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Radar System Engineering

Radar System Engineering

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CHAPTER 5<br />

C-W RADAR SYSTEMS<br />

BY W. W. HANSEN<br />

6.1. General Considerations. -We shall begin with a discussion that<br />

is fundamentally useful in understanding what follows, but has as its<br />

immediate object a definition of the scope of this chapter more precise<br />

than is given by the chapter title.<br />

The simplest conceivable radar system consists of a source of r-f<br />

power, an antenna, and a scattering object or target. The antenna<br />

emits waves with time factor eh~, which, on striking the target at a<br />

distance r, are reflected and returned to the antenna, where their time<br />

factor will be e’(”’-’kr) with k = 27r/A. The returned waves will be<br />

reduced in amplitude by a factor a which depends on the target and<br />

various geometrical factors, as discussed in Chaps. 2 and 3.<br />

This returned wave will give rise to currents and voltages in the<br />

antenna, which add to those produced by the power source and so give<br />

rise to a voltage-current ratio, or impedance, which is changed from the<br />

value existing ~vhen no target is present.<br />

In principle, this impedance, or some similar quantity, might be<br />

measured on an absolute scale, and the deviations from the normal, or<br />

no-targrt value, ascribed to the presence of a target.<br />

Practically, this procedure is impossible because the returned signals<br />

are often 10–9 times as large, on a voltage basis, as the outgoing signals,<br />

with the result that the variations in impedance might be of the order<br />

of a part in 10’. Such variations can hardly be measured in the laboratory<br />

at low frequencies, let alone in the field and at microwave frequencies.<br />

It is therefore necessary to cause the returned signals to vary in some<br />

manner so that the variation can be measured, rather than to attempt<br />

such an absolute measurement as that described above.<br />

This desired variation is caused by a modulation process of some sort.<br />

The word “modulation” is used herein a general sense to include changes<br />

induced by the target as well as changes in signal introduced at the<br />

transmitter. All possible radar systems can then be classified by describing<br />

the type of modulation and the use made of the resulting information.<br />

As a specific example of these general remarks, let us take a very<br />

simple radar system which consists, as shown in Fig. 5.1, of an r-f power<br />

source, an antenna, a rectifier, a high-pass filter, an indicator, and a<br />

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