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Density-temperature relationship

Viscometry measurements were made in benzene at 30 °C and in TFE at 50 °C with uncalibrated Cannon-Ubbelohde dilution viscometers which gave solvent times greater than 100 seconds. The viscometers used had centistoke ranges denoted by viscometer sizes of 50 and 75 for benzene and TFE, respectively. Stock solutions were made up on gram solute/100 gram solution basis and converted to gram/deciliter via the solvent density at the temperature of measurement. The solvent densities used were d ene = 0.8686 (11a) and dlra = 1.3429 obtained from pycno-metric measurements (12). The density—temperature relationship for TFE obtained from regression analysis of the experimental pycnometric data is... [Pg.133]

There are two main classifications of convection, forced and natural. Forced convection is fluid motion that is a result of forced input, such as a fan or pump. Natural convection is a result of density gradients in the flow which cause motion. In forced convection, there is also often a component of natural convection, but this is typically dominated by the forced convection effects. The density gradients in the flow, which are the genesis of natural convection, can be caused by either temperature or solutal buoyancy effects. Temperature effects are simply a result of the density-temperature relationship for a fluid. These effects can be illustrated by imagining a window in a warm apartment on a cold winter day (see Figure 5.41). At the inside surface of the window, the air in the room is cooled by the window and increases in density, sinks down along the window, and causes an uncomfortable draft. [Pg.268]

Figure 10.9. Specific heat-temperature relationships for low-density polyethylene, high-density polyethylene and polystyrene." (The Distillers Company Ltd.)... Figure 10.9. Specific heat-temperature relationships for low-density polyethylene, high-density polyethylene and polystyrene." (The Distillers Company Ltd.)...
In the case of gaseous contaminants, the tracer gas is selected to simu late as well as possible the properties (density, temperature) and momentum of the real contaminant. It is essential to ensure that the tracers arc nontoxic, chemically nonreactive, nonadsorptive on indoor surfaces, and inexpensive. The mixing of the tracer with the actual gaseous contaminant before its release or the release of the tracer with a density near that of the air will improve the validity of the simulation. With tracers, the most difficult task in practice is the relationship of the discharge between the tracer and the real contaminant. Case-by-case techniques to release the tracer are necessary in practice. With tracer gases, the procedure for capture efficiency is described in detail in the European Standard. - The tracer gas concentrations are measured in the exhaust duct for two release locations as illustrated in Fig. 10.108. [Pg.1017]

Materials. Samples of dewatered crude oils were obtained from the Athabasca oil sands of the McMurray formation by extraction using the commercial hot water process (Suncor Inc.) the Bl uesky-Bu11 head formation at Peace River, Alberta by solvent extraction of produced fluids the Clearwater formation at Cold Lake, Alberta by solvent extraction of core material and the Karamay formation in Xing-Jiang, China. A summary of the physical and chemical properties of the crude oils, including chemical composition, and density-temperature and viscosity-temperature relationships, is given in Table I. [Pg.330]

Density - Detonation Pressure and Density -Temperature of Detonation Relationships. [Pg.211]

Density - Temperature of Detonation Relationship. See under Detonation Pressure Charge Density and Temperature of Detonation - Charge Density Relationships... [Pg.211]

Phys 29, 630(1957) (Density-temperature of detonation relationship for some expls)... [Pg.492]

As mentioned above, this work was conducted at the BurMines and its description is scattered in various Progress Repts. Part of this work concerning Density-Temperature of Detonation Relationship is reported in this Volume under Density-Pressure of Detonation and Density-Temperature of Detonation Relationships, where the BurMines Progr Repts are listed as Refs 2 3... [Pg.597]

The density-pressure relationship for powder compaction at room temperature typically increases from the apparent density at zero pressnre to values that approach the theoretical density at high pressures, as illustrated in Figure 7.16. A compact with 100% theoretical density would indicate that it contains no porosity. Soft powders are more easily densified than hard powders at a given pressnre, and irregularly shaped powders have lower densities than spherical powders in the low-pressure regime. [Pg.701]

