June 1960 Radio-Electronics
[Table of Contents]
Wax nostalgic about and learn from the history of early electronics.
See articles from Radio-Electronics,
published 1930-1988. All copyrights hereby acknowledged.
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If I told you I just
learned that there exists an ionized region of the upper atmosphere which
affects electromagnetic waves, and is modulated in intensity and size by
activity on the sun, you would understandably respond with something like,
"Where have you been. Tell me something we haven't known for half a century."
Sure, but in 1960 when this "Ionized Band Encircles the Earth" article was
printed in Radio-Electronics magazine, it was news to most people. The
presence of an ionosphere had been theorized and shown to be existent based on
ground-based experiments beginning a few decades earlier, but it was not until
the
International Geophysical Year (IGY) space shots running from 1957 through
1958 that direct measurements confirmed suspicions. Not mentioned by Mr. Warsaw
was the big part amateur radio operators (aka Hams) played in both the discovery
and early characterization of atmospheric reflection. As I write this,
Solar Cycle 25 is just starting to wind down, having provided a couple years
of phenomenally good long distance (DX) communications.
Ionized Band Encircles the Earth
Fig. 1 - Effect of the ionized band and its relation to sunrise.
By David Warshaw
Electronic studies point toward the discovery of a 100-mile-wide ionized band
that circles the earth.
Recordings of atmospherics at 27 kc indicate the presence of an ionized band
about 100 miles wide encircling the earth at an altitude of 50 miles. Members of
the AAVSO1 Solar Division, using transistorized receivers2
at various locations in the United States, are recording Sudden Enhancements of
Atmospherics (SEA's) at 27 kc for the National Bureau of Standards Indirect Flare-Detection
Patrol. SEA's caused by solar flares, are received and recorded only during daylight
hours, although the equipment operates continuously day and night. As a result,
a very strange pattern in the recording traces of the observers was discovered.
The pattern showed a small dip and hump, or a fall and rise in level, about a half-hour
before sunrise.
What Does It Mean?
The reason for the strange dip pattern on the recordings 36 minutes before sunrise
could be an ionized band, about 100 miles wide, 50 miles above the earth. About
36 minutes before the earth's sunrise, reception of the atmospheric pulses is weakened
for about 8 minutes, during the period when the ionized band is located directly
between the receiving station and the high E- and F-layers. The ionized band temporarily
blocks the atmospheric pulses normally reflected via these layers to the receiving
station (Fig. 1, path b).
The reason for the hump pattern - which follows the dip, appearing on the recordings
about 20 minutes before sunrise - could be the existence of a space, or weakly ionized
separation, in the D-layer region. The hump indicates an improvement in the reception
of the atmospheric pulses and a consequent rise in the level of the recorded trace
(Fig. 1, path c).
Fig. 2 - Recorded trace shows hump and dip that indicate
the presence of the ionized band.
When the earth has rotated the receiving station to a location 20 minutes before
sunrise, the atmospheric pulses become stronger for about 8 minutes. They are then
reflected from the high E- and F-layers, down through this separation to the receiving
station. The separation between the ionized band and the beginning of the D-layer
is about 100 miles. (At New York's latitude, 1° or 4 minutes of the earth's
rotation is equal to about 50 miles. The duration of the dip and the hump on the
record is about 8 minutes for each, or 100 miles.)
Not only does the before-sunrise pattern of the dip and hump indicate the presence
of a narrow ionized band encircling the earth, but there is also an after-sunset
pattern of a hump and dip to offer additional proof of its existence. A recorded
trace from an observing station on the West Coast of the United States clearly shows
both the sunrise and sunset patterns for Feb. 28 and March 1, 1959 (Fig. 2). The
West Coast member of the AAVSO observing group in China Lake, California, is Justin Ruhge, a physicist at a missile base, who operates his own homemade receiver in
his spare time. His equipment runs unattended for several days.
When atmospheric pulses are received, they are stored for about 60 seconds, averaged
into a direct-current output, then graphically recorded. The normal recorded trace
is rather high during the night and low during the day. The D-layer, created only
by the sun's rays, does not exist at night, so atmospheric pulses received during
the night from the thunderstorm centers are reflected from the higher E- and F-layers.
When the reflecting ceiling is higher, it reflects from greater distances and the
receiving station is able to receive a greater number of atmospheric pulses from
more thunderstorm sources on this very low frequency of 27 kc.
