Adiabatic Saturation Process on Psychrometric Chart
If an adiabatic saturator (an idealization of an evaporative cooler) operates at 1 atm with an inlet dry-bulb temperature of 82°F (28°C) and an exit dry-bulb temperature of 65°F (18.5°C), what are the entering humidity ratio and RH?
Given: T_{db1} and T_{db2}.
Figure: See Figures 13.2 and 13.12 (process 1–2).
Assumptions: Thermodynamic equilibrium exists.
The local atmospheric pressure is 1 atm, or 14.696 psia.
Find: W_{1} and \phi_{1}.
Lookup values: At 65°F, the saturation pressure is 0.306 psia from Table A3.
TABLE A.3 (IP Units) Properties of Saturated Steam | ||||||||||||
Pressure (psia) | Saturation Temp. (°F) | Specific Volume (ft³/lb_{m}) |
Internal Energy (Btu/lb_{m}) | Enthalpy (Btu/lb_{m}) | Entropy (Btu/(lb_{m} · °R)) | |||||||
Sat. Liquid | Sat. Vapor | Sat. Liquid | Evap. | Sat. Vapor | Sat. Liquid | Evap. | Sat. Vapor | Sat. Liquid | Evap. | Sat. Vapor | ||
p | Tsat | vf | vg | uf | ufg | ug | hf | hfg | hg | sf | sfg | sg |
0.08866 | 32.02 | 0.016022 | 3302 | 0.00 | 1021.2 | 1021.2 | 0.01 | 1075.4 | 1075.4 | 0.00000 | 2.1869 | 2.1869 |
0.09992 | 35.00 | 0.016021 | 2948 | 2.99 | 1019.2 | 1022.2 | 3.00 | 1073.7 | 1076.7 | 0.00607 | 2.1704 | 2.1764 |
0.12166 | 40.00 | 0.016020 | 2445 | 8.02 | 1015.8 | 1023.9 | 8.02 | 1070.9 | 1078.9 | 0.01617 | 2.1430 | 2.1592 |
0.14748 | 45.00 | 0.016021 | 2037 | 13.04 | 1012.5 | 1025.5 | 13.04 | 1068.1 | 1081.1 | 0.02618 | 2.1162 | 2.1423 |
0.17803 | 50.00 | 0.016024 | 1704.2 | 18.06 | 1009.1 | 1027.2 | 18.06 | 1065.2 | 1083.3 | 0.03607 | 2.0899 | 2.1259 |
0.2563 | 60.00 | 0.016035 | 1206.9 | 28.08 | 1002.4 | 1030.4 | 28.08 | 1059.6 | 1087.7 | 0.05555 | 2.0388 | 2.0943 |
0.3632 | 70.00 | 0.016051 | 867.7 | 38.09 | 995.6 | 1033.7 | 38.09 | 1054.0 | 1092.0 | 0.07463 | 1.9896 | 2.0642 |
0.5073 | 80.00 | 0.016073 | 632.8 | 48.08 | 988.9 | 1037.0 | 48.09 | 1048.3 | 1096.4 | 0.09332 | 1.9423 | 2.0356 |
0.6988 | 90.00 | 0.016099 | 467.7 | 58.07 | 982.2 | 1040.2 | 58.07 | 1042.7 | 1100.7 | 0.11165 | 1.8966 | 2.0083 |
0.9503 | 100.00 | 0.016130 | 350.0 | 68.04 | 975.4 | 1043.5 | 68.05 | 1037.0 | 1105.0 | 0.12963 | 1.8526 | 1.9822 |
1 | 101.70 | 0.016136 | 333.6 | 69.74 | 974.3 | 1044.0 | 69.74 | 1036.0 | 1105.8 | 0.13266 | 1.8453 | 1.9779 |
2 | 126.04 | 0.016230 | 173.75 | 94.02 | 957.8 | 1051.8 | 94.02 | 1022.1 | 1116.1 | 0.17499 | 1.7448 | 1.9198 |
3 | 141.43 | 0.016300 | 118.72 | 109.38 | 947.2 | 1056.6 | 109.39 | 1013.1 | 1122.5 | 0.20089 | 1.6852 | 1.8861 |
4 | 152.93 | 0.016358 | 90.64 | 120.88 | 939.3 | 1060.2 | 120.89 | 1006.4 | 1127.3 | 0.21983 | 1.6426 | 1.8624 |
