The Antenna Research Laboratory
March 1950 Radio & Television News Article
1950, say the author of this story, "No longer are 'aerials' merely required to transfer electromagnetic energy
into space," in reference to airborne platforms. Following great advancements in radio and radar technology during
World War II, great interest lied in what would later become referred to as 'stealth' technology and in secure
communications. The transition of aircraft speeds into the realm of supersonic also mandated that projections beyond
the main airframe outline be either eliminated or very much minimized. The long cable aerials that stretched from
the cockpit area to the tip of the vertical fin, and the round direction finding antennas hanging from below could
not be accommodated at airspeeds above about 300 knots. The aerodynamic drag would be excessive and the forces
would tear the antennas apart. Douglas Aircraft set up one of the first antenna measurement laboratories specifically
to address those issues both for airborne and shipboard platforms.
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By Joseph M. Boyer, Consulting Engineer
Douglas Aircraft's laboratory eliminates costly full-scale experiments by using tiny replicas in solving complicated
antenna design problems.
Fig. 1. Tiny crystal receiver shown in engineer's right hand, is used to detect signals from model antenna.
Plate on side of model plane is removable to permit receivers to be installed within the hollow fuselage of
Never before in the history of radio has interest in the antenna beam been at such
a feverish pitch! No longer are "aerials" merely required to transfer electromagnetic energy into space. Experts
today, working with surrealistic shapes of metal and plastic, are molding radiated energy into the precisely shaped
beams needed for the varied classes of radar - for highly eavesdrop-proof communication links, or even changing
the beam's contour from instant-to-instant, automatically following the boiling vagaries of the Heaviside layer.
The center of all such investigation is the antenna research laboratory. Here antenna engineers work with
worlds in miniature. Out on the model antenna range of one such laboratory it is not uncommon to see a complete
scale replica of a television station: the tiny buildings, the accurately-made antenna towers, even the green rolling
hills of the surrounding country. This Lilliputian model slowly revolves on a turntable, a large horn-type radiator
some distance away "illuminating" it with microwave signals. The miniature antennas of the model station detect
such energy and feed it back to high gain amplifiers in the laboratory. Thus, as the model turns, automatic plotting
instruments draw an accurate trace of the radiation pattern of the station for later study. Such model tests save
costly cut-and-try procedures previously made on full scale installations.
Even more important, in view
of our National Preparedness Program, is the investigation of aircraft antennas. With aircraft now operating both
near and beyond the speed of sound, no object of any kind is permitted to project from the sleek, polished metal
skin to add parasitic drag. This requirement is a death warrant for the numerous masts and wires which once were
draped lavishly over aircraft exteriors. In the high-pressure search for distinctly new antenna types which may
be faired flush into the skin of a high speed airplane, several of the large airframe manufacturers have aided the
radio art immeasurably by taking the lead in such research. In order to see, at first hand, the evolution of a new
antenna, a visit was made to the El Segundo, California antenna laboratory of the Douglas Aircraft Company which
pioneered in this field. Here, work begins with the presentation of the Navy specifications to the aircraft antenna
Such specifications call for a v.h.f. communications antenna. This unit is to be mounted flush
within the skin of a high speed carrier type fighter, yet provide full 360-degree coverage about the horizon. When
used for transmitting, the antenna must produce most of its signal in a zone approximately twenty degrees above
and below the airplane. Efficiency must be equal to the older type protruding antenna because airborne power requirements
are stringent. Finally, as if to complete the designer's frustration, such an antenna must be capable of operating
from 300 to 5901 megacycles while remaining matched to the coaxial transmission line feeding it. Specifically,
it must not exceed a voltage standing wave ratio of 2 to 1.
The resourceful engineer begins a strenuous
period of reading the available technical literature, making rough preliminary calculations, and weighing and discarding
a number of configurations which come to mind. In this process the crude pencil sketches which litter his desk would
be unrecognizable to prewar engineers. There is not a sign of wires or porcelain insulators. One sketch may show
a small square portion of the metal skin isolated from the surrounding surface and fed by a tapered funnel section
of coaxial line. Or perhaps a flat disc of polystyrene a foot or so in diameter is shown, excited at its center
by a sphere of silver designed to function as a wide-band dipole.
Fig. 2. Diagram shows position of model aircraft and rotation axis for each of the three principal
"cuts" made during pattern study.
Finally, the antenna designer may feel he has what is needed. Before he makes a preliminary shop
drawing he must refine his design. This step involves extremely complex calculations. For some such problems he
must discard his slide rule, set up the equations he wishes solved, and pass them on to electronic or mechanical
computing machines. Satisfied that his "brain child" has a good chance of success, the engineer authorizes the experimental
shop to fabricate a full size antenna and pass it on to the antenna laboratory for measurements.
