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Equilibrium water content

Figures 16-18 and 16-19 give the dew-point water-vapor content of a nitrogen-free. natural gas in equilibrium with liquid water. Figures 16-18 and 16-19 give the dew-point water-vapor content of a nitrogen-free. natural gas in equilibrium with liquid water.
The physical state of materials is often defined by their thermodynamic properties and equilibrium. Simple one-component systems may exist as crystalline solids, liquids or gases, and these equilibrium states are controlled by pressure and temperature. In most food and other biological systems, water content is high and the physieal state of water often defines whether the systems are frozen or liquid. In food materials science and characterization of food systems, it is essential to understand the physical state of food solids and their interactions with water. Equilibrium states are not typical of foods, and food systems need to be understood as nonequilibrium systems with time-dependent characteristics. [Pg.67]

Electrolytes are subject to dissociation into negatively charged anions and positive cations. The vital electrolyte balance guarantees the respective uptake and discharge and ensures the correct presence and distribution. This regulatory process is closely linked to the water equilibrium. The intracellular and extracellular spaces differ in their electrolyte content, (s. tab. 16.1)... [Pg.288]

Liquid water, sometimes referred as free liquid water, is present in the porous structure at moisture contents above the fibre saturation point, here assumed constant at all temperatures 0.2 kg water per kg dry wood. The rate of evaporation in Equation (3), C4,+b]ti is indirectly solved from Equation (2) for water vapour, j=HjO. In the presence of liquid water equilibrium v iour pressure is assumed in the gas phase described as 18] ... [Pg.1050]

Figure 3 Different methods of hydrate formation (1-5) each can give a distinct perspective on certain aspects of hydrate formation l-ice + gas at T< 273K 2- ice with the temperature ramped above T = 273K 3 - amorphous ice +gas at T < 13 OK 4 and 5, either quiescent or with agitation are usually used for phase equilibrium studies and the effect of inhibitors. Simulation of natural gas hydrate requires the addition of sediment at various levels of water-sediment content. Figure 3 Different methods of hydrate formation (1-5) each can give a distinct perspective on certain aspects of hydrate formation l-ice + gas at T< 273K 2- ice with the temperature ramped above T = 273K 3 - amorphous ice +gas at T < 13 OK 4 and 5, either quiescent or with agitation are usually used for phase equilibrium studies and the effect of inhibitors. Simulation of natural gas hydrate requires the addition of sediment at various levels of water-sediment content.
Weiss and co-workers reported solubilities for He, " He, Ne, Ar, Kr as well as for O2 and N2 as a function of temperature and salinity for fresh and ocean waters (Table 1 Weiss 1970, 1971 Weiss and Kyser 1978). As this fundamental piece of work was strongly motivated by practical oceanographic research, the noble gas solubilities were expressed in the form of equilibrium concentrations with moist atmospheric air. For the atmosphere, it is justified to assume that its major elemental composition remains constant over the relevant time scales controlling gas exchange. Hence the gas partial pressure pi can be expressed by the total atmospheric pressure ptot corrected for water vapor content, Cw(T), and the volume or mole fraction Zi of the gas i in dry air (Ozima and Podosek 1983). [Pg.620]

Aluminum silicate solubility in water, according to these reactions, may be calculated from equilibrium content of AP in the saturated solution in consideration of its complexation function 3+. Then the solubility equations of the minerals under consideration are... [Pg.268]

Thermodynamic models that determine the equilibrium temperature distribution for an atmospheric column and the underlying surface, subject to prescribed solar radiation at the top of the atmosphere and prescribed atmospheric composition and surface albedo. Submodels for the transfer of solar and terrestrial radiation, the heat exchange between the earth s surface and atmosphere, the vertical redistribution of heat within the atmosphere, the atmospheric water vapor content and clouds are included in these one-dimensional models. Abbreviated as RCM. radiatively active gases... [Pg.207]

Crosslinked poly(2-hydroxyethylmethacrylate), PHEMA, has been prepared by radical polymerization in presence of different amounts of water and water-diacetine solutions. While homogeneous samples can be prepared at all water-diacetine content, amounts of water higher than 40% causes the formation of macroporous opaque sponges. Mechanical properties of water swollen samples have been measured and related to the crosslink formation during the polymerization process. From water diffusion kinetics in sorption and desorption experiments at 37 C the diffusion coefficients have been calculated. Measurements of the swelling at equilibrium in water-diacetine mix-res indicate the presence of "cosolvency" phenomenon for the samples studied. [Pg.311]

