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Gas thermal properties

Example 7 Estimate the Vapor Pressure of Thiophene at 500 K.. . . Example 8 Estimate the Vapor Pressure of Acetaldehyde at 0 C. . . Ideal Gas Thermal Properties. [Pg.49]

The thermal properties of an ideal gas, enthalpy, entropy and specific heat, can be estimated using the method published by Rihani and Doraiswamy in 1965 ... [Pg.90]

An extensive new Section 10 is devoted to polymers, rubbers, fats, oils, and waxes. A discussion of polymers and rubbers is followed by the formulas and key properties of plastic materials. Eor each member and type of the plastic families there is a tabulation of their physical, electrical, mechanical, and thermal properties and characteristics. A similar treatment is accorded the various types of rubber materials. Chemical resistance and gas permeability constants are also given for rubbers and plastics. The section concludes with various constants of fats, oils, and waxes. [Pg.1287]

Ideal gas properties and other useful thermal properties of propylene are reported iu Table 2. Experimental solubiUty data may be found iu References 18 and 19. Extensive data on propylene solubiUty iu water are available (20). Vapor—Hquid—equiUbrium (VLE) data for propylene are given iu References 21—35 and correlations of VLE data are discussed iu References 36—42. Henry s law constants are given iu References 43—46. Equations for the transport properties of propylene are given iu Table 3. [Pg.123]

A substance is in the ideal gas state when the volume of its molecules is a zero fraction of the total volume taken up by the substance and when the individual molecules are far enough apart from each other so that there is no interaction between them. Although this only occurs at infinite volume and zero pressure, in practice, ideal gas properties can be used for gases up to a pressure of two atmospheres with little loss of accuracy. Thermal properties of ideal gas mixtures may be obtained by mole-fraction averaging the pure component values. [Pg.391]

The traditional unipolar diffusion charging model is based on the kinetic theory of gases i.e., ions are assumed to behave as an ideal gas, the properties of which can described by the kinetic gas theory. According to this theory, the particle-charging rate is a function of the square of the particle size dp, particle charge numbers and mean thermal velocity of tons c,. The relationship between particle charge and time according White s... [Pg.1223]

The zeolite-alumina tube is no more gas-tight after the thermal treatment. The presence or absence of the V-AI2O3 toplayer in the starting support does not influence the gas transport properties of the final zeolite-alumina tube. [Pg.132]

In our research, three chemical modification approaches were investigated bromination, sulfonylation, and acylation on the aromatic ring. The specific objective of this paper is to present the chemical modification on the PPO backbone by a variety of electrophilic substitution reactions and to examine the features that distinguish modified PPO from unmodified PPO with respect to gas permeation properties, polymer solubility and thermal behavior. [Pg.46]

Physical, thermal, and chemical stability in order to reduce operating costs, solid sorbents must demonstrate stability under flue gas conditions, adsorption operation conditions, and during the multi-cycle adsorption-regeneration process. In particular, stability in the presence of water vapor is essential for the sustainable performance of the solid sorbent. In addition to thermal properties of the solid sorbent, heat capacity and thermal conductivity are also important in heat transfer operations. [Pg.119]

In contrast to the strong effect of gas properties, it has been found that the thermal properties of the solid particles have relatively small effect on the heat transfer coefficient in bubbling fluidized beds. This appears to be counter-intuitive since much of the thermal transport process at the submerged heat transfer surface is presumed to be associated with contact between solid particles and the heat transfer surface. Nevertheless, experimental measurements such as those of Ziegler et al. (1964) indicate that the heat transfer coefficient was essentially independent of particle thermal conductivity and varied only mildly with particle heat capacity. These investigators measured heat transfer coefficients in bubbling fluidized beds of different metallic particles which had essentially the same solid density but varied in thermal conductivity by a factor of nine and in heat capacity by a factor of two. [Pg.162]

There are at present some actual and potential problems of varying degrees of severity with PBDS. The simplest of these involves the obvious fact that the sample must be in contact with a gas which itself must be pure, unreactive, and have suitable refractive and thermal properties. There is thus a potential... [Pg.412]


See other pages where Gas thermal properties is mentioned: [Pg.381]    [Pg.391]    [Pg.191]    [Pg.385]    [Pg.395]    [Pg.276]    [Pg.381]    [Pg.391]    [Pg.191]    [Pg.385]    [Pg.395]    [Pg.276]    [Pg.158]    [Pg.432]    [Pg.547]    [Pg.516]    [Pg.459]    [Pg.606]    [Pg.143]    [Pg.106]    [Pg.53]    [Pg.797]    [Pg.798]    [Pg.442]    [Pg.1317]    [Pg.208]    [Pg.151]    [Pg.46]    [Pg.211]    [Pg.391]    [Pg.399]    [Pg.469]    [Pg.474]    [Pg.162]    [Pg.314]    [Pg.169]    [Pg.247]    [Pg.488]    [Pg.340]   
See also in sourсe #XX -- [ Pg.191 ]




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Transport and thermal properties of gases

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