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Vapor pressure water, liquid from

TABLE 2-4 Vapor Pressure of Liquid Water from -16 to 0"C ... [Pg.92]

Water was selected for the sealing liquid for which EG(Ethylene Glycol) could be a candidate. EG shows a very low vapor pressure but too high solubility for acetone. As acetone is less soluble in water than in EG, in spite of higher vapor pressure, water was used for sealing liquid and the moisture included in the emitted stream from the pump was supposed to be captured in diyers. [Pg.520]

Phase equilibrium is a dynamic process that is quite different from the static equilibrium achieved as a marble rolls to a stop after being spun into a bowl. In the equilibrium between liquid water and water vapor, the partial pressure levels off, not because evaporation and condensation stop, but because at equilibrium their rates become the same. The properties of a system at equilibrium are independent of the direction from which equilibrium is approached, a conclusion that can be drawn by observing the behavior of the liquid-vapor system. If we inject enough water vapor into the empty flask so that initially the pressure of the vapor is above the vapor pressure of liquid water, PvaplHiO)) then liquid water will condense until the same equilibrium vapor pressure is achieved (0.03126 atm at 25°C). Of course, if we do not use enough water vapor to exceed a pressure of 0.03126 atm, all the water will remain in the vapor phase and two-phase equilibrium will not be reached. [Pg.428]

Rain. Mercury in the gas phase is less readily taken up by water. In deaerated water under nitrogen the solubility is 20 to 30 /Ltg/liter (7). In distilled water saturated with air at 27°C it is 47 /Ltg/liter (24). The washout eflBciency of rain can be calculated from the ratio of the pressure of mercury vapor in air to the vapor pressure over liquid mercury at 20 °C, which is about 0.2 X 10" for an atmospheric concentration of... [Pg.58]

Nanocell is the smallest electrochemical cell developed by Sugimura and Nakagiri [11] and further developed and utilized for ENT by BloeB et al. [10]. The nanocell consists of two electrodes distance between electrodes is generally maintained in the order of less than 1 nm. In between two electrodes, absorbed water film acts as an electrolyte whose volume is maintained by vapor pressure and ranges from 10 to 10 cm. Double layer capacitance is not formed across the solid liquid interface in the nanocell due to the much smaller inter-electrode gap and hence, generated hydrogen ion and hydroxyl ion recombine immediately. Nanotip of microtool such as tip of scanning probe microscope (SPM) or AFM tip is most suitable for the formation of electrochemical nanoceU. [Pg.244]

It is important to note that in these calculations, it is assumed that the solute is in a dissolved form in both phases i.e., it is not present in sorbed, micelle, or colloidal forms. The concentrations must, of course, be less than the saturation values, which correspond to the solubility of the substance in the water phase and to the vapor pressure in the atmosphere. A convenient method of calculating Henry s constants is to express H as the ratio of the solute s saturation vapor pressure P as obtained from handbooks, to the solute s aqueous solubility C It is important that the state of the two phases (i.e., solid or liquid) be the same for both data. This has caused problems with PCBs in which the available solubility data tend to be those of the pure solid isomers, whereas the vapor pressure data are obtained by extrapolation from vapor pressures of liquid mixtures. It is essential that the two sets of data apply to the same solute physical condition. [Pg.308]

The liquids in Table 11.2 are listed in order of increasing molecular weight. Recall that London forces tend to increase with molecular weight. Therefore, London forces would be expected to increase for these liquids from the top to the bottom of the table. If London forces are the dominant attractive forces in these liquids, the vapor pressures should decrease from top to bottom in the table. And this is what you see, except for water and glycerol. (Their vapor pressures are relatively low, and an additional force, hydrogen bonding, is needed to explain them.)... [Pg.440]

When liquid molecules with sufficient kinetic energy break away from the surface, they become gas particles or vapor. In an open container, all the liquid will eventually evaporate. In a closed container, the vapor accumulates and creates pressure called vapor pressure. Each liquid exerts its own vapor pressure at a given temperature. As temperature increases, more vapor forms, and vapor pressure increases. Table 11.4 lists the vapor pressure of water at various temperatures. [Pg.367]

Vapor to Column Liquid from Column Center Water Flow Center Water Feed Top Water Flow Top Water Feed Vapor from Column Column Pressure Drop... [Pg.177]


See other pages where Vapor pressure water, liquid from is mentioned: [Pg.182]    [Pg.45]    [Pg.45]    [Pg.67]    [Pg.248]    [Pg.313]    [Pg.298]    [Pg.15]    [Pg.185]    [Pg.438]    [Pg.5087]    [Pg.3903]    [Pg.427]    [Pg.289]    [Pg.195]    [Pg.540]    [Pg.43]    [Pg.92]    [Pg.1177]    [Pg.131]    [Pg.914]    [Pg.473]    [Pg.137]    [Pg.152]    [Pg.78]    [Pg.1119]    [Pg.485]    [Pg.1101]    [Pg.551]    [Pg.1249]    [Pg.108]   
See also in sourсe #XX -- [ Pg.100 ]




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Liquids liquid water

Liquids vapor pressure

Pressurized water

Vapor Pressure (MPa) of Liquid Water from 0 to

Vapor Pressure of Liquid Water from -16 to

Vapor Pressure of Supercooled Liquid Water from 0 to

Vapor pressure water, supercooled liquid from

Water liquid

Water pressure

Water vapor

Water vapor pressure

Water vaporization

Water vaporization from

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