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Water vapor, partial pressure

Pressure, water vapor partial The pressure that the water vapor in air would exert if it alone occupied the volume of the humid air at the same temperature, in kPa. [Pg.1469]

Volatile can account for up to 40% of the total heat release. Devolatilization involves release of tar, CO, and other hydrocarbons. The rate of volatile release depends upon the temperature of the bed, heating rate, pressure, water vapor partial pressure, and the particle size. [Pg.172]

Temperature rc) Humidity kg HjO/kg dry air) Water vapor partial pressure (kPa) Water v K>r partial density (kg/m ) Water vaporization heat M/kg) Mixture enthalpy (kj/kg dry air) Dry air partial density (lKinematic viscosity (I0< mJ/s) Specific heat (kJ/K kg) Heat conductivity (W/m K) Diffusion factor water air (1 O mJ/s) Temperature rc)... [Pg.82]

Psychrometric coefficient The coefficient in the equation for the determination of the water vapor partial pressure from the wet bulb depression. [Pg.1470]

Fig. 1.82.2. Water vapor partial pressure divided by total pressure as a function of time of a 5 % bovine serum albumin (Fig. 3 from [1.137]). Fig. 1.82.2. Water vapor partial pressure divided by total pressure as a function of time of a 5 % bovine serum albumin (Fig. 3 from [1.137]).
Fig. 3-42 Methanol oxidation current of Nafion SFE Pt electrode after 2 min. cf potential holding at 500 mV or 600 mV atTff C. Methanol was fed throu gas phase at various partial pressures, water vapor pressure 0, electrolyte 3 M H2S04... Fig. 3-42 Methanol oxidation current of Nafion SFE Pt electrode after 2 min. cf potential holding at 500 mV or 600 mV atTff C. Methanol was fed throu gas phase at various partial pressures, water vapor pressure 0, electrolyte 3 M H2S04...
Hence the maximum air feed actual stoichiometry is a function of water vapor partial pressure corresponding to the air exhaust release temperature (pw) and the total pressure on the air cathode exhaust (ptotai)- Figure 2.8 shows the maximum air feed actual stoichiometry calculated from Equation 2.5, using water vapor partial pressure from the CRC Handbook of Chemistry and Physics [D.R. Lide (ed.), 72nd edn, 1991-92], as a function of air cathode exhaust release temperature. [Pg.57]

On the inlet side of the gas ballast pump a water vapor partial pressure p 2 is always present, which is at least as large as the saturation vapor pressure of water at the coolant temperature. This ideal case is realizable in practice only with a very large condenser (see above). [Pg.40]

In this region the vrater vapor pressure exceeds the admissible partial pressure at the inlet. The gas ballast pump must, therefore, have a condenser inserted at the inlet, which is so rated that the water vapor partial pressure at the inlet port of the rotary pump does not exceed the admissible value. The correct dimensions of the condenser are selected depending on the quantity of water vapor involved. For further details, see... [Pg.63]

The lower limit of the water vapor partial pressure is determined through the compression ratio of the Roots pump at the backing pressure, w/hich is determined by the saturation vapor pressure of the condensed water. Also, in this region the intermediate condenser must be able to reduce the vapor partial pressure to at least 60 mbar. The stated arrangement is suitable -when cooling the condenser with water at 15 °C - tor water vapor pressures between about 4 and 40 mbar. [Pg.64]

Eg A/here E is the moisture content before drying q is the temperature-dependent coefficient. Thus equation (2.31) serves only for the temperature at which q was determined K is a factor that depends on the temperature, the water vapor partial pressure in the vicinity of the material, the dimensions, and the... [Pg.64]

Eressure is determined by the water vapor partial pressure, which is carefully ept at saturation with respect to the equilibrium vapor pressure of water at the droplet temperature so that the droplets neither grow nor evaporate. Depending on the temperature of the droplets this sets the minimum pressure at 4 to 20 Torr. The transit time of the droplets through the reaction zone is short, on the order of a few milliseconds, in order to avoid saturation of the trace gas in the liquids. Experimental parameters are computer monitored. The details of the technique and of the experimental procedures are discussed in reference (2). [Pg.508]

With continuing exposure to oxygen compounds, irreversible damage to catalyst activity may occur due to the growth of iron primary crystallites. This damage depends on the water vapor partial pressure and is especially serious at high temperatures. [Pg.175]

The intraannual changes in the water vapor partial pressure follow the annual trend of the air temperature over the sea (Fig. 7a). The lowest values are observed in January and February, while the highest are confined to July and August. During the entire year, the spatial distribution of the water vapor contents also corresponds to the air temperature distribution. The lowest values of the partial pressure of water vapor are noted in the northwest of the Black Sea (4.7-20 hPa on the coast and 5.0-21.0 hPa over the sea). The water vapor content grows in the southeastern direction (7.2-23.4 hPa on the coast and 8.0-24.0 hPa over the sea). [Pg.145]

Carrier s equation expresses actual water-vapor partial pressure in terms of wet-bulb and dry-bulb temperatures ... [Pg.598]

Figure 2-16. Relation between relative humidity and the partial pressure of water vapor at the indicated temperatures. The maximum water vapor partial pressure occurs at 100% relative humidity. Figure 2-16. Relation between relative humidity and the partial pressure of water vapor at the indicated temperatures. The maximum water vapor partial pressure occurs at 100% relative humidity.
As solutes are added to the liquid phase and the mole fraction of water is thereby lowered, water molecules have less tendency to leave the solution. Hence, the water vapor partial pressure in the gas phase at equilibrium becomes less —this is one of the colligative properties of solutions that we mentioned earlier. In fact, adjacent to dilute solutions P at equilibrium depends linearly on the mole fraction of water (Nw) in the liquid phase. This is Raoult s law (also mentioned in Appendix IV). For pure water, Nw equals 1 and Pwv has its maximum value, namely P w> the saturation vapor pressure. [Pg.85]

As we can see from relations such as Equation 8.2 (J = gjAcj = ACjlrj), the conductances or the resistances of the various parts of the pathway determine the drop in concentration across each component when the flux density is constant. Here we will apply this condition to a consideration of water vapor concentration and mole fraction in a leaf, and we will also consider water vapor partial pressures. In addition we will discuss the important effect of temperature on the water vapor content of air (also considered in Chapter 2, Section 2.4C). [Pg.385]


See other pages where Water vapor, partial pressure is mentioned: [Pg.187]    [Pg.2227]    [Pg.1397]    [Pg.144]    [Pg.144]    [Pg.687]    [Pg.191]    [Pg.194]    [Pg.195]    [Pg.111]    [Pg.401]    [Pg.55]    [Pg.27]    [Pg.39]    [Pg.39]    [Pg.40]    [Pg.63]    [Pg.65]    [Pg.290]    [Pg.56]    [Pg.187]    [Pg.116]    [Pg.119]    [Pg.146]    [Pg.76]    [Pg.12]    [Pg.428]    [Pg.85]   
See also in sourсe #XX -- [ Pg.1470 ]




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