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Radar System Engineering

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CHAPTER 2<br />

THE lU.DAR EQUATION<br />

BY E. M.<br />

PURCELL<br />

The operation of a radar set depends on the detection of a weak<br />

signal returned from a distant reflecting object. The factors which<br />

control the strength of the signal so received are clearly of first importance<br />

in determining the maximum range of detection of a given target by a<br />

specified radar set. In Sees. 2.1 to 26 we shall formulate and examine<br />

the basic relation between these quantities, which is commonly known<br />

as the “radar equation. ” Specifically, we want to derive an expression<br />

for the peak radio-frequency signal power S, available at the terminals<br />

of the radar antenna, which will involve measurable properties of the<br />

transmitting and receiving antenna system, the transmission path<br />

through space, and the target itself. Now this relation will not suffice<br />

to fix the maximum range of detection unless the minimum power<br />

required for detection, Sk, is known. This important quantity S~ti we<br />

prefer to discuss separately, beginning in Sec. 2.7 below. It will be found<br />

to depend on many other factors, not all readily accessible to measurement,<br />

ranging from thermal noise in a resistor to the integrating property<br />

of the eye of the radar observer. Thus we choose to divide the problem<br />

into two parts, by a fictitious boundary, as it were, between the radar<br />

antenna and the rest of the set. The relations which we shall develop<br />

in Sees. 2.1 to 2.6 are wholly geometrical ones in the sense that the factors<br />

upon which the received power S depends are all lengths, apart from the<br />

transmitted power P, to which, of course, S is always proportional.<br />

THE RADAR EQUATION FOR FREE-SPACE PROPAGATION<br />

2.1. The Meaning of Free-space Propagation.-Fortunately, the<br />

quasi-optical nature of microwave propagation permits us to concentrate<br />

our attention at the outset on a very simple case, which we shall call<br />

“free-space propagation.” The circumstances implied would be realized<br />

exactly if radar set and target were isolated in unbounded empty space.<br />

They are realized well enough for practical purposes if the following<br />

conditions are fulfilled:<br />

1, No large obstacles intervene between antenna and target, along<br />

an optical line of sight.<br />

18

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