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Radar System Engineering

Radar System Engineering

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442 THE RECEIVING SYSTEM—RADAR RECEIVERS [SEC. 12.4<br />

Another very important factor in radar receiver design is that of<br />

securing a good transient response. Reception of pulses about 1 ~secin<br />

length imposes severe requirements on the pass band of the amplifier.<br />

At the same time, the amplifier must be capable of amplifying pulses<br />

several hundred microseconds in length and yet be fully sensitive to a<br />

weak signal immediately following. It must recover immediately from a<br />

signal thousands of times stronger than the minimum discernible signal.<br />

Frequently special requirements are placed on the receiver. For<br />

example, it may be required that it respond to weak pulses even in the<br />

presence of a c-w signal of considerable strength. The problem of<br />

detecting a weak target echo in the presence of strong sea return is somewhat<br />

similar. Special circuits which go under the general title of “anticlutter<br />

circuits” are usually required in such cases.<br />

The unique requirements outlined in the foregoing three paragraphs<br />

have resulted in a receiver that is considerably different from anything<br />

previously existing. The design of i-f and video amplifiers to meet these<br />

requirements will be discussed in the following sections.<br />

12.4. I-f Ampliiier Design—In an ideal i-f amplifier, all the noise<br />

would originate in the generator connected to its input terminals-that is,<br />

the crystal that serves as converter in<br />

the usual radar receiver. In any practical<br />

amplifier there are additional<br />

sources of noise. Thermal noise from<br />

B+<br />

Fm. 12.4.—Pentodeinput circuit.<br />

resistances in the input circuit and shot<br />

noise due to the uneven flow of electrons<br />

to the plate of the first tube are<br />

the chief sources of excess noise, although<br />

later stages may contribute<br />

slightly. For this reason, care must<br />

be taken in the design and tuning of the network coupling the crystal to<br />

the first grid as well as in the choice of the operating conditions and type of<br />

the first tube.<br />

Figure 1264 shows a typical input circuit, with the primary tuned to<br />

resonate with the crystal and mixer capacity at the intermediate frequency,<br />

and with the secondary tuned to resonate with the input capacity<br />

of the tube and socket. The coils are usually fixed-tuned or “ slugtuned”<br />

1 in order to avoid any extra capacity. The only loading on the<br />

circuit is due to the crystal and the input resistance of the tube; thus,<br />

there are no additional resistances to contribute thermal noise. Thermal<br />

1The inductanceof a ‘1slug-tuned” coil is loweredby the effect of eddy currents<br />

inducedin a metallicrod (slug)insertedin one endof thecoil. The degreeof penetration,<br />

and thereforethe inductance,can be varied by turning the slug in a threaded<br />

support.

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