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Radar System Engineering

Radar System Engineering

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SEC.11.12] ILL US1’IiA TI VE EXA hlI’LES OF R-F IIEADS 431<br />

of one oft he radars. Figure 11“31 shows the interior detail of one of these<br />

compartments; in the other, the items are the same but are mounted the<br />

other end up. The pulse from the modulator comes in through the pulse<br />

connector on the end of the case. For the long-range search set the<br />

power from the modulator is about 2 Mw, or about 10 kv on the 50-ohm<br />

cable. This power goes in parallel to the primary of the pulse transformer<br />

and to a despiking network consisting of a 50-ohm resistor and a 400-~pf<br />

condenser in series to ground. The network provides a transient load<br />

for the modulator while the voltage is rising but before the magnetron<br />

starts to draw current.<br />

On the long-range search set, a 4J32 magnetron furnishes 0.8 Mw of<br />

r-f power. The pulse length is 1 psec and the repetition rate is 39o pps.<br />

Since the peak voltage at the cathode is about 28 kv, good clearance must<br />

be maintained. The magnetron output is in 1~-in. OD coaxial line, but<br />

an immediate transition is made to standard waveguide l+ by 3 in. with<br />

0.080-in. wall. Since both the coaxial line and waveguide are operating<br />

not very far from the voltage-breakdown point, a specially tapered “doorknob”<br />

transition is necessary. A small air gap in the choke-flange<br />

coupling between the transition section and the waveguide outJet absorbs<br />

the tolerances in the magnetron mounting. The whole magnetron highvoltage<br />

compartment is tightly closed in operation. The small upper<br />

compartment is mainly taken up with the fluted case of the pulse transformer.<br />

The antenna waveguide of the other radar goes through in<br />

front and the directional coupler is put in this convenient place.<br />

In the central section are the two duplexer sections and the two<br />

receivers. The duplexer section for the search radar stretches across the<br />

lower part of the case. Nearest the magnetron is the AFC attenuator<br />

and mixer. The mixer is of the type shown in Fig. 11.25, Sec. 11.8. One<br />

coaxial cable brings r-f power from the local oscillator, which is mounted<br />

in a well-shielded compartment in the receiver box. The other carries<br />

the i-f signal to the AFC discriminator and control circuit in the same box.<br />

Next along the guide and on the opposite side are the two ATIt tubes,<br />

of the untuned 1ow-Q type, spaced one half of a guide wavelength apart.<br />

This gives a broadband characteristic. 1 The resonant windows are<br />

made a part of the broad face of the waveguide. A half wavelength<br />

farther down the guide, and on the same side as the AFC attenuator, is<br />

found the duplexer T. The TR cavity is iris-coupled, both on the input<br />

side from the end of the waveguide and on the output to a coaxial mixer<br />

which is otherwise the same as the AFC mixer. As in the AFC case, i-f<br />

cables connect the mixer with the local oscillator and the proper parts<br />

of the receiver.<br />

The last part of the duplexer section is an r-f switch used in testing<br />

1Microwave Duplaxrs, Vol. 14.

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