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Radar System Engineering

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SEC. 10.10] LINE-TYPE PULSERS 377<br />

In large radar equipments, it is often desirable to separate pulser and<br />

r-f units by considerable dktances. The pulse transmission cable necessary<br />

in such cases has been standardized at an impedance level of 50<br />

ohms. Many pulse networks designed for high-power radar have an<br />

impedanceof 500hmsin order toavoid the use ofa matching pulsetransformer<br />

between the network and the cable. As a result, many of the<br />

more desirable switching devices have been designed to give maximum<br />

power output when used with a 50-ohm network.<br />

TABLE10.6.—PULSE-FOEWNG hTETWOItKCH.*RACTEFUSTICS<br />

N’etwork (Fig. 10.38)<br />

Pulse length, ~ec<br />

PRF, 13pS<br />

Power<br />

h’o. 1<br />

0.8<br />

2,2<br />

840<br />

420<br />

25 kw<br />

25 kw<br />

No. 2<br />

0 25<br />

05<br />

2.6<br />

52<br />

1600<br />

800<br />

4oil<br />

200<br />

250 kw<br />

250 kw<br />

250 kw<br />

250 kw<br />

No. 3<br />

1<br />

1000<br />

250 kw<br />

No. 4<br />

1<br />

800<br />

3 3fw-<br />

An important design consideration in pulse network applications is<br />

the average power to be handled. A pulse network designed to have<br />

adequate life at one pulse rate would overheat and perhaps be ruined by<br />

operation at a higher repetition frequency. Since overheating is a function<br />

of both applied voltage and repetition rate, little flexibility remains<br />

in a line-type pulser designed to achieve maximum economy of weight,<br />

space, and power. Provision can be made for shortening pulse length<br />

by bringing out taps on the pulse line. However, this is rather difficult<br />

at high power, because of the problem of designing suitable line switches.<br />

The Sw”tch.—The possible advantages of the line-type pulser greatly<br />

stimulated the design of low-impedance spark switches and thyratrons,<br />

since it became possible to secure flat-topped pulses without the necessity<br />

of opening the switch. Rotary spark gaps, ‘‘ trigatrons,” series gaps,<br />

hydrogen thyratrons, and mercury thyratrons have all been used as network<br />

switching devices. Each has its field of application. Each switch<br />

is limited in one or more of the following respects: (1) poor precision of<br />

firing, (2) low maximum pulse rate, (3) short life on long pulses, (4) narrow<br />

operating range of voltage, (5) occasional erratic firing, (6) inefficient<br />

cathode, and (7) unnecessary complication. The ideal switch has not<br />

yet been designed.<br />

Figure 10.39 shows schematically the simple “series gap” s\vitch.<br />

The Western Electric’ 1B22 is a good example of this class of switch; it<br />

consists of a cathode cylinder of aluminum surrounding an anode rod of

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