Author:
KAUP D. J.,THOMAS GARY E.
Abstract
Assuming the averaged (background) electron distribution in a crossed-field
device, such as a magnetron or crossed-field amplifier, to be slowly varying
between the cathode and the anode, we develop a WKB approximation for the
cold-fluid plasma equations of a planar magnetron. In this approximation,
we
can give general expressions for the solution of linearized, high-frequency
oscillations in such a device in terms of two integrals. Assuming also
that the
high-frequency wave in the slow-wave structure drives the response in the
electron plasma, we are then able to show that the current drawn by a crossed-field device will be proportional to the power propagating in the slow-wave
structure. Thus the device will operate as a linear amplifier. We also
show, in
the same approximation, that the averaged electron sheath that forms when
the
device is operating is independent of the current being drawn. Thus the
current
will not be limited by the sheath, but only by the ability of the cathode
to emit
electrons. In the process, we also obtain expressions for the linear growth
rate
and the value of the quasilinear diffusion coefficient at the diocotron
resonance,
in terms of parameters of the background electron sheath.
Publisher
Cambridge University Press (CUP)
Cited by
8 articles.
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