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Radar System Engineering

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SEC. 10.9] THE HARD-TUBE P ULSER 369<br />

care in processing and use it is possible, nevertheless, to arrive at a satisfactory<br />

and highly flexible pulser desigu using the oxide-cathode pulse<br />

tube up to 20 kv. Where extreme reliability and relative immunity to<br />

overload are required, the designer will prefer the thoriated-tungsten<br />

cathode switch tube in spite of its greater cathode power requirements.<br />

Switching tubes of the oxide-cathode variety usually can be counted upon<br />

to emit 300 to 600 ma/watt of heating power while the emission of the<br />

best thonated-tungsten cathodes is only about 100 ma/watt.<br />

The oxide-cathode tube is limited in power output by the onset of<br />

grid emission. It is impossible to prevent thermionically active cathode<br />

material from contaminating the grid structure. Great care must be<br />

taken, therefore, to cool the grid by fins, heavy rods, and other means, for<br />

it can emit a few milliamperes even at a sub-visible temperature. A few<br />

milliamperes may sound small in comparison with several amperes pulse<br />

current, but a few milliamperes flowing all the time can cause serious<br />

heating of the anode and screen, which are at relatively high potentials.<br />

Usually the result is a runaway condition in which grid control is lost.<br />

The most successful oxide-cathode high-power switch tube is the 715B<br />

developed at Bell Telephone Laboratories. The 715B has a gold-clad<br />

grid which poisons and “absorbs” act ive material, thereby lowering its<br />

efficiency as a thermionic emitter.<br />

TABLE 1O.4.—TYE’ICALOIV:RATING cmm~c’rmus’mcs<br />

Tube<br />

type<br />

3D21<br />

3E2!l<br />

715B<br />

5D21<br />

304TH<br />

6C21<br />

6D21<br />

527<br />

Cathode<br />

type<br />

Oxide<br />

Oxide<br />

Oxide<br />

Oxide<br />

Th-W<br />

Th-W<br />

Th-W<br />

Th-VV<br />

C’athode<br />

plate<br />

Max.<br />

>owei-, voltage,<br />

watts kv<br />

10<br />

14<br />

56<br />

56<br />

125<br />

140<br />

150<br />

770<br />

Emiscur-<br />

sion,<br />

rent, amp/<br />

amp watt,<br />

3.5 5 0.5<br />

5.0 8 0.57<br />

15.0 15 0.27<br />

20.0 15 0.27<br />

15.0 6 0.05<br />

30.0 15 0.11<br />

37.5 15 0.10<br />

30.0IPulse<br />

60 0.08<br />

cutoff<br />

grid<br />

vOltage*<br />

– 70<br />

– 100<br />

– 500<br />

– 500<br />

– 900<br />

–1000<br />

– 500<br />

– 1200<br />

plate<br />

drop,<br />

Volts<br />

400<br />

600<br />

1500<br />

1500<br />

2000<br />

1500<br />

2000<br />

1500<br />

9, creen<br />

voltage<br />

800<br />

Soo<br />

1200<br />

1200<br />

2000<br />

‘ositive<br />

grid<br />

drive,<br />

volts<br />

150<br />

150<br />

200<br />

200<br />

200<br />

1500<br />

1500<br />

1500<br />

* 0,2-ma cutoff.<br />

A good output pulse tube must possess a sharp grid cutoff. For<br />

efficient operation, the plate current must be one milliampere or less when<br />

the grid is biased to some reasonable value. Because the anode is at very<br />

high voltage between pulses, any “leakage current” delivers excessive<br />

power to the anode. As an example, consider a pulse tube normally<br />

giving 20-amp pulses with an anode drop of 3 kv at a duty ratio of ~m.<br />

Such a tube will display a peak power anode loss of 60”kw, but an average<br />

power loss of only 60 watts. If the leakage current at “ cutoff” amounts

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