ASHRAE FUNDAMENTALS SI CH 1-2017 Psychrometrics.pdf
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1、1.1CHAPTER 1PSYCHROMETRICSComposition of Dry and Moist Air 1.1U.S. Standard Atmosphere. 1.1Thermodynamic Properties of Moist Air . 1.2Thermodynamic Properties of Water at Saturation. 1.4Humidity Parameters. 1.8Perfect Gas Relationships for Dry and Moist Air 1.8Thermodynamic Wet-Bulb and Dew-Point Te
2、mperature. 1.9Numerical Calculation of Moist Air Properties. 1.10Psychrometric Charts. 1.10Typical Air-Conditioning Processes 1.12Transport Properties of Moist Air 1.15Symbols 1.15SYCHROMETRICS uses thermodynamic properties to ana-Plyze conditions and processes involving moist air. This chapterdiscu
3、sses perfect gas relations and their use in common heating,cooling, and humidity control problems. Formulas developed byHerrmann et al. (2009) may be used where greater precision isrequired.Herrmann et al. (2009), Hyland and Wexler (1983a, 1983b), andNelson and Sauer (2002) developed formulas for th
4、ermodynamicproperties of moist air and water modeled as real gases. However,perfect gas relations can be substituted in most air-conditioningproblems. Kuehn et al. (1998) showed that errors are less than 0.7%in calculating humidity ratio, enthalpy, and specific volume of satu-rated air at standard a
5、tmospheric pressure for a temperature range of50 to 50C. Furthermore, these errors decrease with decreasingpressure.1. COMPOSITION OF DRY AND MOIST AIRAtmospheric air contains many gaseous components as well aswater vapor and miscellaneous contaminants (e.g., smoke, pollen,and gaseous pollutants not
6、 normally present in free air far from pol-lution sources).Dry air is atmospheric air with all water vapor and contaminantsremoved. Its composition is relatively constant, but small variationsin the amounts of individual components occur with time, geo-graphic location, and altitude. Harrison (1965)
7、 lists the approximatepercentage composition of dry air by volume as: nitrogen, 78.084;oxygen, 20.9476; argon, 0.934; neon, 0.001818; helium, 0.000524;methane, 0.00015; sulfur dioxide, 0 to 0.0001; hydrogen, 0.00005;and minor components such as krypton, xenon, and ozone, 0.0002.Harrison (1965) and H
8、yland and Wexler (1983a) used a value 0.0314(circa 1955) for carbon dioxide. Carbon dioxide reached 0.0379 in2005, is currently increasing by 0.00019 percent per year and is pro-jected to reach 0.0438 in 2036 (Gatley et al. 2008; Keeling andWhorf 2005a, 2005b). Increases in carbon dioxide are offset
9、 bydecreases in oxygen; consequently, the oxygen percentage in 2036 isprojected to be 20.9352. Using the projected changes, the relativemolecular mass for dry air for at least the first half of the 21st centuryis 28.966, based on the carbon-12 scale. The gas constant for dry airusing the current Moh
10、r and Taylor (2005) value for the universal gasconstant isRda= 8314.472/28.966 = 287.042 J/(kgdaK) (1)Moist air is a binary (two-component) mixture of dry air andwater vapor. The amount of water vapor varies from zero (dry air) toa maximum that depends on temperature and pressure. Saturation isa sta
11、te of neutral equilibrium between moist air and the condensedwater phase (liquid or solid); unless otherwise stated, it assumes aflat interface surface between moist air and the condensed phase.Saturation conditions change when the interface radius is very small(e.g., with ultrafine water droplets).