5 | 162.21 | 0.016407 | 73.53 | 130.15 | 932.9 | 1063.0 | 130.17 | 1000.9 | 1131.0 | 0.23486 | 1.6093 | 1.8441 |
6 | 170.03 | 0.016451 | 61.98 | 137.98 | 927.4 | 1065.4 | 138.00 | 996.2 | 1134.2 | 0.24736 | 1.5819 | 1.8292 |
8 | 192.84 | 0.016526 | 47.35 | 150.81 | 918.4 | 1069.2 | 150.84 | 988.4 | 1139.3 | 0.26754 | 1.5383 | 1.8058 |
10 | 193.19 | 0.016590 | 38.42 | 161.20 | 911.0 | 1072.2 | 161.23 | 982.1 | 1143.3 | 0.28358 | 1.5041 | 1.7877 |
14.696 | 211.99 | 0.016715 | 26.80 | 180.10 | 897.5 | 1077.6 | 180.15 | 970.4 | 1150.5 | 0.31212 | 1.4446 | 1.7567 |
15 | 213.03 | 0.016723 | 26.29 | 181.14 | 896.8 | 1077.9 | 181.19 | 969.7 | 1150.9 | 0.31367 | 1.4414 | 1.7551 |
20 | 227.96 | 0.016830 | 20.09 | 196.19 | 885.8 | 1082.0 | 196.26 | 960.1 | 1156.4 | 0.33580 | 1.3962 | 1.7320 |
25 | 240.08 | 0.016922 | 16.306 | 208.44 | 876.9 | 1085.3 | 208.52 | 952.2 | 1160.7 | 0.35345 | 1.3607 | 1.7142 |
30 | 250.34 | 0.017004 | 13.748 | 218.84 | 869.2 | 1088.0 | 218.93 | 945.4 | 1164.3 | 0.36821 | 1.3314 | 1.6996 |
35 | 259.30 | 0.017073 | 11.900 | 227.93 | 862.4 | 1090.3 | 228.04 | 939.3 | 1167.4 | 0.38093 | 1.3064 | 1.6873 |
40 | 267.26 | 0.017146 | 10.501 | 236.03 | 856.2 | 1092.3 | 236.16 | 933.8 | 1170.0 | 0.39214 | 1.2845 | 1.6767 |
45 | 274.46 | 0.017209 | 9.403 | 243.37 | 850.7 | 1094.0 | 243.51 | 928.8 | 1172.3 | 0.40218 | 1.2651 | 1.6673 |
50 | 281.03 | 0.017269 | 8.518 | 250.08 | 845.5 | 1095.6 | 250.24 | 924.2 | 1174.4 | 0.41129 | 1.2476 | 1.6589 |
55 | 287.10 | 0.017325 | 7.789 | 256.28 | 840.8 | 1097.0 | 256.46 | 919.9 | 1176.3 | 0.41963 | 1.2317 | 1.6513 |
60 | 292.73 | 0.017378 | 7.177 | 262.06 | 836.3 | 1098.3 | 262.25 | 915.8 | 1178.0 | 0.42733 | 1.2170 | 1.6444 |
65 | 298.00 | 0.017429 | 6.657 | 267.46 | 832.1 | 1099.5 | 267.67 | 911.9 | 1179.6 | 0.43450 | 1.2035 | 1.6380 |
70 | 302.96 | 0.017478 | 6.209 | 272.56 | 828.1 | 1100.6 | 272.79 | 908.3 | 1181.0 | 0.44120 | 1.1909 | 1.6321 |
75 | 307.63 | 0.017524 | 5.818 | 277.37 | 824.3 | 1101.6 | 277.61 | 904.8 | 1182.4 | 0.44749 | 1.1790 | 1.6265 |
80 | 312.07 | 0.017570 | 5.474 | 281.95 | 820.6 | 1102.6 | 282.21 | 901.4 | 1183.6 | 0.45344 | 1.1679 | 1.6214 |
85 | 316.29 | 0.017613 | 5.17 | 286.3 | 817.1 | 1103.5 | 286.58 | 898.2 | 1184.8 | 0.45907 | 1.1574 | 1.6165 |
90 | 320.31 | 0.017655 | 4.898 | 290.46 | 813.8 | 1104.3 | 290.76 | 895.1 | 1185.9 | 0.46442 | 1.1475 | 1.6119 |
95 | 324.16 | 0.017696 | 4.654 | 294.45 | 810.6 | 1105.0 | 294.76 | 892.1 | 1186.9 | 0.46952 | 1.1380 | 1.6076 |
100 | 327.86 | 0.017736 | 4.434 | 298.28 | 807.5 | 1105.8 | 298.61 | 889.2 | 1187.8 | 0.47439 | 1.1290 | 1.6034 |
