ASHRAE REFRIGERATION SI CH 48-2010 ULTRALOW-TEMPERATURE REFRIGERATION《超低温制冷》.pdf
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1、48.1CHAPTER 48ULTRALOW-TEMPERATURE REFRIGERATIONAutocascade Systems . 48.1Custom-Designed and Field-Erected Systems . 48.2Single-Refrigerant Systems 48.2Cascade Systems 48.3Low-Temperature Materials. 48.6Insulation . 48.9Heat Transfer . 48.9Secondary Coolants . 48.10LTRALOW-TEMPERATURE refrigeration
2、 is defined hereUas refrigeration in the temperature range of 50 to 100C.What is considered low temperature for an application depends on thetemperature range for that specific application. Low temperaturesfor air conditioning are around 0C; for industrial refrigeration,35 to 50C; and for cryogenics
3、, approaching 0 K. Applicationssuch as freeze-drying, as well as the pharmaceutical, chemical, andpetroleum industries, use refrigeration in the low temperature rangeas designated in this chapter.The 50 to 100C temperature range is treated separatelybecause design and construction considerations for
4、 systems thatoperate in this range differ from those encountered in industrialrefrigeration and cryogenics, which bracket it. Designers and build-ers of cryogenic facilities are rarely active in the low-temperaturerefrigeration field. One major type of low-temperature system is thepackaged type, whi
5、ch often serves applications such as environ-ment chambers. The other major category is custom-designed andfield-erected systems. Industrial refrigeration practitioners are thegroup most likely to be responsible for these systems, but they maydeal with low-temperature systems only occasionally; the
6、experienceof a single organization does not accumulate rapidly. The objectiveof this chapter is to bring together available experience for thosewhose work does not require daily contact with low-temperature sys-tems.The refrigeration cycles presented in this chapter may be usedin both standard packa
7、ged and custom-designed systems. Cascadesystems are emphasized, both autocascade (typical of packagedunits) and two-refrigerant cascade (found in custom-engineeredlow-temperature systems).AUTOCASCADE SYSTEMSAn autocascade refrigeration system is a complete, self-containedrefrigeration system in whic
8、h multiple stages of cascade cooling ef-fect occur simultaneously by means of vapor/liquid separation andadiabatic expansion of various refrigerants. Physical and thermody-namic features, along with a series of counterflow heat exchangersand an appropriate mixture of refrigerants, allow the system t
9、o reachlow temperature.Autocascade refrigeration systems offer many benefits, such as alow compression ratio and relatively high volumetric efficiency.However, system chemistry and heat exchangers are complex, re-frigerant compositions are sensitive, and compressor displacementis large.Operational C
10、haracteristicsComponents of an autocascade refrigeration system typicallyinclude a vapor compressor, an external air- or water-cooled con-denser, a mixture of refrigerants with descending boiling points, anda series of insulated heat exchangers. Figure 1 is a schematic of asimple system illustrating
11、 a single stage of autocascade.In this system, two refrigerants with significantly different boilingpoints are compressed and circulated by one vapor compressor. As-sume that one refrigerant is R-23 (normal boiling point, 82C) andthe second refrigerant is R-404a (normal boiling point, 46.7C).Assume
12、that ambient temperature is 25C and that the condenser is100% efficient.With properly sized components, this system should be able toachieve 60C in the absorber while the compression ratio is main-tained at 5.1 to 1. As the refrigerant mixture is pumped through themain condenser and cooled to 25C at
13、 the exit, compressor dis-charge pressure is maintained at 1524 kPa (gage). At this condition,virtually all R-404a is condensed at 35C and then further chilled tosubcooled liquid. Although R-23 molecules are present in both liq-uid and vapor phases, the R-23 is primarily vapor because of thelarge di
14、fference in the boiling points of the two refrigerants. A phaseseparator at the outlet of the condenser collects the liquid by gravi-tational effect, and the R-23-rich vapor is removed from the outlet ofthe phase separator to the heat exchanger.At the bottom of the phase separator, an expansion devi
15、ce adia-batically expands the collected R-404a-rich liquid such that the out-let of the device produces a low temperature of 19C at 220 kPa(gage) (Weng 1995). This cold stream is immediately sent back tothe heat exchanger in a counterflow pattern to condense the R-23-rich vapor to liquid at 18.5C an
16、d 1524 kPa (gage). The R-23-richliquid is then adiabatically expanded by a second expansion deviceto 60C. As it absorbs an appropriate amount of heat in the ab-sorber, the R-23 mixes with the expanded R-404a and evaporates inthe heat exchanger, providing a cold source for condensing R-23 onthe high-
17、pressure side of the heat exchanger. Leaving the heat ex-changer at superheated conditions, the vapor mixture then returns tothe suction of the compressor for the next cycle.The preparation of this chapter is assigned to TC 10.4, Ultralow-TemperatureSystems and Cryogenics.Fig. 1 Simple Autocascade R
18、efrigeration SystemFig. 1 Simple Autocascade Refrigeration System48.2 2010 ASHRAE HandbookRefrigeration (SI)As can be seen from this simple example, the autocascade effectderives from a short cycle of the refrigerant circuit within the sys-tem that performs only internal work to condense the lower b
19、oilingpoint refrigerant.The concept of the single-stage cycle can be extended to multiplestages. Figure 2 shows the flow diagram of a four-stage system. Thecondensation and subsequent expansion of one refrigerant providesthe cooling necessary to condense the next refrigerant in the heatexchanger dow
20、nstream. This process continues until the last refrig-erant with the lowest boiling point is expanded to achieve extremelylow temperature.Design ConsiderationsCompressor Capacity. As can be seen from Figures 1 and 2, asignificant amount of compressor work is used for internal evapo-rating and conden
21、sing of refrigerants. The final gain of the system istherefore relatively small. Compressor capacity must be enough toproduce an appropriate amount of final refrigerating effect.Heat Exchanger Sizing. Because there is a significant amountof refrigerant vapor in each stage of the heat exchanger, the
22、overallheat transfer coefficients on both the evaporating and condensingsides are rather small compared to those of pure components atphase-changing conditions. Therefore, generous heat-transfer areashould be provided for energy exchange between refrigerants on thehigh- and low-pressure sides.Expans
23、ion Devices. Each expansion device is sized to providesufficient refrigerating effect for the adjacent downstream heatexchanger.Compressor Lubrication. General guidelines for lubrication ofrefrigeration systems should be adopted.CUSTOM-DESIGNED AND FIELD-ERECTED SYSTEMSIf refrigeration is to maintai
24、n a space at a low temperature to storea modest quantity of product in a chest or cabinet, the packaged low-temperature system is probably the best choice. Prefabricated walk-in environmental chambers are also practical solutions when theycan accommodate space needs. When the required refrigerationc
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