise and fall, along each branch, as J increases. [Pg.257]

Unless the cavity is tuned to a particular wavelength the vibration-rotation transition with the highest gain is the P-branch transition involving the rotational level which has the highest population in the 3 state. This is P(22), with J" = 22 and J = 21, at normal laser temperatures. The reason why this P-branch line is so dominant is that thermal redistribution of rotational level populations is faster than the population depletion due to emission. [Pg.359]

When -xylene is used as the monomer feed in a plasma polymer process, PX may play an important role in the formation of the plasma polymer. The plasma polymer from -xylene closely resembles the Gorham process polymer in the infrared, although its spectmm contains evidence for minor amounts of nonlinear, branched, and cross-linked chains as well. Furthermore, its solubiUty and low softening temperature suggest a material of very low molecular weight (15). [Pg.430]

Psychrometrics. Psychrometrics is the branch of thermodynamics that deals specifically with moist air, a biaary mixture of dry air and water vapor. The properties of moist air are frequentiy presented on psychrometric charts such as that shown ia Figure 2 for the normal air conditioning range at atmospheric pressure. Similar charts exist for temperatures below 0°C and above 50°C as well as for other barometric pressures. AH mass properties ate related to the mass of the dry air. [Pg.353]


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See also in sourсe #XX -- [ Pg.430 ]

See also in sourсe #XX -- [ Pg.19 ]

See also in sourсe #XX -- [ Pg.19 ]




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Branching at Different Temperatures

Branching melting temperature

Chain branching glass transition temperature

Effects of Branching on Apparent Theta-Temperature

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