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Radar System Engineering

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SEC. 10.5] MAGNETRON CHARACTERISTICS 341<br />

nal to the tube and are accessible to change. In microwave magnetrons,<br />

the circuit elements are an integral part of the tube and must be incorporated<br />

with great care into every new design.<br />

Thus any radar system designed to meet a new set of conditions or to<br />

operate on a new frequency will require the development of a new magnetron<br />

type, or at least a critical evaluation of the characteristics of<br />

existing types. Since the over-all characteristics of the radar system<br />

are so closely related to, and restricted by, the performance of the magnetron,<br />

a general knowledge of the important characteristics of magnetrons<br />

is essential.<br />

Listed below with a discussion of each are the characteristics of<br />

magnetrons of particular importance to system design. These characteristics<br />

are not usually independent of one another and their relationships<br />

are also considered.<br />

Wavelen@h S’caling.-Since the wavelength of the radiation from a<br />

magnetron is fixed or at best variable over a limited range, operation on<br />

different wavelengths requires different tubes. To a first approximation,<br />

magnetrons of different wavelength are derived from one another by a<br />

simple over-all scaling process. All essential dimensions of the tube are<br />

altered by the scaling factor a = A/XO, where A is the new wavelength<br />

desired and XOis the wavelength associated with the original dimensions.<br />

If thk is done, the new tube at wavelength ~ will operate at the original<br />

voltage and current, and at a magnetic field H = ~ Ho, where Ho is the<br />

operating magnetic field of the original magnetron. The power input,<br />

and thus the power output, increases with increasing wavelength. A<br />

rough rule is: The pulse power output (or input) of sculed magnetrons<br />

varies as the square of their wavelength. The change in the size of the tube<br />

with wavelength is the basis of this rule. The pulse power input is often<br />

limited by cathode emission and, since the cathode area is proportional<br />

to hz, pulse power input is also proportional to ~? Similar reasoning<br />

shows that if the pulse power output is limited by r-f voltage breakdown<br />

tvithin the tube, the same variation of power with wavelength is to be<br />

expect ed.<br />

This rule is an important one from the standpoint of system design.<br />

At any given time it may not be exact, because special emphasis may<br />

have been given to obtaining high peak powers at a particular wavelength<br />

and a better design evolved as a result. In the long run, however,<br />

the validity of the rule is reestablished, because any new design can,<br />

within limits, be used to advantage at other wavelengths.<br />

Pulse Power.-The most outstanding characteristic of pulsed microwave<br />

magnetrons is their extremely high pulse power output, made<br />

pchsible by the very large emission yielded by oxide cathodes when pulsed,

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