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TELE-TECH & - AmericanRadioHistory.Com

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F<br />

A<br />

Optical Radar<br />

EIMAC Vacuum Switches<br />

for high- voltage switching<br />

in severe environments.<br />

In explosive atmospheres and high altitude<br />

airborne conditions, Eimac vacuum switches<br />

operate reliably and safely.<br />

Used extensively in air and ground<br />

mobile applications, the small size and fast<br />

closing time of Eimac vacuum switches<br />

make them ideal for antenna changeover.<br />

They handle RF peak potentials up to<br />

20kv in this service, and 1.5 amps at 5kv<br />

in DC switching service.<br />

Eimac single pole double throw vacuum<br />

switches are available in four types,<br />

including one for pulse service.<br />

If you have a switching problem,<br />

write our Application Engineering<br />

Department for further information.<br />

EITEL - McCULLOUGH, INC.<br />

S A N B R U N O C A L I<br />

O R N I<br />

The World's Largest Manufacturer of Transmitting Tubes<br />

(Continued from page 191)<br />

ly by the "pick -up" device on the<br />

radar indicator.<br />

B. Noise. The 1P21 photo- multiplier<br />

tube is a natural noise generator.<br />

The white noise (or grass)<br />

can be varied in intensity by varying<br />

the level of ambient light. Almost<br />

any signal -to -noise ratio desired<br />

can be achieved.<br />

C. Target Size. Since the size of<br />

the target image on the radar indicator<br />

resulting from the signals it<br />

receives from the "pick -up" device<br />

will be proportional to the size of<br />

the light spot, larger targets are<br />

simulated by larger spots.<br />

D. Simulation of Altitude and<br />

IFF. Future plans involve simulation<br />

of altitude and IFF in addition<br />

to range and azimuth by means of<br />

modulation of the target lights.<br />

This is still in the experimental<br />

stage however.<br />

Nonlinear Relation Between<br />

Range and Time<br />

The time delay between the sending<br />

and receiving of a pulse from a<br />

radar antenna to a target is directly<br />

proportional to the range of the<br />

target. Unfortunately this linear<br />

relation does not exist between<br />

time and range in the present simulated<br />

system. As has been pointed<br />

out previously in the simulated system<br />

R =h tan, ì. =h tan 20.)t. Now<br />

for small angles (). = 20 °) the approximation<br />

tan A = ), is quite<br />

sufficiently accurate, and if the<br />

"pick-up" device is removed sufficiently<br />

far from the screen no problem<br />

arises. However, if space is<br />

limited and /or optical problems become<br />

serious at great distances,<br />

other solutions must be found.<br />

One simple solution would be to<br />

use a non -linear scale on the face of<br />

the radar screen. However, this<br />

would introduce a degree of unreal -<br />

ism. Several schemes are now under<br />

consideration. One method involves<br />

producing a sweep voltage<br />

shaped like the tangent curve instead<br />

of the conventional sawtooth<br />

curve. Different methods for generating<br />

the tangent curve are now<br />

in the experimental stage but a<br />

few show good promise of success.<br />

192 For product information, use inquiry card on pages 209 -210. Tele-Tedi & ELECTRONIC INDUSTRIES June 1956

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