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Two-step cooling

Fig. 4.3. Temperature-entropy diagram for two step cooling, (a) Cooling air taken at appropriate pre.ssures and (b) LP cooling air throttled from compressor exit. Fig. 4.3. Temperature-entropy diagram for two step cooling, (a) Cooling air taken at appropriate pre.ssures and (b) LP cooling air throttled from compressor exit.
For two step cooling, now with irreversible compression and expansion, Fig. 4.7 shows that the turbine entry temperature is reduced from Ti. to by mixing with the cooling air i/ H taken from the compressor exit, at state 2, pressure p2, temperature T2 (Fig. 4.7a). After expansion to temperature Tg, the turbine gas flow (1 + lp ) is mixed with compressor air at state 7 (mass flow i/h.) at temperature Tg. This gas is then expanded to temperature T g. [Pg.58]

The two step cooling example given above can in theory be extended to multi-step cooling of the turbine. It is more convenient to treat the turbine expansion as a modification of normal polytropic expansion the analysis is essentially an adaptation of that given in Section 4.2.1.3 for the multi-step cooled turbine cycle. [Pg.59]

Figure 110.5 Space time profiles of fractional conversion and reactor temperature in a PFR. These profiles correspond to the constant cooling eind two step cooling cases. Figure 110.5 Space time profiles of fractional conversion and reactor temperature in a PFR. These profiles correspond to the constant cooling eind two step cooling cases.
Steps. Thermal-swing cycles have at least two steps, adsorption and heating. A cooling step is also normally used after the heating step. A portion of the feed or product stream can be utilized for heating, or an independent fluid can be used. Easily condensable contaminants may be regenerated with noncondensable gases and recovered by condensation. Water-iminiscible solvents are stripped with steam, which may be condensed and separated from the solvent by decantation. Fuel and/or air may be used when the impurities are to be burned or incinerated. [Pg.279]

The Dravo hydrate addition at low temperature process involves a two-step injection of water and dry sorbent in a rectangular 19.8-m duct having a cross section of 2 m. In one step water is injected through atomization nozzles to cool the flue gas from 150°C to approximately a 15°C approach to adiabatic saturation. The other step involves the dry injection of hydrated lime, either downstream or upstream of the humidifica tion nozzles. Typical SO2 removals were 50—60% at a Ca S ratio of 2. [Pg.261]

Tanks cool, contents partially freeze, and solids drop to bottom or rise to top. This case requires a two-step calculation. The first step is handled as in case 1. The second step is calculated by assuming an isothermal system at the freezing point. It is possible, given time and a sufficiently low ambient temperature, for tank contents to freeze solid. [Pg.1049]

The nomenclature introduced by Hawthorne and Davis [4] is adopted and gas turbine cycles are referred to as follows CHT, CBT, CHTX, CBTX, where C denotes compressor H, air heater B, burner (combustion) T, turbine X, heat exchanger. R and I indicate reversible and irreversible. The subscripts U and C refer to uncooled and cooled turbines in a cycle, and subscripts 1,2, M indicate the number of cooling steps (one, two or multi-step cooling). Thus, for example, [CHT] C2 indicates an irreversible cooled simple cycle with two steps of turbine cooling. The subscript T is also used to indicate that the cooling air has been throttled from the compressor delivery pres.sure. [Pg.48]

Fig. 4.2. Temperalure-en(ropy diagram for single-step cooling—equivalent two cycles (after Ref. [5 ). Fig. 4.2. Temperalure-en(ropy diagram for single-step cooling—equivalent two cycles (after Ref. [5 ).
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]

For the a/s example quoted earlier, with this form of two stage cooling (with a = 2.79, Ah = 1.22, i//h = 0.1, i/ l = 0.05), the thermal efficiency is reduced from 0.4442 (uncooled) to 0.4257, i.e. by 0.0185, still not a significant reduction. If the second step of cooling uses compressor delivery air rather than air taken at the appropriate pressure along the compressor, then the analysis proceeds as before, except that the expansion work for the processes 7, 11 in Fig. 4.7a is replaced by that corresponding to 7, 11 in Fig. 4.7b. It may be shown [5] that the efficiency may then be written as... [Pg.58]

Further unintended variations will occur with the flow of the primary cooling medium. With two-step (on-off) control of the compressor within an air-conditioning unit, the temperature will slowly rise while the compressor is off until the compressor restarts. [Pg.300]

Preparation. On a coml scale the nitration of naphthalene is carried out in two steps using a cylindrical jacketed reactor 1.6 x lm with a conical bottom. It is fitted with a discharge pipe 8cm in diameter and a stirrer which can be rotated at 85—90rpm. The jacket can be heated with steam or cooled with cold w. The cover is provided with an opening for the addn of naphthalene and a vent for the removal of gaseous prods... [Pg.192]

Path A is an isothermal, reversible expansion. Path B has two steps. In the first step, the gas is cooled at constant volume to 1.19 atm. In the second step, the gas is heated and allowed to expand against a constant external pressure of 1.19 atm until the final volume is 7.39 L. Calculate the work for each path. [Pg.379]

The compounds were mixed in three steps The first two steps were done in an internal mixer with a mixing chamber volume of 390 mL. The mixing procedures employed in the first two steps are indicated in Table 29.2. The starting temperamre was 50°C and the cooling water was kept at a constant temperature of 50°C. The rotor speed was 100 rpm and the fill factor 66%. After every mixing step the compound was sheeted out on a 100-mL two-roll mill. The third mixing step was done on the same two-roll mill. The accelerators and sulfur were added during this step. [Pg.806]

C by external cooling. During this process a part of the reduction occurs between titanium tetrachloride and sodium vapor and this leads to the formation of titanium powder. To avoid this, the reduction is carried out in two steps. Initially, stoichiometric amounts of sodium and titanium tetrachloride are metered into the steel retort at 700 to 750 °C to produce titanium dichloride ... [Pg.420]


See other pages where Two-step cooling is mentioned: [Pg.51]    [Pg.52]    [Pg.58]    [Pg.425]    [Pg.897]    [Pg.791]    [Pg.51]    [Pg.52]    [Pg.58]    [Pg.425]    [Pg.897]    [Pg.791]    [Pg.117]    [Pg.457]    [Pg.265]    [Pg.405]    [Pg.471]    [Pg.437]    [Pg.304]    [Pg.199]    [Pg.333]    [Pg.783]    [Pg.778]    [Pg.779]    [Pg.514]    [Pg.233]    [Pg.288]    [Pg.112]    [Pg.153]    [Pg.188]    [Pg.9]    [Pg.303]    [Pg.261]    [Pg.286]   
See also in sourсe #XX -- [ Pg.51 , Pg.58 ]




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