Fig. 3. Typical aircraft antenna radiation pattern. The pattern shown was photo. graphed on the screen of antenna
range cathode-ray "pattern painter." Magnetic deflection coils move in synchronization with rotation of model
under study, tracing out an accurate polar diagram of antenna signal variation around the plane model.
Fig. 4. Operating and recording position. Shown are the v.h.f. and microwave transmitters, power supplies, and
switching panel. In front of operator is a pen recorder and the Douglas cathode-ray "pattern painter." The "full
moon" labeling device is seen as the white window below the cathode-ray tube.
Fig. 5. A coaxial slotted line in use. The slotted coaxial line is used to measure the voltage standing wave
ratio of the prototype antenna. The radiator under test is mounted on the outside metal surface of the wall,
directly behind the Hewlett Packard Voltage Standing Wave Ratio meter shown in photo.
The antenna laboratory technician, highly-trained and experienced
in this specialized field, first may mount the prototype antenna upon a large ground plane. This usually is a metal
wall forming one side or the roof of the laboratory building. In some cases the antenna may actually be mounted
into a full scale wire cloth mock-up of the aircraft itself. A precision section of slotted coaxial transmission
line (Fig. 5) is connected in series with the antenna and a laboratory v.h.f. oscillator. Beginning at one end of
the frequency range to be covered by the antenna, the technician makes measurements of the voltage standing wave
ratio in the transmission line. If the antenna is a perfect match there will be no change in the measured voltage
from one end of the transmission line to the other. Such "flat" lines, however, are rarely encountered. There usually
is a small v.s.w.r, but it must be under the called-for 2:1 ratio. If the designer has done his job properly this
condition will be met over the entire frequency range desired. So far so good, but more hurdles remain to be cleared.
Once more an order goes to the experimental model shop: "Fabricate one 1/20th scale model of the antenna
for range pattern tests." The men who receive this assignment are not ordinary machinists or metalsmiths. They are,
for the most part, former instrument makers used to working with tiny precision parts under a powerful lens. They
are fantastically ingenious in devising ways of soldering and welding parts the size of a pin head into place within
complex assemblies, of bending and twisting metal into shape while it is glowing in the flame of an alcohol lamp.
An idea of the difficulty of their job can be obtained when it is realized that ordinary RG 8/U coaxial cable reduced
to 1/20th scale is the size of store string. The inner conductor of such cable is the diameter of a human hair,
yet must be soldered to the minute antenna without melting an extremely thin, easily-destroyed polyethylene sheath
which insulates the assembly. Upon completing his exacting task, the model shop craftsman places the tiny antenna
into the metal skin of a previously prepared 1/20th scale model of the aircraft in which it is intended to see service.
Radiation Pattern Measurements
Briefly, the basic idea behind the use of the model
antenna pattern range is this: an aircraft operates far from the earth. The only environment which affects the antenna
on the airplane is the configuration of the craft itself. Any attempts to measure radiation patterns on a full size
aircraft resting on the earth would be futile. Patterns taken by means of flight tests are not only prohibitively
expensive, difficult to measure and interpret, but usually end in doubtful results. However, by reducing the aircraft
to 1/20th or 1/40th of the full scale dimensions it is possible to mount it from 40 to 60 wavelengths from the ground.
This can be done because the operating frequencies must also be multiplied by 20 or 40 to keep in step with the
model dimension change. That such theory is correct, when suitable precautions are taken, has been demonstrated
The scaled-down model aircraft, complete with its test antenna, is mounted upon a special
dielectric tower, the base of which rests on a motor-driven turntable. Within the hollow belly of the little plane
is a simple receiver usually consisting of an impedance matching transformer and a silicon crystal detector or hot
With the tower placed as many as 100 wavelengths from the laboratory building, technicians
energize a tunable Klystron transmitter which excites a large horn type antenna projecting toward the model through
the wall of the laboratory. The transmitter's signal is amplitude modulated by a square wave with a repetition rate
of 1000 cycles. A square wave is needed to avoid frequency modulation of the Klystron. Operating frequency is carefully
adjusted to be 20 or 40 times the full scale point in the spectrum where the antenna is intended to function.
Reference to Fig. 2 will make clear the patterns to be described. The antenna specialist refers to such
patterns as "cuts." The first "cut" is made by slowly rotating the model so that every portion of the plane's horizontal
axis is exposed to the radio beam from the laboratory transmitting horn antenna. The model on the tower is then
turned 90 degrees and again rotated by means of the turntable, exposing its nose, belly, topside surface, and tail,
to the beam. Finally, a "cut" is made presenting the wingtips, belly, and topside surface of the model. This triad
of cuts - the horizontal, longitudinal vertical, and transverse vertical, are fundamental in any pattern investigation
and quickly tell if the radiation pattern of a new antenna is going to meet specifications. At least the three patterns
just described must be made at frequent intervals over the simulated radio spectrum in which the antenna is going
to operate. An antenna may frequently have the desired radiation pattern at one end of its frequency range and fail
miserably at the opposite extreme.
