Project Cyclops, A Design... - Department of Earth and Planetary ...
Project Cyclops, A Design... - Department of Earth and Planetary ...
Project Cyclops, A Design... - Department of Earth and Planetary ...
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We conclude that none <strong>of</strong> the above alternatives is<br />
attractive, <strong>and</strong> the best way to avoid chromatic aberration<br />
in a delay line imager is to image at the original<br />
b<strong>and</strong>, or near it.<br />
If we wish to have m image points <strong>and</strong> if the n<br />
antennas in our array were scattered at r<strong>and</strong>om points,<br />
we would require mn cables to make all the connections<br />
in the imager. For n = 1000 <strong>and</strong> m = 4000 we need 4<br />
million cables. However, if both the antennas <strong>and</strong> the<br />
image points are in regular lattice patterns, this number<br />
can be reduced by performing the transformation in two<br />
steps as allowed by equation (38).<br />
The simplest case is that <strong>of</strong> a square antenna array <strong>of</strong><br />
n elements arranged in _ rows <strong>and</strong> colunms, <strong>and</strong> a<br />
square image field <strong>of</strong> m image points arranged in V_<br />
rows <strong>and</strong> columns. Between the signal <strong>and</strong> image plane<br />
we place an intermediate plane having _ junction<br />
points. If we transform first by rows <strong>and</strong> then by<br />
columns, the intermediate plane will have V_" rows <strong>and</strong><br />
V_ columns. Each <strong>of</strong> the n signal plane points connects<br />
to the V_" intermediate plane points on the same row,<br />
while each <strong>of</strong> the n image plane points connects to the<br />
intermediate plane points in the same column, for a<br />
total <strong>of</strong><br />
columns. There will therefore be<br />
junction points <strong>and</strong><br />
connections.<br />
1+2v - -3<br />
n]- 3<br />
(60)<br />
N = n 1+2 + m (61)<br />
3<br />
The values <strong>of</strong> n] <strong>and</strong> N for the various configurations<br />
with n = 1000 <strong>and</strong> m = 4000 are shown in Table 11-2<br />
TABLE 11-2<br />
Antenna Array: Junctions: Connections:<br />
Shape Lattice Number Ratio Number Ratio<br />
Square Square 2000 1.00 190,000 1.00<br />
Circular Square 2257 1.13 206,000 1.09<br />
Circular Hexagonal 3246 1.62 238,000 1.25<br />
N = nv_ + mVrff" (57)<br />
interconnections.<br />
If the antenna array is circular with a square lattice<br />
there will be x/r_"/lr rows <strong>and</strong> therefore<br />
= (58)<br />
,/o • • °<br />
* o "/I I. • I I<br />
•': 2:-X/"<br />
• x<br />
\,<br />
SIGNAL PLANE<br />
junction points in the intermediate plane. We then find<br />
ROWS AND COLUMNS<br />
/<br />
/<br />
(59)<br />
INTERMEDIATE<br />
PLANE<br />
•v_ ROWS, _ COLUMNS<br />
The connections are illustrated in Figure 11-17 for the<br />
top row <strong>and</strong> left-h<strong>and</strong> column.<br />
If we use hexagonal lattices, the image plane lattice is<br />
rotated 90 ° with respect to the signal plane lattice.<br />
Assuming the antenna array is circular <strong>and</strong> that in the<br />
image plane one <strong>of</strong> the three sets <strong>of</strong> rows, characteristic<br />
<strong>of</strong> a hexagonal lattice, is horizontal, there will be<br />
_x/'3 rows. The image field will be hexagonal in<br />
outline with two opposite sides <strong>of</strong> the hexagon forming<br />
the top <strong>and</strong> bottom, <strong>and</strong> will contain (i + 2_)/3<br />
The cost<br />
where<br />
Figure 11-17. Wild Cat's cradle.<br />
<strong>of</strong> a delay line imager is<br />
C = "ysn+ "y/n/+"yim + VcN (62)<br />
146