110 | 334.82 | 0.017813 | 4.051 | 305.52 | 801.6 | 1107.1 | 305.88 | 883.7 | 1189.6 | 0.48355 | 1.1122 | 1.5957 |
120 | 341.30 | 0.017886 | 3.73 | 312.27 | 796 | 1108.3 | 312.67 | 878.5 | 1191.1 | 0.49201 | 1.0966 | 1.5886 |
130 | 347.37 | 0.017957 | 3.457 | 318.61 | 790.7 | 1109.4 | 319.04 | 873.5 | 1192.5 | 0.49989 | 1.0822 | 1.5821 |
140 | 353.08 | 0.018024 | 3.221 | 324.58 | 785.7 | 1110.3 | 325.05 | 868.7 | 1193.8 | 0.50727 | 1.0688 | 1.5761 |
150 | 358.48 | 0.018089 | 3.016 | 330.24 | 781 | 1111.2 | 330.75 | 864.2 | 1194.9 | 0.51422 | 1.0562 | 1.5704 |
0.6113 | 0.01 | 0.001 | 206.14 | 0 | 2375.3 | 2375.3 | 0.01 | 2501.3 | 2501.4 | 0 | 9.1562 | 9.1562 |
1.0 | 6.98 | 0.001 | 129.21 | 29.30 | 2355.7 | 2385.0 | 29.30 | 2484.9 | 2514.2 | 0.1059 | 8.8697 | 8.9756 |
1.5 | 13.03 | 0.001001 | 87.98 | 54.71 | 2338.6 | 2393.3 | 54.71 | 2470.6 | 2525.3 | 0.1957 | 8.6322 | 8.8279 |
2.0 | 17.50 | 0.001001 | 67.00 | 73.48 | 2326.0 | 2399.5 | 73.48 | 2460.0 | 2533.5 | 0.2607 | 8.4629 | 8.7237 |
2.5 | 21.08 | 0.001002 | 54.25 | 88.48 | 2315.9 | 2404.4 | 88.49 | 2451.6 | 2540.4 | 0.3120 | 8.3311 | 8.6432 |
3.0 | 24.08 | 0.001003 | 45.67 | 101.04 | 2307.5 | 2408.5 | 101.05 | 2444.5 | 2545.5 | 0.3545 | 8.2231 | 8.5776 |
4.0 | 28.96 | 0.001004 | 34.80 | 121.45 | 2293.7 | 2415.2 | 121.46 | 2432.9 | 2554.4 | 0.4226 | 8.0520 | 8.4746 |
5.0 | 32.88 | 0.001005 | 28.19 | 137.81 | 2282.7 | 2420.5 | 137.82 | 2423.7 | 2561.5 | 0.4764 | 7.9187 | 8.3951 |
7.5 | 40.29 | 0.001008 | 19.24 | 168.78 | 2261.7 | 2430.5 | 168.79 | 2406.0 | 2574.8 | 0.5764 | 7.6750 | 8.2515 |
10 | 45.81 | 0.001010 | 14.67 | 191.82 | 2246.1 | 2437.9 | 191.83 | 2392.8 | 2584.7 | 0.6493 | 7.5009 | 8.1502 |
15 | 53.97 | 0.001014 | 10.02 | 225.92 | 2222.8 | 2448.7 | 225.94 | 2373.1 | 2599.1 | 0.7549 | 7.2536 | 8.0085 |
20 | 60.06 | 0.001017 | 7.649 | 251.38 | 2205.4 | 2456.7 | 251.40 | 2358.3 | 2609.7 | 0.8320 | 7.0766 | 7.9085 |
25 | 64.97 | 0.001020 | 6.204 | 271.90 | 2191.2 | 2463.1 | 271.93 | 2346.3 | 2618.2 | 0.8931 | 6.9383 | 7.8314 |
30 | 69.10 | 0.001022 | 5.229 | 289.20 | 2179.2 | 2468.4 | 289.23 | 2336.1 | 2625.3 | 0.9439 | 6.8247 | 7.7686 |
40 | 75.87 | 0.001027 | 3.993 | 317.53 | 2159.5 | 2477.0 | 317.58 | 2319.2 | 2636.8 | 1.0259 | 6.6441 | 7.6700 |
50 | 81.33 | 0.001030 | 3.240 | 340.44 | 2143.4 | 2483.9 | 340.49 | 2305.4 | 2645.9 | 1.0910 | 6.5029 | 7.5939 |
75 | 91.78 | 0.001037 | 2.217 | 384.31 | 2112.4 | 2496.7 | 384.39 | 2278.6 | 2663.0 | 1.2130 | 6.2434 | 7.4564 |
100 | 99.63 | 0.001043 | 1.6940 | 417.36 | 2088.7 | 2506.1 | 417.46 | 2258.0 | 2675.5 | 1.3026 | 6.0568 | 7.3594 |
125 | 105.99 | 0.001048 | 1.3749 | 444.19 | 2069.3 | 2513.5 | 444.32 | 2241.0 | 2685.4 | 1.3740 | 5.9104 | 7.2844 |