Leaving the antenna designer for the moment with his problem let us enter
the laboratory building proper and investigate the equipment used to study the radiation characteristics of antennas.
Several racks of audio amplifiers are the first instruments seen. These are quite special items. There are preamplifiers
capable of boosting the few millivolts or so of signal received from the model to about 10 or 20 volts. This piece
of equipment is linear in response and features a tuned feedback network which permits the amplifier to operate
with full gain only at 1000 cycles. All other signals of random frequency and noise are sharply attenuated. The
output of the linear preamplifier drives a logarithmic amplifier which is also sharply tuned to 1000 cycles. Logarithmic
response is desired so as to properly record variations in the model signal which may extend over 50 decibels or
more. To graphically present the radiation pattern several different types of recorders are used.
The most common is a so-called polar recorder in which a pen is driven by signal variations from the model through
the use of a servo-mechanism. In appearance this unit may resemble an automatic phonograph record changer. A circular
piece of polar graph paper is placed upon its turntable and centered by means of a pinpoint of light at the center.
The paper edges are clamped down by means of small Alnico magnets. Rotation of the recorder turntable is synchronized
by means of selsyns to turn in step with the model out on the pattern range. When the model is rotated the servo-driven
pen moves back and forth on a radius, tracing out the pattern.
Fig. 6. General view of antenna model pattern range. A scale model of the Douglas "Skyraider" is shown mounted
on the motor driven dielectric tower. The large electromagnetic horn antenna to the right is being turned to
change electric polarization of signal to model. Smaller horn to the left of the picture covers the three centimeter
Fig. 7. Scale model aircraft and antenna shown in process of construction. Craftsman in foreground solders a
connection in minute cavity type slot antenna. The 1/20th scale aircraft model shown is of wood.
Also used is a cathode-ray pattern painter
illustrated in Fig. 4. This instrument has several important advantages over the pen type recorders. One of the
most valuable is lack of mechanical inertia. There are occasions when a radiation pattern being recorded varies
from a deep null to maximum signal intensity within a fraction of a degree of rotation. Even for the slow speeds
at which the model turns (3/4 to 1 r.p.m.) this condition requires the pen to whip over the graph paper at an exceptionally
fast rate. The consequent lack of response and "overshooting" of the pen distort such patterns.
is absent in the cathode-ray "pattern painter." Here the magnetic deflection coils actually rotate about the neck
of the cathode-ray tube in synchronism with the model. Thus, as the signal intensity changes the electron beam can
follow the speediest variation with no time lag, no error. When used for radiation pattern plotting the screen (long
persistence) of the tube is photographed on 35 mm. film for a permanent record (Fig. 3), Another fine feature of
the particular model developed at the Douglas laboratory is an edge-lighted Lucite disc seen in the illustration
mounted below the cathode-ray tube. This disc is called the "full moon" because of its characteristic of glowing
with evenly distributed white light. All pertinent data such as frequency, aircraft type, and description of the
"cut," is typed on transparent gummed paper and this is then fixed over the face of the "full moon." Easily photographed
on the same film as the pattern, such a screen label feature permits the laboratory to obtain a very complete, foolproof
record of work in progress.
Antenna laboratories must have transmitters
available to cover enormous ranges of frequencies. To see the reason why, let us assume that the full scale frequencies
of three antennas to be tested span the region 80 to 1600 megacycles. Not only must oscillators be on hand for these
exact frequencies but, in addition, if the model range measurements are to be made at 1/20th scale, r.f. generators
are required for the simulated range 1600 to 32,000 megacycles. Spanning such an expanse of radio territory calls
for an imposing collection of coaxial cavity, and "butterfly" type oscillators, many, many Klystron tuners as well
as elaborate high-voltage regulated power supplies and frequency measuring equipment of great accuracy. It is no
wonder that antenna engineers always ask for bar-gains in frequency coverage when shopping for transmitters; otherwise
such equipment would overflow the laboratory.
To cover the multitude of problems which trouble an antenna
specialist's slumber would be beyond the scope of this article. Some of the especially serious ones, however, may
be of interest. The first and worst of these is spurious reflected signals. Exactly the same problem is faced by
television service technicians in the form of "ghosts." The aircraft model itself is, of course, placed carefully
"in the clear." Any posts, buildings, fences, or personnel in its vicinity would reflect signals into the model
as if they were secondary transmitters. Such reflections, depending upon their instantaneous phase, either add or
subtract in certain directions from the true magnitude pattern of the model.
