September 1969 Electronics Illustrated
Table
of Contents
Wax nostalgic about and learn from the history
of early electronics. See articles from Electronics Illustrated, published May 1958
- November 1972. All copyrights hereby acknowledged.
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As with many areas
of electronics communications, much of both the initial and continued research in
atmospheric scattering of electromagnetic signals was/is done by amateur radio operators.
The phenomenon is routinely used for accomplishing long distance communications
(DX, in Ham terms) by exploiting the reflection property of ionized layers when
radio signals impinge at a certain angle. The portion of the signal that returns
to the transmitter location, when monitored, can provide information to the sender
about the height, distance, and frequency range of the reflecting atmospheric layer.
Some of the first indications of backscattering were noticed by radar operators
who would receive echo returns from "phantom" targets that were really atmospheric
reflections.
They're Taking the Guesswork out of Scatter Communications
To get a good signal into a target area international short-wave
broadcasters now are probing the ionosphere.
By Stanley Leinwoll
International broadcasters located in the United States are developing a system
based on the principles of radar that will boost the signals aimed into target areas
without requiring increased power or antenna gain. The system, called backscatter
sounding, is expected to be operational within a year. If successful it could revolutionize
broadcasting techniques on both short-wave and amateur bands.
How It Works
Radio waves striking objects on or above the earth are reflected and scattered
in all directions. A small portion of this reflected energy always returns to its
source. By measuring the time between the transmission of the energy and its return
to the point of origin, accurate determination of the reflecting objects distance
from the transmitter can be made.
We know radio waves travel at the speed of light - 186,000 mi. per second. A
delay of a microsecond between the time a radio wave is transmitted and the time
it's received back at the transmitter corresponds to a round trip (984 ft.) over
a path 492 ft. long. All radar measurements are based on this principle. Most radar
devices, however, operate at frequencies of 1,000 mc or more because short wavelengths
give a more accurate determination of the size and shape of physical objects.
Shortly after World War II it was discovered that short radio waves (between
3 and 30 mc) display radar-like characteristics. These properties help to reveal
information about a signal as well as valuable information about the ionosphere.
Fig. 1 - Nomograph shows relationship of backscatter time to
target distance. Height of Ionosphere (up to 300 mi.) depends on amount of solar
activity.
Long-distance short-wave communication is possible because there exists in the
atmosphere a series of electrified layers collectively referred to as the ionosphere.
The ionosphere is capable of reflecting radio waves in the high-frequency (3-30
mc) portion of the RF spectrum. However, the ionized gases making up the ionosphere
change from day to night, from season to season and over an 11-year cycle dependent
on the number of sunspots.
A high-frequency radio wave entering the ionosphere will either be absorbed,
be reflected back to earth or be lost in outer space. Reflection back to earth depends
on the amount of ionization in the layers, the frequency of the radio signal and
the angle at which the wave strikes a particular layer. Most radio energy returning
to earth is reflected by the earth back to the ionosphere, where it is again reflected
to a distant point. These sky waves make communication over great distances possible.
Backscatter Technique
Because of irregularities on the surface of the earth, a small portion of the
energy striking it at some point will be scattered in all directions and even scattered
back toward the transmitter. (Hence, the term backscatter.) By setting up a directional
antenna and a receiver that feeds its output into an oscilloscope the backscattered
signal can be monitored and analyzed right in the vicinity of the transmitter.
Engineer for Radio Free Europe compiles detailed charts as he listens to
international short-wave band. Effort is made to Improve RFE's signal. UPI Photo
If the transmitter should send a series of pulses at different frequencies, say
beginning at 3 mc and sweeping up at predetermined intervals to 30 mc, a receiver
monitoring these pulses will show just what frequencies are being backscattered.
Some of the signals will be absorbed by the ionosphere, some will penetrate it and
some will be propagated. Backscatter sounding tells the broadcaster which frequencies
are being propagated by the ionosphere and consequently which frequencies can be
used for communication to a specific area of the world.
In addition, when the pulses are viewed on a scope, the time delay can be calculated.
