W. Knoche: lieber die räumliche und zeitliche Verteilung des Wärmegehalts der unteren Luftschicht. 
31 
IXechrrungsta’belleiT und Anlagen. 
Tabelle I. 
Logarithmen des Wasserdampfgelialtes der Luft (in gr pro kbm), 
welcher den einzelnen Wasserdampfdrucken (in mm Hg) entspricht. 
e 
in mm 
log f 
e 
in mm 
log f 
e 
in mm 
log f 
e 
in mm 
log J 
e 
in mm 
log f 
0.4 
0.6749-1 
4.7 
0.6963 
9.0 
0.9635 
13.3 
1.1239 
17.6 
1.2391 
0.5 
0.7694-1 
8 
0.7051 
1 
0.9680 
4 
1.1271 
7 
1.2413 
0.6 
0.8414-1 
9 
0.7132 
2 
0.9726 
13.5 
1.1300 
8 
1.2438 
0.7 
0.9090-1 
5.0 
0.7214 
o 
O 
0.9771 
6 
1.1332 
9 
1.2458 
0.8 
0.9643-1 
1 
0.7297 
4 
0.9812 
7 
1.1364 
18.0 
1.2482 
0.9 
0.0112 
2 
0.7382 
9.5 
0.9858 
8 
1.1393 
1 
1.2504 
1.0 
0.0577 
3 
0.7455 
6 
0.9899 
9 
1.1421 
2 
1.2529 
l 
0.0966 
4 
0.7531 
7 
0.9944 
14.0 
1.1449 
3 
1.2550 
2 
0.1316 
5.5 
0.7609 
8 
0.9985 
1 
1.1480 
4 
1.2572 
3 
0.1661 
e 
0.7682 
9 
1.0026 
2 
1.1511 
18.5 
1.2594 
4 
0.1970 
7 
0.7754 
10.0 
1.0069 
3 
1.1538 
6 
1.2617 
1.5 
0.2243 
8 
0.7812 
1 
1.0107 
4 
1.1569 
7 
1.2639 
6 
0.2512 
9 
0.7899 
2 
1.0149 
14.5 
1.1593 
8 
1.2660 
7 
0.2746 
6.0 
0.7963 
3 
1.0187 
6 
1.1623 
9 
1.2683 
8 
0.2980 
1 
0.8036 
4 
1.0233 
7 
1.1650 
19.0 
1.2705 
9 
0.3212 
2 
0.8100 
10.5 
1.0269 
8 
1.1679 
1 
1.2725 
2.0 
0.3442 
3 
0.8164 
6 
1.0306 
9 
1.1706 
2 
1.2746 
1 
0.3638 
4 
0.8232 
7 
1.034« 
15.0 
1.1735 
3 
1.2767 
2 
0.3833 
6.5 
0.8294 
8 
1.0382 
1 
1.1761 
4 
1.2790 
3 
0.3995 
6 
0.8358 
9 
1.0422 
2 . 
1.1790 
19.5 
1.2813 
4 
0.4188 
7 
0.8420 
11.0 
1.0461 
Ö 
1.1816 
6 
1.2831 
2.5 
0.4347 
8 
0.8483 
1 
1.0496 
4 
1.1841 
7 
1.2851 
6 
0.4523 
9 
0.8542 
2 
1.0535 
15.5 
1.1870 
8 
1.2874 
7 
0.4676 
7.0 
0.8602 
3 
1.0573 
6 
1.1895 
9 
1.2894 
8 
0.4823 
1 
0.8658 
4 
1.0607 
7 
1.19 20 
20.0 
1.2914 
9 
0.4964 
2 
0.8715 
11.5 
1.0641 
8 
1.1948 
1 
1.2934 
3.0 
0.5106 
3 
0.8775 
6 
1.0678 
9 
1.1973 
2 
1.2954 
1 
0.5245 
4 
0.8828 
7 
1.0715 
16.0 
1.1998 
3 
1.2973 
2 
0.5376 
7.5 
0.8884 
8 
1.0748 
1 
1.2022 
4 
1.2995 
•3 
0.5500 
e 
0.8939 
9 
1.0785 
2 
1.2049 
20.5 
1.3017 
4 
0.5623 
7 
0.8992 
12.0 
1.0817 
3 
1.2074 
6 
1.3036 
3.5 
0.5745 
8 
0.9046 
1 
1.0849 
4 
1.2100 
7 
1.3056 
6 
0.5858 
9 
0.9099 
2 
1.0888 
16.5 
1.2125 
8 
1.3075 
7 
0.5970 
8.0 
0.9151 
3 
1.0920 
6 
1.2148 
9 
1.3094 
8 
0.6082 
1 
0.9202 
4 
1.0952 
7 
1.2175 
21.0 
1.3115 
9 
0.6193 
2 
0.9252 
12.5 
1.0986 
8 
1.2199 
1 
1.3135 
4.0 
0.6304 
3 
0.9301 
6 
1.1021 
9 
1.2222 
2 
1.3151 
1 
0.6394 
4 
0.9352 
7 
1.1052 
17.0 
1.2248 
3 
1.3172 
2 
0.6494 
8.5 
0.9400 
8 
1.1082 
1 
1.2271 
4 
1.3191 
3 
0.6594 
6 
0.9451 
9 
1.1123 
2 
1.2297 
21.5 
1.3212 
4 
0.6688 
7 
0.9497 
13.0 
1.1146 
3 
1.2320 
6 
1.3228 
4.5 
0.6784 
8 
0.9543 
1 
1.1176 
4 
1.2343 
7 
1.3247 
6 
0.6874 
9 
0.9589 
2 
1.1209 
17.5 
1.2365 
8 
1.3268 
e 
in mm 
¿Off f 
21.9 
1.3286 
22.0 
1 
2 
3 
4 
22.5 
6 
7 
8 
9 
23.0 
1 
2 
3 
4 
1.3304 
1.3322 
1.3341 
1.3359 
1.3377 
1.3397 
1.3416 
1.3434 
1.3450 
1.3469 
1.3487 
1.3504 
1.3522 
1.3541 
1.3558 
6 
7 
8 
9 
24.0 
1 
2 
3 
4 
24.5 
6 
7 
8 
9 
25.0 
1 
2 
3 
4 
1.3574 
1.3593 
1.3610 
1.3627 
1.3644 
1.3662 
1.3679 
1.3694 
1.3713 
1.3729 
1.3746 
1.3762 
1.3779 
1.3795 
1.3811 
1.3829 
1.3845 
1,3861 
1.3878 
1.3893 
25.5 
6 
7 
8 
9 
1.3909 
1.3927 
1.3943 
1.3955 
1.3972