Oxygen Content of the Stratosphere
NATURE
544
SEPTEMBER
26, 1936
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Oxygen Content of the Stratosphere
AIR from different heights of the stratosphere was
brought down by registering balloons by means of a
new device for air sampling. As the apparatus was
protected against the low air temperature in the
stratosphere by a "Cellophane" case, it was possible
to employ ordinary stop-cocks.
At the desired
heights the latter were operated by an electrical
arrangement actuated by aneroids. The glass vessels
for air sampling were constructed so that the oxygen
content could be determined in them by means of
heating metallic copper without it being necessary
to change the vessel. Before and after heating the
copper the volume was brought to the same level,
so that the diminution of pressure divided by the
initial pressure immediately gives the oxygen content.
The following table gives the values obtained for
the oxygen contents :
Date
24. 8.36
19.12.35
5.12.35
18. 8.36
5.12.35
12. 2.36
6. 5.36
I
Height
(km.)
0
14·5
18·5
19
22·2
24
28-29
I
Oxygen content
(per cent by vol.)
20·92
20 ·89
20·84
20 ·87
20·57
20 ·74
20 ·39
±
±
±
±
±
±
±
0·02
0·05
0·02
0·02
0·05
0·02
0·05
In approaching the height of 20 km. the oxygen
content is diminished noticeably in comparison with
the value at the earth's surface (20·90-20·95 per
cent) ; above 20 km. the diminution begins to be
more pronounced ; at the greatest height there is a
deficit of 2-3 per cent of the oxygen content. The
values agree with the determination of the helium
content of the stratosphere by F. Paneth 1 , who at a
height of 21 km. finds a helium surplus of 8 per cent.
It is remarkable that at heights greater than
20 km. the values differ rather considerably. This is
probably due to the weather conditions. In air masses
of polar origin it seems that the diffusive separation
begins at lower heights than in equatorial regions
where the top of the troposphere is remarkably higher.
The insolation in equatorial regions is very much
stronger, and the turbulence of the atmosphere
reaches to greater heights. Lepape and Colange 2
also find that the content of helium plus neon in
the stratosphere is slightly increased, and more
variable than on the earth's surface. If my assumption
is true, then the height of the ozone layer in the
stratosphere should also be lower in polar regions
than in equatorial regions, first, because the oxygen
content in polar regions decreases with heights more
rapidly than in equatorial regions, and secondlywhich is perhaps of even greater effect--because the
greater stability of the atmosphere in the polar
regions tends to increase the diffusion of the heavy
ozone downwards.
A more detailed report will be published shortly
in Luftfahrtjorschung.
Physikalisches Institut der
Technischen Hochschule,
Stuttgart.
Sept. 6.
E.
REGENER.
F. A. Paneth and E Gliickauf, NATURE, 136, 7l7 (1935).
'A. Lepape and G. Colange, NATURE, 137, 459 (1936).
1
Absence of Cosmic Rays from Nova Lacertre
THE appearance of Nova Lacertre gave us a. second
opportunity of investigating whether the conclusion
at which we arrived when investigating the relation
of Nova Herculis to cosmic rays 1 , namely, that no
cosmic rays emitted from novre are observable, was
correct or not. For this purpose we have turned the
centre line of the field of our apparatus (field of the
apparatus : 40° in east-west, 10° in north-south
direction; 36 em. lead between the counters) as soon
as the outburst of the nova was signalled, into such a
position that the centre line showed only an angle of
2° 09' north of the nova at culmination. In such a
position a set of measurements was performed from
June 19unti1July 17,1936.
z
h
.,
1,)
0
cc:
1
2
0
.5
6
11
16
Z:J
.S.T
.s !1.E.T
.2*
FIG. 1, Variation of cosmic ray intensity (average values) with
sidereal time (S.T.) and Central European time (M.E.T.). The horizontal straight line above the diagram Indicates the time during
which Nova Lacertre passed through the field of our apparatus, and
the arrow the time of its culmination.
Fig. I shows the average variation of the intensity
for the different hours of the day, as a percentage
of the mean value. As can be easily seen, the curve
indicates only the well-known diurnal variation, and
no increase at the time of culmination of the nova.
The assumption that no effect of the nova was
detectable, because its cosmic radiation was of much
shorter period than the duration of the measurement,
cannot be maintained, for even the ratio of the
© 1936 Nature Publishing Group
(...truncated)