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High pressure diagram

Figure 3.8a shows the temperature-composition diagram for a minimum-boiling azeotrope that is sensitive to changes in pressure. This azeotrope can be separated using two columns operating at different pressures, as shown in Fig. 3.86. Feed with mole fraction of A Ufa)) of, say, 0.3 is fed to the high-pressure column. The bottom product from this high-pressure column is relatively pure B, whereas the overhead is an azeotrope with jcda = 0-8, jcdb = 0.2. This azeotrope is fed to the low-pressure column, which produces relatively pure A in the bottom and in the overhead an azeotrope with jcda = 0.6, jcdb = 0.4. This azeotrope is added to the feed of the high-pressure column. Figure 3.8a shows the temperature-composition diagram for a minimum-boiling azeotrope that is sensitive to changes in pressure. This azeotrope can be separated using two columns operating at different pressures, as shown in Fig. 3.86. Feed with mole fraction of A Ufa)) of, say, 0.3 is fed to the high-pressure column. The bottom product from this high-pressure column is relatively pure B, whereas the overhead is an azeotrope with jcda = 0-8, jcdb = 0.2. This azeotrope is fed to the low-pressure column, which produces relatively pure A in the bottom and in the overhead an azeotrope with jcda = 0.6, jcdb = 0.4. This azeotrope is added to the feed of the high-pressure column.
The hysteresis loops to be found in the literature are of various shapes. The classification originally put forward by de Boer S in 1958 has proved useful, but subsequent experience has shown that his Types C and D hardly ever occur in practice. Moreover in Type B the closure of the loop is never characterized by the vertical branch at saturation pressure, shown in the de Boer diagrams. In the revised classification presented in Fig. 3.5, therefore. Types C and D have been omitted and Type B redrawn at the high-pressure end. The designation E is so well established in the literature that it is retained here, despite the interruption in the sequence of lettering. [Pg.116]

Even at the lowest temperatures, a substantial pressure is required to soHdify helium, and then the soHd formed is one of the softest, most compressible known. The fluid—soHd phase diagrams for both helium-3 and helium-4 are shown in Eigure 1 (53). Both isotopes have three allotropic soHd forms an fee stmeture at high pressures, an hep stmeture at medium and low pressures, and a bcc stmeture over a narrow, low pressure range for helium-4 and over a somewhat larger range for helium-3. The melting pressure of helium-4 has been measured up to 24°C, where it is 11.5 GPa (115 kbar) (54). [Pg.7]

In addition to the three principal polymorphs of siUca, three high pressure phases have been prepared keatite [17679-64-0] coesite, and stishovite. The pressure—temperature diagram in Figure 5 shows the approximate stabiUty relationships of coesite, quart2, tridymite, and cristobaUte. A number of other phases, eg, siUca O, siUca X, sihcaUte, and a cubic form derived from the mineral melanophlogite, have been identified (9), along with a stmcturaHy unique fibrous form, siUca W. [Pg.474]

Fig. 51eft. Schematic flow diagram of an ethylene plant using naphtha feedstock. CW = cooling water QW = quench water QO = quench oil LPS = low pressure steam MPS = medium pressure steam SPS = super high pressure steam C3R = propylene refrigerant and... Fig. 51eft. Schematic flow diagram of an ethylene plant using naphtha feedstock. CW = cooling water QW = quench water QO = quench oil LPS = low pressure steam MPS = medium pressure steam SPS = super high pressure steam C3R = propylene refrigerant and...
If reheat is introduced between a high pressure turbine and a low pressure turbine then examination of the T,s diagram (Fig. 3.4a) shows that the complete cycle is now made up... [Pg.30]

A reversible cycle with turbine expansion split into two steps (high pressure, HP, and low pressure, LP) is illustrated in the T, s diagram of Fig. 4.3. The mass flow through the heater is still unity and the temperature rises from T2 to Tt, = Tq hence the heat supplied (3b is unchanged, as is the overall isentropic temperature ratio (x). But cooling air of mass flow i//H is used at entry to the first HP turbine (of isentropic temperature ratio. xh) and additional cooling of mass flow is introduced subsequently into the LP turbine (of isentropic temperature ratio Xl)- The total cooling flow is then i/( = i/ h + >h.-... [Pg.51]

Figure 1-1 is a block diagram of a production facility that is primarily designed to handle gas wells. The well flow stream may require heating prior to initial separation. Since most gas wells flow at high pressure, a... [Pg.1]

A sehematie diagram of a heart-eut LC-LC system is depieted in Figure 5.4. The eolumn switehing teehnique was developed by employing two high-pressure four-way pneumatie valves inserted before and after the preeolumn (39). The front-eut and the end-eut of the sample eluted from the first eolumn were vented to waste. The valves were manipulated to transfer only the heart-eut of the analyte of interest to the analytieal eolumn. The detailed operational eonditions for the four-step sequenee of this system ean be deseribed as follows ... [Pg.123]

Figure 6.2 Schematic diagram showing the basic components of (a) SFE and (b) SFC instruments 1, carbon dioxide 2, high pressure pump 3, oven 4, exti action cell (SFE) or column (SFC) 5, collection vial (SFE) or data system (SEC). Figure 6.2 Schematic diagram showing the basic components of (a) SFE and (b) SFC instruments 1, carbon dioxide 2, high pressure pump 3, oven 4, exti action cell (SFE) or column (SFC) 5, collection vial (SFE) or data system (SEC).
Figure 6.3 Schematic diagram of an on-line SFE-GC instmment 1, carbon dioxide 2, high-pressure syringe pump 3, tliree-poit valve 4, extraaion cell 5, oven 6, gas cliromato-graph. Figure 6.3 Schematic diagram of an on-line SFE-GC instmment 1, carbon dioxide 2, high-pressure syringe pump 3, tliree-poit valve 4, extraaion cell 5, oven 6, gas cliromato-graph.
The shaded region is that part of the phase diagram where liquid and vapor phases coexist in equilibrium, somewhat in analogy to the boiling line for a pure fluid. The ordinary liquid state exists on the high-pressure, low-temperature side of the two-phase region, and the ordinary gas state exists on the other side at low pressure and high temperature. As with our earlier example, we can transform any Type I mixture... [Pg.154]

Figure 1 Schematic diagram of formation of ECC by crystallization under high pressure. (From Ref. 18.)... Figure 1 Schematic diagram of formation of ECC by crystallization under high pressure. (From Ref. 18.)...
The high-pressure study on the Ti-H alloys showed stress-strain properties are not the only ones which are affected by pressure, but phase equilibria are also strongly dependent on this parameter . A new ( -phase and a corresponding single phase region in the isobaric T — C section of the T — P — C phase diagram appear in the... [Pg.434]


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See also in sourсe #XX -- [ Pg.759 , Pg.760 ]




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High-pressure Phase Diagrams and Critical Properties of Fluid Mixtures

Pressure diagram

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