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Radar System Engineering

Radar System Engineering

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R-F<br />

CHAPTER 11<br />

COMPONENTS<br />

BY A. E. WHITFORD<br />

11.1. The R-f Transmission Problem.—In the block diagram of a<br />

basic radar system shown in Fig. 14, the parts shown as heavy double<br />

lines transmit the radio-frequency (r-f) energy from the magnetron to the<br />

antenna, and carry the faint echo signals into the T-branch where the<br />

receiving apparatus is located. For the types of radar treated in this<br />

book this function is performed by coaxial lines and waveguides. A<br />

considerable body of theory and a new set of techniques have grown up<br />

around this class of transmission circuits. The essential new feature is,<br />

of course, that the wavelength is of the same order as the physical size of<br />

the circuit elements; the length of the line may be many wavelengths.<br />

Although space permits only a limited treatment here,l sufficient introduction<br />

will be given to show the general approach, and to make understandable<br />

some of the reasons for current practices in microwave radar.<br />

Standing Waves.—When a voltage is suddenly applied to the input<br />

terminals of a long and uniform transmission line, ‘the current which flows<br />

in the initial interval, before reflections from the far end arrive to confuse<br />

the situation, is determined by the property of the line known as its<br />

“characteristic impedance. ” The characteristic impedance, ZO, is a<br />

function of the geometry of the conductors and insulators of the line, and<br />

for good conductors and low-loss dielectrics is almost purely resistive.<br />

For a concentric line, neglecting losses,<br />

where k is the dielectric constant of the material in the annular space<br />

between the conductors, r, is the inner radius of the outer conductor, and<br />

TI is the outside<br />

radius of the inner conductor.<br />

A uniform line terminated at any point in its characteristic impedance<br />

behaves as if the line were infinitely long; there is no reflection. Power<br />

introduced at the input terminals disappears into the termination with<br />

small losses in the line. However, any discontinuous change along the<br />

1 Xfl-... -... --2.2 .-... —.-. --- L.f... –.l :- _. L-- L__,.. _.<br />

.)1”, .L:. --:- .-.. -;. 11..<br />

c CALC,,Utl, l,,edLII,e,, b Uii,, lJ~,UU,, U Ill“1,,,~~ ““”KSUlLILIS SSlltX) ~h~CL-l?llly<br />

(1)<br />

vol. 9; (z) Microwave hpk%rs,<br />

Micrwave Transmission ~01. 14;<br />

Circuits,<br />

(3) Wavegwid. Handbook, Vol. 10; (4) Principles of Microwave Circuik?, Vol. 8.<br />

391

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