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Radar System Engineering

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SEC.5.8] F-M RANGE-MEASURING SYSTEM 145<br />

(7)<br />

‘I’his is of the nature of a maximum error and can be much reduced<br />

by averaging over a number of modulation cycles.<br />

Design Procedure. —Design of such an altimeter is begun by using<br />

the above equation, together with an allowable altitude error, to pick a<br />

suitable Af. In the present case Aj was chosen as 40 Xfc/see, which<br />

corresponds to ah = 6 ft, and so, because of averaging, to a rather smaller<br />

operational error.<br />

The mean transmitter frequency is now chosen. This must be<br />

fairly high in order to keep. the frequency variation from being an impossibly<br />

large fraction of the mean trequency. On the other hand there is no<br />

gain in very high frequencies and there may be some loss in intensity<br />

over such terrain as forests. These considerations, plus a consideration<br />

of the tubes available, led to the choice of a mean frequency of 440<br />

Me/see, which can be obtained from acorn tubes; the frequency modulation<br />

is accomplished mechanically.<br />

The modulation frequency is next chosen to give a convenient range<br />

of beat frequenciesf~, subject to the restriction that the time of a modulating<br />

cycle shall be long compared to the maximum signal transit time.<br />

A value of 120 cps was picked. This gives ~a = 8000 cps at an altitude of<br />

400 ft. A second range of O to 4000 ft is obtained by reducing Aj to<br />

4 Me/see.<br />

This completes the major specifications, except for the power. Practically<br />

speaking, power must be decided on the basis of experience,<br />

calculations of available power and thermal noise power being quite<br />

useless since, in practice, the limitation is not thermal noise but microphonics,<br />

etc. Thus if we consider the earth as a diffuse reflector }\-e<br />

easily find the received power is (1/2m) (A/r2) times the earth’s reflection<br />

coefficient and times the transmitted power. Even for very small<br />

transmitter powers and reflection coefficients, this power is large compared<br />

to thermal noise. On the basis of experience, then, it was decided that<br />

the 0.3 watt available from an acorn tube would be sufficient for altitudes<br />

up to 5000 ft, provided certain points of apparatus detail were correct,<br />

as explained below.<br />

Apparatus Considerations. —The leading parameters having been<br />

specified, one can proceed with the detailed design. This is straightforward,<br />

except for certain steps necessary to reduce various spurious<br />

signals in the receiver which might limit the range.<br />

These signals, for the most part, are due to amplitude modulation in<br />

the transmitter. This amplitude modulation comes from microphonics<br />

and fwm slight variation of transmitter amplitude with fTE!qU(311Cy.

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