12、 The relative molecular mass ofwater is 18.015 268 on the carbon-12 scale. The gas constant forwater vapor isRw= 8314.472/18.015 268 = 461.524 J/(kgwK) (2)2. U.S. STANDARD ATMOSPHEREThe temperature and barometric pressure of atmospheric air varyconsiderably with altitude as well as with local geogra
13、phic andweather conditions. The standard atmosphere gives a standard of ref-erence for estimating properties at various altitudes. At sea level,standard temperature is 15C; standard barometric pressure is101.325 kPa. Temperature is assumed to decrease linearly with in-creasing altitude throughout th
14、e troposphere (lower atmosphere), andto be constant in the lower reaches of the stratosphere. The lower at-mosphere is assumed to consist of dry air that behaves as a perfect gas.Gravity is also assumed constant at the standard value, 9.806 65 m/s2.Table 1 summarizes property data for altitudes to 1
15、0 000 m.Pressure values in Table 1 may be calculated fromp = 101.325(1 2.25577 105Z)5.2559(3)The equation for temperature as a function of altitude ist =15 0.0065Z (4)whereZ = altitude, mp = barometric pressure, kPat =temperature, CThe preparation of this chapter is assigned to TC 1.1, Thermodynamic
16、s andPsychrometrics.Table 1 Standard Atmospheric Data for Altitudes to 10 000 mAltitude, m Temperature, C Pressure, kPa500 18.2 107.4780 15.0 101.325500 11.8 95.4611000 8.5 89.8751500 5.2 84.5562000 2.0 79.4952500 1.2 74.6823000 4.5 70.1084000 11.0 61.6405000 17.5 54.0206000 24.0 47.1817000 30.5 41.
17、0618000 37.0 35.6009000 43.5 30.74210 000 50 26.436Source: Adapted from NASA (1976).1.2 2017 ASHRAE HandbookFundamentals (SI)Equations (3) and (4) are accurate from 5000 m to 11 000 m.For higher altitudes, comprehensive tables of barometric pressureand other physical properties of the standard atmos
18、phere, in both SIand I-P units, can be found in NASA (1976).3. THERMODYNAMIC PROPERTIES OF MOIST AIRTable 2, developed from formulas by Herrmann et al. (2009),shows values of thermodynamic properties of moist air based on theInternational Temperature Scale of 1990 (ITS-90). This ideal scalediffers s
19、lightly from practical temperature scales used for physicalmeasurements. For example, the standard boiling point for water (at101.325 kPa) occurs at 99.97C on this scale rather than at the tra-ditional 100C. Most measurements are currently based on ITS-90(Preston-Thomas 1990).The following propertie
20、s are shown in Table 2:t = Celsius temperature, based on the ITS-90 and expressed relativeto absolute temperature T in kelvins (K) by the followingrelation:T = t + 273.15Ws= humidity ratio at saturation; gaseous phase (moist air) exists inequilibrium with condensed phase (liquid or solid) at givente
21、mperature and pressure (standard atmospheric pressure). Atgiven values of temperature and pressure, humidity ratio W canhave any value from zero to Ws.vda= specific volume of dry air, m3/kgda.vas= vs vda, difference between specific volume of moist air at saturation and that of dry air, m3/kgda, at
22、same pressure and temperature.vs= specific volume of moist air at saturation, m3/kgda.hda= specific enthalpy of dry air, kJ/kgda. In Table 2, hdais assigned avalue of 0 at 0C and standard atmospheric pressure.has= hs hda, difference between specific enthalpy of moist air atsaturation and that of dry
23、 air, kJ/kgda, at same pressure andtemperature.hs= specific enthalpy of moist air at saturation, kJ/kgda.sda= specific entropy of dry air, kJ/(kgdaK). In Table 2, sdaisassigned a value of 0 at 0C and standard atmospheric pressure.ss= specific entropy of moist air at saturation kJ/(kgdaK).Table 2 The
24、rmodynamic Properties of Moist Air at Standard Atmospheric Pressure, 101.325 kPaTemp., CtHumidity RatioWs, kgw/kgdaSpecific Volume, m3/kgdaSpecific Enthalpy, kJ/kgdaSpecific Entropy, kJ/(kgdaK)Temp., Ctvdavasvshdahashssdass60 0.0000067 0.6027 0.0000 0.6027 60.341 0.016 60.325 0.2494 0.2494 6059 0.00
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