56
THERMODYNAMIC METEOROLOGY
TABLE 15
Comparison of the Pressures Computed by the Non-Adiabatic
Formula and those Observed at Great Heights
Heights
in
Meters
Lindenburg
May 5, 1909
Lat. +52°
Lindenburg
July 27, 1908
Lat. +52°
Atlantic Ocean
Sept. 9,1907
Lat. +26°
Atlantic Ocean
June 19,1906
Lat. -2°
z
Be
B a
Be-
Bo
Be
B 0
Be —
Bo
Be
Bo
Be —
Bo
Be
Bo
Bc-Bo
19000
18000
.0589
.0600
-.0011
17000
.0679
.0670
+.0009
.0692
.0690
+
2
.0742
.0740
+ .0002
16000
.0794
.0790
+
4
.0808
.0790
+
18
.0861
.0860
+
1
15000
.0927
.0930
-
3
.0945
.0950
—
5
.1004
.1010
-
6
.1021
.1020
+.0001
14000
.1082
.1090
—
8
.1101
.1110
—
9
.1177
.1170
+
7
.1203
.1200
+
3
13000
.1266
.1270
—
4
.1289
.1300
—
11
.1381
.1380
+
1
.1409
.1410
—
1
12000
.1484
.1490
—
6
.1512
.1520
—
8
.1615
.1610
+
5
.1641
.1640
+
1
11000
.1744
.1750
—
6
.1772
.1780
—
8
.1881
.1880
+
1
.1902
.1900
+
2
10000
.2041
.2050
-
9
.2067
.2080
-
13
.2179
.2180
-
1
.2191
.2190
+
1
9000
.2374
.2390
_
16
.2399
.2410
11
.2509
.2510
_
1
.2512
.2510
+
2
8000
.2746
.2760
—
14
.2769
.2780
—
11
.2875
.2880
—
5
.2870
.2870
0
7000
.3159
.3180
—
21
.3181
.3190
—
9
.3281
.3290
—
9
.3268
.3260
+
8
6000
.3619
.3630
—
11
.3639
.3650
—
11
.3732
.3740
—
8
.3709
.3710
—
1
5000
.4128
.4130
-
2
.4149
.4160
-
11
.4233
.4240
-
7
.4200
.4200
0
4000
.4696
.4700
_
4
.4716
.4720
_
4
.4789
.4800
_
11
.4747
.4750
_
3
3000
.5330
.5340
—
10
.5344
.5340
+
4
.5402
.5410
—
8
.5356
.5350
+
6
2000
.6035
.6040
—
5
.6040
.6040
0
.6077
.6060
+
17
.6031
.6030
+
1
1000
.6823
.6840
—
17
.6806
.6810
—
4
.6821
.6820
+
1
.6783
.6780
+
3
Surface
.7599
.7599
0
.7551
.7551
0
.7640
.7640
0
.7610
.7610
0
The differences between B c and B 0 are probably due to an
assignment of the temperature to a slightly erroneous height,*
owing to the movement of the balloon ahead of the record of
the barograph and thermograph, which requires a correction
for lag. The pressure recorded by the aneroid is for the mixture
of dry air and aqueous vapor, so that by (75) for the same height,
where T = T 0 and p = p 0 ,
(185) P 0 = P (l - 0.378
B 0 = B (l - 0.378
where P or B is the dry air pressure, and Po or B 0 the
pressure in the mixture, e being the vapor pressure in the
* The heights have been read from the aneroid record and are not corrected
for the supposed lag; but the error is less for T than for P because T changes
more slowly than P.