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

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PAGE BLANK NOT<br />

APPENDIX<br />

H<br />

POLARIZATION<br />

CONSIDERATIONS<br />

The sensitivity <strong>of</strong> the <strong>Cyclops</strong> array depends on the<br />

alignment <strong>of</strong> the polarization <strong>of</strong> the transmitter with the<br />

polarization <strong>of</strong> the receiver. The polarization <strong>of</strong> the<br />

transmitter is unknown, however, <strong>and</strong> to avoid loss <strong>of</strong><br />

sensitivity, steps must be taken to ensure that the<br />

receiver receives most <strong>of</strong> the incident polarization. The<br />

discussion is facilitated if the Poincar_ sphere (ref. l)<br />

shown in Figure H-I is used. Any arbitrary polarization<br />

is described by the radius vector from the origin to a<br />

point on the sphere. If the vector representing the<br />

incident polarization makes an angle 0 with the vector<br />

representing the receiver polarization, the received field<br />

strength is:<br />

If horizontally <strong>and</strong> vertically polarized receivers are<br />

provided, then the angle 0 will be no greater than n/2<br />

from one or the other <strong>of</strong> the receivers. The maximum<br />

loss would then be 3 dB. An expected value <strong>of</strong> loss may<br />

also be calculated if the incident polarization is assumed<br />

to be r<strong>and</strong>omly distributed. This number is 1.3 dB.<br />

Suppose now that the horizontal <strong>and</strong> vertical channels,<br />

designated by H <strong>and</strong> V, are received, <strong>and</strong> that after<br />

amplification the processing scheme shown in Figure<br />

H-2a is used. This processing results in an equal spacing<br />

<strong>of</strong> the receivers around the equator <strong>of</strong> the Poincard<br />

sphere. Again the maximum loss is 3 dB but the<br />

expected<br />

value <strong>of</strong> loss is now 0.7 dB.<br />

E<br />

= E0cos-<br />

0<br />

2<br />

Vo<br />

v+___H_<br />

LEFT CIRCULAR<br />

POLARIZATION<br />

I<br />

(0) HO<br />

,°",L.C,vo<br />

H<br />

o V {LHC)<br />

("V')<br />

_V+H<br />

V-H<br />

( "H" )<br />

(RH)<br />

Ho<br />

o H (RHC)<br />

°uA_<br />

v+jH<br />

v-j_____H<br />

.v/r _ 1135"1<br />

qC5<br />

I<br />

RIGHT CIRCULAR<br />

POLARIZATION<br />

Figure H-I. The Poincard sphere.<br />

l<br />

Figure H-2. Polarization conversion.<br />

To carry this operation to its logical conclusion,<br />

receivers would be placed at the cardinal points <strong>of</strong> the<br />

Poincard sphere. The processing scheme shown in Figure<br />

207

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