150 | 111.37 | 0.001053 | 1.1593 | 466.94 | 2052.7 | 2519.7 | 467.11 | 2226.5 | 2693.6 | 1.4336 | 5.7897 | 7.2233 |
175 | 116.06 | 0.001057 | 1.0036 | 486.8 | 2038.1 | 2524.9 | 486.99 | 2213.6 | 2700.6 | 1.4849 | 5.6868 | 7.1717 |
200 | 120.23 | 0.001061 | 0.8857 | 504.49 | 2025.0 | 2529.5 | 504.70 | 2201.9 | 2706.7 | 1.5301 | 5.5970 | 7.1271 |
225 | 124 | 0.001064 | 0.7933 | 520.47 | 2013.1 | 2533.6 | 520.72 | 2191.3 | 2712.1 | 1.5706 | 5.5173 | 7.0878 |
250 | 127.44 | 0.001067 | 0.7187 | 535.10 | 2002.1 | 2537.2 | 535.37 | 2181.5 | 2716.9 | 1.6072 | 5.4455 | 7.0527 |
275 | 130.6 | 0.001070 | 0.6573 | 548.59 | 1991.9 | 2540.5 | 548.89 | 2172.4 | 2721.3 | 1.6408 | 5.3801 | 7.0209 |
300 | 133.55 | 0.001073 | 0.6058 | 561.15 | 1982.4 | 2543.6 | 561.47 | 2163.8 | 2725.3 | 1.6718 | 5.3201 | 6.9919 |
325 | 136.3 | 0.001076 | 0.5620 | 572.90 | 1973.5 | 2546.4 | 573.25 | 2155.8 | 2729.0 | 1.7006 | 5.2646 | 6.9652 |
350 | 138.88 | 0.001079 | 0.5243 | 583.95 | 1965.0 | 2548.9 | 584.33 | 2148.1 | 2732.4 | 1.7275 | 5.2130 | 6.9405 |
375 | 141.32 | 0.001081 | 0.4914 | 594.40 | 1956.9 | 2551.3 | 594.81 | 2140.8 | 2735.6 | 1.7528 | 5.1647 | 6.9175 |
400 | 143.63 | 0.001084 | 0.4625 | 604.31 | 1949.3 | 2553.6 | 604.74 | 2133.8 | 2738.6 | 1.7766 | 5.1193 | 6.8959 |
450 | 147.93 | 0.001088 | 0.4140 | 622.77 | 1934.9 | 2557.6 | 623.25 | 2120.7 | 2743.9 | 1.8207 | 5.0359 | 6.8565 |
500 | 151.86 | 0.001093 | 0.3749 | 639.68 | 1921.6 | 2561.2 | 640.23 | 2108.5 | 2748.7 | 1.8607 | 4.9606 | 6.8213 |
550 | 155.48 | 0.001097 | 0.3427 | 655.32 | 1909.2 | 2564.5 | 655.93 | 2097.0 | 2753.0 | 1.8973 | 4.8920 | 6.7893 |
600 | 158.85 | 0.001101 | 0.3157 | 669.90 | 1897.5 | 2567.4 | 670.56 | 2086.3 | 2756.8 | 1.9312 | 4.8288 | 6.7600 |
650 | 162.01 | 0.001104 | 0.2927 | 683.56 | 1886.5 | 2570.1 | 684.28 | 2076.0 | 2760.3 | 1.9627 | 4.7703 | 6.7331 |
700 | 164.97 | 0.001108 | 0.2729 | 696.44 | 1876.1 | 2572.5 | 697.22 | 2066.3 | 2763.5 | 1.9922 | 4.7158 | 6.7080 |
750 | 167.78 | 0.001112 | 0.2556 | 708.64 | 1866.1 | 2574.7 | 709.47 | 2057.0 | 2766.4 | 2.0200 | 4.6647 | 6.6847 |
800 | 170.43 | 0.001115 | 0.2404 | 720.22 | 1856.6 | 2576.8 | 721.11 | 2048.0 | 2769.1 | 2.0462 | 4.6166 | 6.6628 |
850 | 172.96 | 0.001118 | 0.2270 | 731.27 | 1847.4 | 2578.7 | 732.22 | 2039.4 | 2771.6 | 2.0710 | 4.5711 | 6.6421 |
900 | 175.38 | 0.001121 | 0.2150 | 741.83 | 1838.6 | 2580.5 | 742.83 | 2031.1 | 2773.9 | 2.0946 | 4.5280 | 6.6226 |
950 | 177.69 | 0.001124 | 0.2042 | 751.95 | 1830.2 | 2582.1 | 753.02 | 2023.1 | 2776.1 | 2.1172 | 4.4869 | 6.6041 |
1000 | 179.91 | 0.001127 | 0.19444 | 761.68 | 1822.0 | 2583.6 | 762.81 | 2015.3 | 2778.1 | 2.1387 | 4.4478 | 6.5865 |
