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Radar System Engineering

Radar System Engineering

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SEC. 3.11] EXTENDED SC’RFACE 1’ARGETS 87<br />

We can generalize this formula t o the case of an extended surface target,<br />

if we replace a by an expression whose fmm will be deduced though<br />

statistical arguments similar to those used in Sec. 3.10. As long as the<br />

relative positions of the objects in the target layer are random,l we add<br />

the power received from each object in the area to find the average<br />

\’-.<br />

/<br />

rh<br />

,,<br />

II<br />

L<br />

I \<br />

--&l-<br />

FIG.3.15.—Theareacontributingto the instantaneouspowerreceivedfrom an extended<br />

surfacetargetis hmitedin rangeandazinluthhy theresolutionof theradarsystem.<br />

level of the probability distribution. The average signal S will thus be<br />

proportional to the area A, but it can also be expected to depend on<br />

the aspect angle 8, in a way which need not be specified here beyond<br />

l Specifically,we requirethat the wave trainsreceivedfrom the individual scattererswithinthe<br />

targetareashouldcombine in randomphase,which will be the case<br />

if the rangesI?i to the scatteringobjects are distributedwith a randomnessor deviation<br />

much greaterthan one wavelength,over a rangeintervalAR itselfmuch greater<br />

than one wavelength.

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