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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

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