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Vaporization, heat composition

The solution at composition x is heated to its boiling point at Tx, producing vapor of composition x2 (enriched in low-boiling component A). [Pg.247]

The bypassed vapor heats up the liquid there, thereby causing the pressure to rise. WTien the bypass is closed, the pressure falls. Sufficient heat transfer surface is provided to subcool the condensate, (f) Vapor bypass between the condenser and the accumulator, with the condenser near ground level for the ease of maintenance When the pressure in the tower falls, the bypass valve opens, and the subcooled liquid in the drum heats up and is forced by its vapor pressure back into the condenser. Because of the smaller surface now exposed to the vapor, the rate of condensation is decreased and consequently the tower pressure increases to the preset value. With normal subcooling, obtained with some excess surface, a difference of 10-15 ft in levels of drum and condenser is sufficient for good control, (g) Cascade control The same system as case (a), but with addition of a TC (or composition controller) that resets the reflux flow rate, (h) Reflux rate on a differential temperature controller. Ensures constant internal reflux rate even when the performance of the condenser fluctuates, (i) Reflux is provided by a separate partial condenser on TC. It may be mounted on top of the column as shown or inside the column or installed with its own accumulator and reflux pump in the usual way. The overhead product is handled by an alter condenser which can be operated with refrigerant if required to handle low boiling components. [Pg.51]

In a dew point flash, the fraction vapor is set at the unity limit, at a specified temperature or pressure. The dependent variables are the pressure or temperature, the heat duty, and the liquid and vapor compositions. The only product is a saturated vapor with composition equal to that of the feed. The equilibrium liquid composition corresponds to the first liquid drop resulting from infinitesimal condensation. As in the bubble point flash, dew points can exist only within certain ranges of temperature and pressure. Referring to Figure 2.1, no dew points can exist at temperatures above the cricondentherm or at pressures above the cricondenbar. At temperatures or pressures where retrograde condensation can occur, there can be two dew points a normal dew point and a retrograde dew point. [Pg.82]

The froth on the tray is where mass transfer takes place between the phases, assumed to exist at equilibrium at the vapor-liquid interface. The well mixed liquid phase is at its bubble point temperature at equilibrium with the vapor interfacial composition Y. The vapor leaving tray j with composition Fy, is at temperature Ty, determined by heat transfer rates according to Equations 14.17 and 14.18. This temperature may be above the dew point. [Pg.510]

Ta, when heated to T, will produce the first bubble of equilibrium vapor of composition >>a- Conversely, a superheated vapor of composition Ya at T2, when cooled to Ti, will condense, the first drop of liquid being of composition Xa. Figure 3.2a also shows that, in general, complete vaporization or condensation of a binary mixture occurs over a range of temperatures, rather than at a single temperature as with a pure substance. [Pg.439]

Fig. 8.3.A-1 shows the concentrations in the liquid and the volume of the latter as a function of time Fig. 8.3.A-2 shows the temperature of the reactor contents, T, and the inlet and exit temperatures of the heat exchanging medium, and respectively and Fig. 8.3. A-3 the vapor-phase composition and vapor withdrawal rate, ... Fig. 8.3.A-1 shows the concentrations in the liquid and the volume of the latter as a function of time Fig. 8.3.A-2 shows the temperature of the reactor contents, T, and the inlet and exit temperatures of the heat exchanging medium, and respectively and Fig. 8.3. A-3 the vapor-phase composition and vapor withdrawal rate, ...
The assumption of equal molal latent heats greatly simplifies the calculations. If 1 mole of vapor (any composition) is condensed, the heat that is removed is just sufficient to vaporize a mole of liquid (at its boiling point). Thus the number of moles of vapor that travel up the column is tiie same at any plate, provided that the feed is introduced as a liquid at its boiling point. Likewise, the reflux or overflow from plate to plate is a constant amount in each section of the tower (see envelope II, Mg. 16-18) because the reflux is equal to the moles of vapor minus the moles of product for the rectifying section and to moles of vapor plus moles of waste for the eidukusting section. [Pg.502]

Environmental Aging. AH ceUular polymers are subject to a deterioration of properties under the combined effects of light or heat and oxygen. The response of ceUular materials to the action of light and oxygen is governed almost entirely by the composition and state of the polymer phase (22). Expansion of a polymer into a ceUular state increases the surface area reactions of the foam with vapors and Hquids are correspondingly faster than those of soHd polymer. [Pg.415]


See other pages where Vaporization, heat composition is mentioned: [Pg.313]    [Pg.313]    [Pg.51]    [Pg.246]    [Pg.124]    [Pg.119]    [Pg.123]    [Pg.246]    [Pg.428]    [Pg.51]    [Pg.246]    [Pg.51]    [Pg.66]    [Pg.226]    [Pg.124]    [Pg.994]    [Pg.41]    [Pg.327]    [Pg.113]    [Pg.129]    [Pg.193]    [Pg.324]    [Pg.753]    [Pg.198]    [Pg.532]    [Pg.105]    [Pg.123]    [Pg.525]    [Pg.439]    [Pg.501]    [Pg.166]    [Pg.207]    [Pg.353]    [Pg.614]    [Pg.1911]    [Pg.88]    [Pg.389]    [Pg.39]    [Pg.43]    [Pg.253]   
See also in sourсe #XX -- [ Pg.195 , Pg.261 , Pg.297 ]

See also in sourсe #XX -- [ Pg.195 , Pg.261 , Pg.297 ]




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Vapor composition

Vaporization, heat

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