As well as the sulfur cyde, there are other cycles in nature water, nitrogen, phosphorus and carbon. Man has influenced them all, but the sulfur cycle is the most disturbed among aU these cydic processes. Fossil fuels are burned in order to warm up houses and to provide cars, power stations and industries with energy. Then the sulfur that was built into coal, oil and natural gas, millions of years ago, is set free. It is transported as sulfur dioxide to the atmosphere, the SO content of which has increased considerably compared to the equilibrium content of the natural cyde. The acid gas is transported by the winds over the continents, and, long distances from a specific source, people experience a rain of sulfuric acid . This acid rain not only attacks the needles and leaves of trees but also damages the roots of plants. In acidified lakes the ability of fish to reproduce is disturbed. If acidification is not neutralized by liming, metal ions may be leached from rocks and damage animal life. [Pg.1057]

Soheilmoghaddam et al. (2014a, b) also reported the equilibrium content of RC and RC/GNS as a function the time conditioned at 75 % RH. It was observed that the water resistance of the nanocomposites improved with GNS incorporation. Water absorption of pure RC was 147 % but decreased by 40 % for the 0.75 wt% GNS nanocomposite. The presence of GNS in the RC nanocomposite films enhanced their water resistance. This was attributed to the less hydrophilicity of GNS in the RC matrix and also the potential hydrogen bond formation between GNS and RC. This partially blocks the hydrophilic site of RC owing to the presence of less OH group interaction with the water molecules. [Pg.312]

As is demonstrated by the results summarized in Tables I and II, introduction of water vapour into the carrier gas led to a decrease in the retention times of all the sorbates, compared with those obtained in the dry carrier gas. An analogous decrease in the retention times when using water vapour in the carrier gas was also described in e.g. the paper by Guillemin and Millet [18]. The authors employed much higher water vapour contents (above 10%) and classical adsorbents (silica gel, alumina, porous polymers). With cyclodextrins, a perceptible decrease in the retention occurs even for 0.8% water vapour in the carrier gas. This phenomenon can be explained by partial adsorption of water molecules on the stationary phase surface, in a similar manner to common adsorbents. However, the experimental results, especially those obtained with a-CD as the stationary phase (Table I), indicate an effect on the equilibrium in the formation of the sorbate-cyclodextrin inclusion complex, in favour of the free guest. A great excess of water vapour over the sorbate apparently leads to competitive inclusion of water molecules and thus to faster desorption of the guest. [Pg.302]

The influence of the partial pressure of the solute on its equilibrium content in the solvent, the loading Xabs> is shown in Figure 3.3.24 for a physical absorption of CO2 in water and methanol and a chemical absorption in an aqueous solution of monoethanolamine (MEA). [Pg.108]

Figure 7-13. Calculated activity of all potassium-containing vapor species for K2CO3 in equilibrium with a gas phase of 9CO2 102 at 1160 K as a function of water vapor content. (Pareek and Shores, 1991. Reprinted with permission of the American Ceramic Society.)... Figure 7-13. Calculated activity of all potassium-containing vapor species for K2CO3 in equilibrium with a gas phase of 9CO2 102 at 1160 K as a function of water vapor content. (Pareek and Shores, 1991. Reprinted with permission of the American Ceramic Society.)...
The water vapor content of saturated natural gas is also affected by gas composition. The presence of substantial concentrations of CO2 or H2S, for example, increases the equilibrium water concentration, particularly at pressures above 1,000 psia. This effect has been correlated by Robinson et al. (1978) for gas pressures from 1,000 to 10,(XX) psia and combined acid... [Pg.947]

FIO. 2 Equilibrium Water Vapor Content of Natural Gases... [Pg.205]

TABLE 3 Equilibrium Water Vapor Contents of Natural Gases Above the Critical Temperatures... [Pg.208]

Eormula (12.50) is related to the boundary conditions of water equilibrium in proton exchange membrane. It uses the principle of the adsorption isotherm when the membrane is under standard temperature. The water content of the formula is obtained by linear interpolation, that is, the boundary of the water content in the proton exchange membrane ... [Pg.563]

The Cg value, the concentration of the maximally freeze concentrated glass (see Glossary), for most carbohydrate solutions has a similar value (see Table 9.3). Highly viscous solutions do not reach equilibrium, and a cooling curve will follow the lower trajectory on graph 1.14 (see Chapter 1). This means that the concentration of water in the glass is actually above the equilibrium content, and subsequent heating will increase mobility such that the excess water can recrystallise to form ice. Both Tg and Cg will thus be difficult to obtain from simple measurements. [Pg.388]

Above the melting temperature of the polymer (PA 6 = 215 °C PA 12 = 180 °C) the equilibrium is established in a one-phase system. In the melt and for CL polymerization the equilibrium content of the monomer and water-extractable oligomers reaches 8-10wt% (see Section 7.6). On the other hand, the content of extractables for poly(co-laurolactam) is only 2 wt% and it is not necessary to remove this from the crude product. [Pg.171]


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See also in sourсe #XX -- [ Pg.155 , Pg.157 ]




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