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by E. King Stodola; in 'Radar Developments to 1945', Edited by Russell Burns, Published by Peter Peregrinus Ltd., London, United Kingdom, on behalf of the Institution of Electrical Engineers. 1988 Pages 478 - 492 Web Sections...
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Some examples of post World War II radar in
the USA
E. K. Stodola
With the end of
World
War II, applications of radar to space exploration and utilization
produced
many new developments. One of the most spectacular of these was the
world's
first achievement of radar detection of the moon by the US Army's Evans
Signal Laboratory in early 1946. The background of our Evans Laboratory
group in precision frequency stabilization and signal processing in the
coherent pulse Doppler system, along with a strong laboratory support
system,
made it possible to successfully meet this challenge.
The moon had long
been considered as a radar target and could clearly be detected with
pulse
energies which were large, but not beyond available capabilities. As
World
War II ended, we considered the possibilities of moon radar detection.
The laboratory director at Evans Signal Laboratory Lt. Col. J.H.Dewitt,
an ex-engineer from the radio broadcasting industry, had several years
earlier attempted tire feat, but without success because of
insufficiencies
in various elements of his experiment (which he clearly recognised at
the
time).
We reconsidered
the problem in the light of the resources we had or could easily
assemble
at Evans Laboratory and concluded that we could work along the lines of
conventional radar but with constants greatly re-scaled to handle a
3520km
diameter target at a range of about 384000km and moving rapidly with
respect
to the earth's surface. These figures led to some of the following
radar
constants: p.r.f. 0.33Hz; pulse width 250000us;receiver bandwidth
10-50Hz.
Doppler effect from relative target motion was in excess of the desired
receiver bandwidth, necessitating controlled offsetting of receiver and
transmitter frequencies. Earlier work on moving target detection had
developed
both the capability and much equipment to provide the necessary
precision
frequency management; still earlier work on the Army's
SCR-270/271 search radars had evolved high pulse energy
and effective antenna array capabilities which could be gathered
together
to produce a set which could theoretically perform the feat with an
encouraging
decibel margin.
The system was
rapidly
assembled as planned, (see Figs. 37.7., 37.8., 37.9. and 37.10.), and
successfully
demon-strated [10] .

Click on image for replacement
large view of Block diagram of moon radar
Please note this is the same
diagram as Fig 37.3 - this is a publishers error.
Fig. 37.7 Block diagram of moon radar

Fig. 37.8 Moon radar site at Evans Signal Laboratory at Belmar, NJ
Fig.37.7 shows
the
block diagram of the moon radar. A bandwidth of 50Hz was selected
rather
than an optimum figure of under lOHz; the slight loss of visibility was
balanced by less stringent tuning requirements and possible additional
frequency shift or spreading resulting from the libration of the moon.
It should be noted that a portion of the receiver was obtained from an
experimental f.m. radar set which had been built for the Army Signal
Corps
by Major Armstrong. (The f.m. radar was similar in principle to
aircraft
radio altimeters using sawtooth frequency modulation.)
Fig. 37.9 Moon radar apparatus room with oscilloscope in wooden box |
Fig. 37.10 SCR-271 radar transmitter oscillator neutralised for use as high power amplifier |

Fig. 37.11 Oscilloscope display; a very widely
published
oscillogram
Page updated August 31,
2007
page created August 30, 2001
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