How the D-Layer Works
As the earth rotates the receiving station into daylight, the D-layer, formed
by the sun's rays, gradually begins to take form about 50 miles overhead, below
the higher E- and F-layers. As atmospheric pulses at 27 kc cannot pass through the
D-layer, it becomes the reflecting ceiling. Because the D-layer is lower, the number
of reflections increases and each reflection absorbs some of the energy of the atmospheric
pulses. As a result, the receiving station receives fewer and weaker atmospheric
pulses and the recorded trace gradually falls to a lower level. The trace usually
remains low during daylight hours, except when a solar flare causes an SEA.
On the daylight side of the earth, the sun's rays create the D-layer region,
an umbrella of ionization, 50 miles above the sunlit half of the earth's surface.
The amount of sunlight intensity concentrated on a surface increases with the sine
of the angle formed by the sun's rays and the surface (Fig. 3).
Fig. 3 - How amount of sunlight intensity increases with sine
of angle formed by sun's rays and surface.
Fig. 4 - Ionized band in Northern Hemisphere - Dec. 21.
For this reason the earth's surface is weakly illuminated at sunrise, but not
by the sun's direct rays. 50 miles directly above the earth at sunrise, the concave
or under surface of the D-layer region is also weakly concentrated for the same
reason. At this same 50-mile altitude the sun's rays form an angle of about 10°
to a neighboring layer or region which curves into the earth's shadow, and the concentration
on this layer is more intense.
The neighboring layer, about 100 miles wide, is the ionized band, which is separated
from the actual D-layer. It is illuminated and ionized by the sun's rays penetrating
the earth's atmosphere below the 50-mile altitude. Until recently it was not thought
probable that the ionizing rays could penetrate this lower altitude enough to induce
formation of the ionized band. The existence of radiation that penetrates below
the D-region is taken for granted nowadays.
For each day of August, 1958, when there were thunderstorms in the mountains
of New England, the recording traces received in New York failed to show the pre-sunrise
dip and hump patterns. When reception is from the northeast, instead of the usual
southwest, the reflecting ceilings are the E- and F-layers. The propagation path
from this source to the receiving station passes through the separation or space
between the D-layer and the ionized band (Fig. 1, path d). Because neither the D-layer
nor the ionized band blocks the path of propagation, the recording trace shows no
dip or hump pattern.
Position of the Band
On December 21, at geographic latitude 77.5° north, the ionized band is located
directly overhead for about 2 hours before and after noon, as shown in Fig. 4. However,
it is not difficult to plot the ionized band for the other seasons. For example,
during the summer it is directly overhead for about 4 hours around midnight at geographic
latitude 56.5° north. During the March and September equinoxes, at all latitudes
except 80° north, the ionized band is directly overhead a half-hour before local
sunrise and a half-hour after local sunset, for only a few minutes. At 80° north
latitude, the ionized band is directly overhead from about 10 pm to 2 am. When plotting
the position of the ionized band for any day of the year, remember that the ionized
band encircles the earth in a plane perpendicular to the sun's rays and situated
about 10° farther than the tangent point made by the sun's rays to the earth's
surface (sunrise). Some of the communications problems of airlines using the arctic
areas should be eased with the knowledge of the exact location of the ionized band.
Recent rocket observations of the upper atmosphere have indicated that shortwave
radio fadeout3 (5 to 30 mc) are caused by an extra ionized layer which
is formed by an increased intensity of X-rays emitted by the sun during solar flares.
This extra layer of ionization may extend downward to about 12 miles below the normal
D-layer while the higher layers appear to remain undisturbed during the fadeout.
The extra or additional layer, present during solar flares, temporarily makes a
better reflecting ceiling for atmospheric pulses on 27 kc, thus causing an SEA at
the same time as the solar flare.
AAVSO Solar Division members receive and record SEA's and send the recordings
to their chairman, H. L. Bondy in Flushing, N. Y. He analyzes the tabulations for
the Central Radio Propagation Laboratory, Radio Warning Services Section of the
National Bureau of Standards, in Boulder, Colo. SEA record tabulations are correlated
and published monthly by the National Bureau of Standards CRPL in series F, part
B, Solar-Geophysical Data, listed under Ionospheric Effects of Solar Flares. The
Indirect Flare Detection Patrol gathers the information appearing under SEA's, SCNA
(Sudden Cosmic Noise Absorption) at about 18 mc and bursts of solar radio noise,
which are also at 18 mc.
1 American Association of Variable Star Observers, Solar Div. 6130 157th St.,
Flushing 67, N. Y.
2 Solar-Flare Indicator-Transistorized, Radio-Electronics, August, 1956, and
Improved Solar-Flare Indicator, Radio-Electronics, January, 1959.
3 Science, Jan. 17, 1958
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