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Radar System Engineering

Radar System Engineering

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134 C-W RADAR SYSTEMS [SEC. 56<br />

transmitter, and the doppler frequency. The d-c component is removed<br />

by passage through a transformer, or otherwise, and the doppler frequency<br />

is used to actuate the indicator.<br />

An incidental but important advantage of this modification is that<br />

it enables the use of a suitable and easily adjustable crystal current.<br />

These modifications are introduced in a manner indicated in Fig. 5.5<br />

which shows a block diagram of the system. Everything is straightforward,<br />

except for the local-oscillator power which is obtained by<br />

modulating the transmitter and selecting a suitable sideband by means<br />

of a bandpass filter. This insures a constant intermediate frequency and<br />

avoids any tuning problems. Frequency-doubling is employed in the<br />

modulator to avoid difficulties in keeping leakage from the crystal<br />

oscillator out of the i-f amplifier.<br />

Transmitting<br />

antenna<br />

Receiving<br />

antenna<br />

3000 Me/see<br />

I<br />

Oscillator<br />

1<br />

30 Mclsec<br />

i.f<br />

amplifler<br />

2nd<br />

detector<br />

FIG. 5.5.—Block diagram of simple doppler-type radar system.<br />

Design Procedure. —Having blocked out a proposed system, we may<br />

now sketch the design procedure that fixed the various apparatus constants<br />

and dimensions.<br />

Design commenced with the choice of an indicator. A voltmeter<br />

will certainly work, but experience has shown that a speaker or pair of<br />

earphones, in conjunction with the operator’s hearing sense, is much<br />

more effective provided the frequencies to be detected lie in the range<br />

between a few hundred and a few thousand cycles per second. 1 Within<br />

this range, the ear easily recognizes pure tones in the presence of hiss<br />

even when the pure note is much too weak to be seen on an oscillograph.<br />

This phenomenon is analogous to the averaging performed by the eye<br />

when looking at an A-scope, as discussed in Chap. 2. Rough experiments<br />

show that the ear will detect a pure tone in the presence of hiss<br />

when the tone is stronger than the noise in a 200-cps bandwidth. If<br />

the ear can do this over the range 200 to 3000 cps, then by using the<br />

I A detailed study of the aural detection problem can be found in RRL Report<br />

No. 411-86, May 5, 1944,

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