1100 | 184.09 | 0.001133 | 0.17753 | 780.09 | 1806.3 | 2586.4 | 781.34 | 2000.4 | 2781.7 | 2.1792 | 4.3744 | 6.5536 |
1200 | 187.99 | 0.001139 | 0.16333 | 797.29 | 1791.5 | 2588.8 | 798.65 | 1986.2 | 2784.8 | 2.2166 | 4.3067 | 6.5233 |
1300 | 191.64 | 0.001144 | 0.15125 | 813.44 | 1777.5 | 2591.0 | 814.93 | 1972.7 | 2787.6 | 2.2515 | 4.2438 | 6.4953 |
Source: Courtesy of ASHRAE, Handbook of Fundamentals, American Society of Heating, Refrigerating and Air-Conditioning Engineers, Atlanta, GA, 1997. With permission. |
As indicated in Figure 13.12, this process is a constant wet-bulb temperature process, not a constant-enthalpy process because water supplied to maintain the sump water level carries enthalpy with it. From Equation 13.14, the humidity ratio at the exit can be found to be
W = 0.622 \times \left\lgroup \frac{p_{vap}}{p_{tot} – p_{vap}} \right\rgroup (13.14)
W_{2} = 0.622 \times \left\lgroup \frac{0.306}{14.696 – 0.306} \right\rgroup = 0.0132 lb_{w}/lb_{a}Equation 13.40, IP can now be used to find the inlet humidity ratio:
W_{1} = \frac{(1093 – 0.556 T_{wb2}) W_{2} – 0.240 \times (T_{db1} – T_{wb2})}{1093 + 0.444 T_{db1} – T_{wb2}} (13.40)
W_{1} = \frac{(1093 – 0.556 \times 65) \times 0.0132 – 0.240 \times (82 – 65)}{1093 + 0.444 \times 82 – 65}= 0.00927 lb_{w}/lb_{a}
To find the inlet RH, Equation 13.14 can be solved for the water vapor pressure:
W_{1} = 0.00927 = 0.622 \left\lgroup \frac{p_{vap,1}}{14.696 – p_{vap,1}} \right\rgroupfrom which p_{vap,1} = 0.216 psia
from which p_{vap,1} = 0.216 psia.
At 82°F, the saturation pressure is 0.542 psia from Table A3. Finally, from the definition of RH, we have
Comments
It is a common human experience to have an evaporating liquid cool one’s skin. Adiabatic saturation is the basic process involved in evaporative cooling of airstreams. It provides an economical method for reducing the dry-bulb temperature of air in climates with low ambient air humidity. Evaporative cooling is essentially an incomplete adiabatic saturation process. In actual practice, the exit airstream is often not entirely saturated or at the thermodynamic wet-bulb temperature.
This same phenomenon is used in mechanical equipment for buildings in several ways, for example, space cooling can be achieved in dry climates by passing air over or through a wet medium or spray. Sensible heat is removed from the airstream by evaporating some of the liquid.
Evaporative cooling equipment is discussed in Section 20.8. Cooling towers (discussed in Section 17.7) are used to reject heat from chillers using the same principle.