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Radar System Engineering

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378 THE MAGNETRON AND THE PULSER [SEC. 10.10<br />

the same material. The tube is filled to a pressure of a little less than one<br />

atmosphere with a mixture of 75 per cent hydrogen and 25 per cent argon.<br />

Two or three tubes are used in series, with a voltage divider across them<br />

to ensure that the network voltage is divided equally among all the gaps<br />

before the pulse takes place. Triggering is accomplished as shown in<br />

Fig. 10.39 by depressing or raising quickly the voltage of the two middle<br />

electrodes. This breaks down one of the gaps and throws full voltage<br />

across the second gap. The overvolted second gap thereupon also<br />

breaks down, forming a low-impedance path between points A and A‘.<br />

These switches are efficient and are quite satisfactory in use. Their chief<br />

limitations are in the allowable pulse repetition frequency (about 2000<br />

DDSmaximum) . .<br />

and in obtainable precision of pulse timing. This type<br />

of switch can handle several megawatts,<br />

and should be useful in applications<br />

that do not require great<br />

flexibility or accuracy of firing.<br />

A particularly successful version<br />

of the series-gap switch is the Bell<br />

R T e 1e p h o n e Laboratories’ 1B42,<br />

which substitutes a mercury-saturated<br />

iron “sponge” for the solid<br />

aluminum cathode of the 1B22. By<br />

\<br />

coup<br />

\!<br />

-1<br />

Trigger input<br />

*<br />

II<br />

/<br />

R<br />

FIG. 10.39.—Series gaps.<br />

\<br />

Voltage<br />

dwider<br />

(r<br />

‘t<br />

Triggerinput<br />

FIG.<br />

10 40. —Trigatron.<br />

using an atmosphere of relativel y high-pressure hydrogen, the temperature<br />

variation of mercury vapor pressure is made unimportant. Since the<br />

ordinary series. gap is limited in operation by pitting and spike growth,<br />

the mercury cathode provides better operation over a wide range of

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