In reality, however, the synergistic effects of density, temperature, and composition on retention (In k ) will necessitate the inclusion of one or more cross terms in equation 5, at least for some sets of experimental conditions. Since the precise relationship depends on the parent fluid, the modifier, and the location of the experimental conditions relative to the critical point, it is often difficult to make intuitive predictions about which cross-terms, if any, should be included. Such predictions may become easier as the knowledge base of SFC continues to grow. [Pg.313]

The reduced density, temperature, and pressure along with the characteristic temperature, pressure, and volume are calculated from the following relationships. [Pg.12]

Although amorphous pharmaceutical materials can be readily isolated and may persist for many thousands of years,they are in fact a thermodynamically metastable state and will eventually revert to the more stable crystalline form. Fig. 4 shows a snapshot in time of the free energy-temperature relationship for a material that can be isolated as both an amorphous form and a crystalline form. This quasi-equilibrium thermodynamic view of the amorphous state shows that the amorphous form has a significantly higher free energy than the crystalline form, and illustrates why it is expected to have a much higher aqueous solubility and significantly different physical properties (e.g., density). [Pg.86]

Correlations for the key volumetric properties (the van der Waals volume and the molar volumes, densities and coefficients of thermal expansion of amorphous polymers) will be developed in Chapter 3 followed by discussions of pressure-volume-temperature relationships and of the effects of crystallinity on the density. [Pg.54]

Since the enhancement was observed at high current densities, one may ascribe this behaviour to a better ion transport through the membrane under such conditions. Yet, this conjecture is not supported by the analysis of the cell resistance-temperature relationship (Fig. 7). [Pg.42]

Interaction increases quadratically with the step density (b) Relationship between the projected surface free energy and the crystal shape as a function of temperature. [Pg.497]

The epoxy is a crosslinked system with a well-defined Tg. The temperature dependency of the modulus in such materials is related to the crosslink density. The relationship of the DTUL modulus to the room temperature modulus in this case is similar to that observed for the PET. However, in this case the crosslinked system provides an extended region of stability well beyond Tg and the DTUL. Thus, while both thermoplastic systems are no longer solid above 250 "C, the epoxy has structural integrity and virtually the same modulus at 300 "C as it has at 250 C. It is therefore still serviceable for short-term excursions above the DTUL and may prove useful for extended periods under reduced loads providing that it possesses good thermal and oxidative stability. [Pg.583]

The relationships of temperature to vapor pressure, density, specific gravity, and latent heat for liquid ammonia are shown in Table 1. Vapor pressure-temperature and density-temperature curves are shown in Figs. 1 and 2, respectively. Values of thermodynamic properties of liquid... [Pg.242]

Another useful compilation of physical data is Pressure-volume-temperature Relationships of Organic Compounds, by R. R. Dreisbach (Sandusky, 1952). Azeotropic Data are given in volume 6 of the Advances in Chemistry series and in Physical and Azeotropic Data by G. Claxton (London, National Benzole and Allied Products Association, 1958) which lists melting point, boiling point, density and refractive index for hydrocarbons and sulphur compounds boiling below 200°C. Information is also given on azeotrope formation. [Pg.110]


See other pages where Density-temperature relationship is mentioned: [Pg.304]    [Pg.74]    [Pg.699]    [Pg.304]    [Pg.74]    [Pg.699]    [Pg.438]    [Pg.443]    [Pg.325]    [Pg.9]    [Pg.73]    [Pg.153]    [Pg.196]    [Pg.182]    [Pg.163]    [Pg.295]    [Pg.449]    [Pg.454]    [Pg.587]    [Pg.32]    [Pg.81]    [Pg.333]    [Pg.358]    [Pg.29]    [Pg.247]    [Pg.24]    [Pg.421]    [Pg.188]   
See also in sourсe #XX -- [ Pg.241 ]




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Temperature, relationship

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