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Project Cyclops, A Design... - Department of Earth and Planetary ...

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systemas for the IF systemitself.For a thous<strong>and</strong><br />

element 10-km-diameter array this would be about 5000<br />

to 7000 miles <strong>of</strong> cable. Clearly, the use <strong>of</strong> IF cable for<br />

all the delay would be cumbersome <strong>and</strong> costly.<br />

Nevertheless, it might be worth considering making<br />

all the IF cables in the IF distribution system the same<br />

length as the longest cable. This would add about 50%<br />

more IF cable <strong>and</strong>, using the equalization scheme<br />

proposed, would require no more repeaters. The additional<br />

cost would average about $5000 per line for the<br />

lO-km array, which may not be much greater than the<br />

cost <strong>of</strong> an electronic delay unit. The extra IF cable could<br />

be accommodated by running it out a side tunnel as far<br />

as necessary <strong>and</strong> then back to the antenna involved. We<br />

would then have an array already phased <strong>and</strong> stabilized<br />

for looking at the zenith <strong>and</strong> would need only to add the<br />

variable delay to tilt the delay plane.<br />

Acoustic surface wave delay lines appear to be the<br />

best broadb<strong>and</strong> delay devices available at this time. In<br />

these devices, a thin film interdigital electrode structure<br />

is used to launch a Rayliegh or Love type surface wave<br />

on a piezoelectric crystal substrate such as quartz or<br />

lithium niobate. A similar electrode structure detects the<br />

passage <strong>of</strong> the wave at the other end or at an<br />

intermediate point. The surface waves propagate with<br />

essentially no dispersion <strong>and</strong> with very little loss<br />

(_ l dB//Jsec). The loss, b<strong>and</strong>width, <strong>and</strong> dispersion problems<br />

occur in the transducers (electrode structures) used<br />

to couple tile electrical signals into <strong>and</strong> out <strong>of</strong> the crystal.<br />

A good survey <strong>of</strong> acoustic surface wave techniques is<br />

given by R.N. White in the August 1970 Proceedings <strong>of</strong><br />

the IEEE.<br />

Lithium niobate lines appear most attractive at this<br />

time. Some <strong>of</strong> the properties obtainable with this<br />

material are listed in Table 10-3.<br />

TABLE 10-3<br />

be lengthened<br />

by an amount<br />

a<br />

t_ = v(r_ - c) (1 --a ) (21)<br />

thereby filling in the basic delay cone in Figure 10-10 to<br />

a new cone (shown dotted) having its apex a/c below the<br />

delay r_. The total delay that now must be added by the<br />

delay system to achieve full steerability is 2a/c <strong>and</strong> is the<br />

same for each IF line. Although full use will never be<br />

made <strong>of</strong> the variability <strong>of</strong> central delay units, several<br />

advantages including interchangeability accrue from having<br />

all units<br />

alike.<br />

It is proposed that the delay system associated with<br />

each line consist <strong>of</strong> individual delay units connected in<br />

t<strong>and</strong>em, each unit having a delay<br />

r k = ¢o + 2k nsec (22)<br />

when switched in, <strong>and</strong> a delay ro when switched out.<br />

For a lO-km array, k ranges from -2 to +14. The delay<br />

required in any line (in units <strong>of</strong> 250 picoseconds) is then<br />

expressed as a 17-digit binary number <strong>and</strong> the delay<br />

units are switched in or out if the digit they represent is<br />

a 0 or 1 respectively.<br />

t<br />

r<br />

COMPUTER<br />

CONTROL<br />

Velocity 3.45X 10s cm/sec<br />

Temperature coefficient 85 ppm/°C<br />

Insertion loss 10- 35 dB<br />

Fractional b<strong>and</strong>width 75%<br />

Center frequency 0.1 to 1 GHz<br />

Delay precision

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