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Radar System Engineering

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SEC. 15.10] COMPONENTS DESIGN 607<br />

1. Azimuth angle of beams does not shift with a change in wavelength.<br />

2. Multiple beams from separate transmitter-receiver systems can be<br />

accurately set to the same azimuth angle. This property is very<br />

desirable if the system is to be equipped for work with radar<br />

beacons.<br />

3. Open mesh or a grid structure can be used for the reflector surface<br />

to reduce wind resistance. The linear-array system requires a<br />

solid surface for the reflector, since the comparatively high gain<br />

of the linear-array feed will give an objectionable back lobe<br />

through<br />

mesh or gridwork.<br />

The ilfodulator.-Because of its simplicity and power-handling<br />

capacity, an a-c resonance-charging line-type modulator using a rotary<br />

FIG. 15 6.—Modulator of high-power ground radar.<br />

gap as a switching device was chosen. The rotary gap is mounted<br />

directly on the shaft of a 400-cps alternator, which excites the network<br />

and is properly phased by mechanical adjustment (Fig. 15.6). This<br />

modulator choice was important in fixing the value of the PRF, but,<br />

as already remarked, the desirable value lies in the neighborhood of<br />

400 pps in any event.<br />

Separate transmitters are used on the upper-beam and the lowerbeam<br />

systems; both are driven, through pulse transformers, from a<br />

single modulator. The modulator is rated at 3000 kw.<br />

R-j Components.—The high pulse powers used in this system demand<br />

the use of waveguide for the r-f system. Each magnetron operates in a<br />

field of 2S00 gauss at 28 kv pulse voltage, dra\ving a current of about 30<br />

amp and putting 750 k\v of r-f power into the line at about 65 per cent<br />

efficiency.<br />

Crystal protection at this high power level is difficult, and a scheme<br />

of “repulsing” the TR tube is used. Part of the 8-kv modulator pulse

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