The real villain of this story, however, is the ground or platform upon which the antenna laboratory rests. "Splash"
from this source is almost impossible to eliminate completely. Great care is exercised in designing the large sectorial
horn antennas which "illuminate" the models so that just enough beam width with uniform phase front is produced
to cover the model with r.f. energy. Even though this precaution lowers the magnitude of floor "splash" it does
not completely remove it. Sometimes low metal fences properly called detraction edges are placed on the model range
to deflect the "splash" signal into a harmless area. Placing these fences for each frequency used (and sometimes
as many as 200 "cuts" are made on a single model) is more of an art than a science.
Fig. 8. Close-up of 1 cm. transmitter and horn antenna. A complete 30,000 mc. Klystron transmitter, cavity wavemeter,
and high gain horn radiator makes only a light handful of microwave equipment.
Fig. 9. Slot antenna and cable. The size of a pair of 1/20th scale slot antennas and miniature coaxial cable
may be judged by comparison with hand holding them.
Fig. 10. View of computer showing vacuum tube bays. Mathematician inspects plug board which inserts problem
into the 1285 vacuum tube electronic computer used to solve complex antenna equations. Such machines are now
routine tools in the search for new antenna designs and antenna improvements.
Fig. 11. View of "feed" end of large horn type antenna. Coaxial cable shown supplies v.h.f. energy to probe
"feed" for the large horn type "illuminating" antenna. Microwatts are precious, and technician carefully adjusts
the matching stub for the maximum obtainable signal.
is the small coaxial cable which conveys the detected signal from the model down the tower to the laboratory. This
is, of course, a metallic conductor of many wavelengths projecting from the model. Pattern distortion will be introduced
by this cable, and only highly experienced personnel can minimize this difficulty by judicious placement of the
cable when setting the model up for a "cut." To overcome this hazard some researchers have actually placed midget
transmitters inside the model aircraft. Battery power or an air-driven generator energized by a high pressure hose
are used, but the attendant cooling problems and frequency drift due to lack of power supply regulation makes this
technique a last resort measure.
The problem of distance in wavelengths at the operating frequency between
the model under test and the "illuminating" horn antenna poses, at times, a nightmarish enigma for the antenna worker.
In order that an accurate radiation pattern be secured, the model aircraft must sometimes be placed as many as 100
wavelengths from the laboratory antenna, otherwise true "free space" conditions are not realized. Even at the microwave
frequencies 100 wavelengths may be a sizable distance physically. Unfortunately, the power output of laboratory
type Klystron tubes is only about 200 milliwatts for the region up to about 8000 mc. and 40 to 50 mw. for frequencies
above this. Sensitivity of the simple receivers used in the models is quite low and, upon numerous occasions, the
model simply cannot be placed at the required distance and still secure sufficient signal to record a pattern. The
model tower must then be moved into the so-called "near zone" region and many hours spent in calculations and educated
guesses in order to replot the pattern to some degree of accuracy. The uninitiated invariably suggest going to higher
powered transmitters such as radar pulsed units. When such suggestor, however, ponders over the problem of building
or purchasing the number of high power, room-size radars needed to cover the frequencies called for, he soon realizes
that a fairly large warehouse would be needed to mount them for use.
Rejoining the antenna engineer it is
found that his new antenna has successfully completed its preliminary radiation pattern tests. While mildly jubilant
he must still subject his creation to an investigation to determine its response to cross-polarized signals. Also
he must investigate what effect additional structures, such as wing mounted rockets or bombs, have on its pattern.
The worried frown will remain on his brow for some time to come as he follows the antenna through the intricate
maze of production decisions, cost analysis, and lastly the flight test which places the final stamp of approval
on his work.
While emphasis has been placed on the aircraft antenna because of its present importance, it
should be made clear that the laboratories of such institutions as Ohio State University are carrying on programs
of investigation into many other aspects of the antenna problem. For example, in the study of land-based radio stations
scientists must content themselves not only with dimensional perfection with regard to towers and buildings, but
must also actually design the soil of these scale models to have proper conductivity at the higher model frequencies
in order that it simulate the soil found in the region under study. The "guess and by-gosh" methods of the past
in making costly antenna installations are slowly giving way to exact knowledge.
Last but by no means least,
Naval research centers are engaged in measuring the radiation patterns of antennas mounted within the complex maze
produced by a ship's masts, cables, and other marine structure. As might be expected, Naval antenna designers must
take the sea into account when making their scaled-down ships for range tests. To an electromagnetic wave a ship
resting upon the sea appears to have an exact mirror image directly beneath it. This can be duplicated on "the Naval
antenna model range by cutting a ship model off at its water line and resting it upon a large sheet of metal. In
lieu of this, two ship models are constructed, sawed off at the water line, and one fastened upside down to the
waterline of the other. The technique of making the actual radiation pattern measurements is identical to that described
1 Military frequencies are classified. Those given are only