The time delay between the transmitted pulse and received echo gives the approximate
location of the point of reception. This is illustrated in Fig 1. If a scope shows
a delay time of 20 milliseconds at a particular frequency, we can arrive at our
target's distance by estimating the height of the ionosphere (HL). In general, 300
kilometers is a reasonable assumption and the chart gives us a target distance of
about 2,900 kilometers. Since no energy has been returned from a closer location
it follows that the target distance was about 2,900 kilometers (or 1828 miles).
Radio Free Europe. The backscatter sounding system currently under test by Radio
Free Europe is more sophisticated than the technique described above. It consists
of a high-gain curtain antenna for transmitting and a frequency-shift pulse keyer
at the input. This device shifts the carrier frequency of a transmitter for short
periods of time while pulses of energy are sent out. A receiver and antenna system
are tuned in step with the shifted carrier. The antenna consists of nine vertically-stacked
cubicle-quad elements mounted on a 108-meter tower. It operates in the 11.8-, 15.3-,
and 17.8-mc international short-wave bands and can be adjusted so that the vertical-radiation
angle changes to receive maximum energy at different angles (from 3.5 to 22.5 degrees).
Changing the optimum receiving angle is important because it helps determine
which receiving mode is producing the strongest signal at a given frequency. International
broadcasters such as Radio Free Europe operate on a fixed frequency schedule and
cannot utilize backscatter equipment to determine which band is propagating best
in order to make an assignment in that band. Instead, they have to determine which
angle is producing the strongest signal on a particular frequency and then adjust
the transmitting antenna to fire at that angle; this way a better signal is propagated
into the target area.
Fig. 2 - RFE backscatter depends on finding best angle propagation
of signal at a given frequency. Distance increases as angle decreases.
The technique of adjusting your radiation angle is called slewing. RFE has a
number of vertically-slewable antennas and is planning to construct others to take
maximum advantage of its backscatter equipment. Fig. 2 shows what a typical display
looks like. Mode I corresponds to the lowest transmitting angle and Modes 2 to 5
refer to increasing vertical angles. As expected, Fig. 2 shows that as the transmitting
angle is decreased, the backscattering distance increases. Modes 1 and 2 show energy
returning from two distinct zones; this is probably caused by reflection of the
signal from different layers of the ionosphere. This situation frequently occurs
during daylight hours.
Amateur Applications
Backscatter sounding promises to lend itself even more to amateur radio than
to international broadcasting because the amateur is not limited to a fixed frequency
schedule. To understand the great potential for an amateur backscatter network consider
the display shown in Fig. 3. Instead of making soundings at different radiation
angles on a single frequency, we switch to soundings for the different ham bands
(i.e., 40, 20, 15, 10 and 6 meters).
The first pulse is the one received directly from the transmitter. The 40-meter
trace shows two other pulses, one relatively close to the transmitter, the second
about twice as far away. This is probably due to a second-hop transmission. Because
of signal strength. the signal has returned to the ionosphere a second time, been
reflected by the earth a second time, and both backscattered signals have been picked
up at the receiver.
Fig. 3 - Backscatter display for amateur bands. First pulse
is from transmitter; echoes indicate distance of transmission (greater with higher
frequency).
Succeeding traces show that as frequency is increased, the skip also increases-until
at 6 meters we find there is no trace at all. This means that at 6 meters the ionosphere
was not propagating and the radio energy was probably penetrating into outer space.
Communication on all the other bands was possible, however.
Fig. 3 emphasizes the significance backscatter sounding has for the radio amateur.
Here is a method by which instantaneous information on skip in various bands can
be obtained. One might envision a network of backscatter sounding stations run by
the ARRL and located at various points in the United States. Each such station would
have a horizontally-rotatable backscatter array so that soundings could be made
in all directions.
Periodic announcements could be made over official ARRL station W1AW, as well
as over regional stations, giving the best bands and the approximate skip distances
on all bands. By listening to these stations hams would know which bands to operate
in. Such forecasts would help CBers and SWLs too.
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