14 History Update
(3) turned on, (4) manned, and most importantly (5) heeded.
5
The probability of all those events
occurring was infi nitesimally small in the 1920s. For example, the better idea optical rangefi nder
had not yet been installed on any of those destroyers. But the potential was there—just not
appreciated for either maritime or military use.
As a result, those rejections ended all radar work for the next 18 years. That, in fi nal retrospect,
was the major tragedy of Hülsmeyer’s work: it was forgotten. There was no documentation of his
successful experiments in technical journals—just a few newspaper articles and obscure patents
buried in the fi les. So his legacy was lost to the engineering community, which was then forced to
start over with new and, as it turned out, quite different approaches.
This radar effect was rediscovered by A. H. Taylor and L. C. Young in 1922 when they were
carrying out 60 MHz propagation experiments using a superheterodyne receiver and a 50-W
transmitter amplitude-modulated at 500 Hz at the U.S. Navy Aircraft Laboratory, Anacostia,
DC. They fi rst detected bistatic refl ections from buildings, trees, and other stationary objects and
then a wooden steamer traveling down the Potomac River, which cut the beam in what is now
known as the forward-scatter mode [2, 8]. Again and likely for similar reasons such as no range
measurements, the concept was rejected by the U.S. Navy.
Then in the next 15 years both this forward-scatter effect and the doppler beat frequency
generated between the direct path signal and echoes from moving targets were observed by many
engineers and scientists conducting RF (radio frequency) propagation experiments. Both effects
could be observed together, as shown in Figure 2–5.
These experiments used new, commercial radio transmitters or similar experimental equipment
operating between 30 and 80 MHz.
6
Table 2–1 summarizes these events.
7
5 On December 7, 1941, an SCR-270 air surveillance radar at Pearl Harbor was installed, working, turned on, and
manned. But its data was not heeded.
6 An exception is the 1935 U.K. experiment, which exploited the 6-MHz BBC transmitter station at Daventry.
7 There is a sketchy report [10] about A. S. Popov detecting the Russian warship Lieutenant Il’in when it crossed a radio
communication link between two other Russian ships Europe and Africa on the Baltic Sea in 1897. The report then
credited him with discovering radiolocation—yet another father of radar. (Such claims lead Lamont Blake, nominated
by this author as father of the defi nitive radar range equation, to conclude that radar was one of those bastard
inventions: one mother, many fathers.) Unfortunately the Popov et al.’s 1945 report (in Russian) is not accessible.
Since nothing further appears to have been accomplished or published, we shall let it be.
E
(F)
(F')
R
l'avion
s'approche
l'avion
coupela
base
l'avion
s'eloigne
⋅
Figure 2–5 1937 drawing by Pierre David, showing an aircraft approaching, crossing, and then departing his
electromagnetic barrier [9]. (F) is the barrier, also called the fence or baseline. The doppler beat
frequency decreases during the approach, is zero during the crossing, and increases during the
departure. The increase in amplitude is the forward-scatter radar cross-section enhancement. (Pierre
David, Le Radar © PUF, coll “Que sais-je?” No. 381, 1969.)