Multipactor in Low Pressure Gas and in ... - of Richard Udiljak
Multipactor in Low Pressure Gas and in ... - of Richard Udiljak
Multipactor in Low Pressure Gas and in ... - of Richard Udiljak
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Chapter 5<br />
<strong>Multipactor</strong> <strong>in</strong> coaxial l<strong>in</strong>es<br />
The coaxial l<strong>in</strong>e is a very common <strong>and</strong> important component <strong>in</strong> microwave<br />
systems. It is a transmission l<strong>in</strong>e that consists <strong>of</strong> an <strong>in</strong>ner<br />
cyl<strong>in</strong>drical conductor <strong>and</strong> a coaxial outer conductor. A constant crosssection<br />
is ma<strong>in</strong>ta<strong>in</strong>ed by means <strong>of</strong> a dielectric medium, which is conta<strong>in</strong>ed<br />
between the conductors. In some space applications, as well as <strong>in</strong><br />
other systems, the dielectric medium has been partly omitted <strong>in</strong> order to<br />
save weight or to reduce the dielectric losses. In a vacuum environment,<br />
the l<strong>in</strong>e may become evacuated, which makes it exposed to the risk <strong>of</strong> a<br />
multipactor discharge.<br />
The electric field <strong>in</strong> a coaxial l<strong>in</strong>e is nonuniform, which makes analytical<br />
analysis difficult, s<strong>in</strong>ce the the equation <strong>of</strong> motion for an electron becomes<br />
a non-l<strong>in</strong>ear differential equation. However, multipactor <strong>in</strong> a coaxial<br />
l<strong>in</strong>e has been studied experimentally [63] <strong>and</strong> numerically [64–67]. In<br />
these studies it was found that two different types <strong>of</strong> resonant multipactor<br />
can occur, namely a two-sided discharge between the outer <strong>and</strong><br />
the <strong>in</strong>ner conductors <strong>and</strong> the one-sided analogue on the outer conductor.<br />
In an attempt to underst<strong>and</strong> the effect <strong>of</strong> vary<strong>in</strong>g the relative <strong>in</strong>ner<br />
radius, i.e. vary<strong>in</strong>g the characteristic impedance <strong>of</strong> the coaxial l<strong>in</strong>e,<br />
different scal<strong>in</strong>g laws were suggested <strong>in</strong> these studies. Another study focused<br />
on the current due to the multipact<strong>in</strong>g electrons <strong>and</strong> treated this<br />
as a radially oriented Hertzian dipole <strong>in</strong> order to determ<strong>in</strong>e the electric<br />
field generated by the multipactor discharge [68].<br />
In paper E resonant multipactor <strong>in</strong> a coaxial l<strong>in</strong>e is analysed by<br />
means <strong>of</strong> an approximate analytical solution <strong>of</strong> the non-l<strong>in</strong>ear differential<br />
equation <strong>of</strong> motion, which <strong>in</strong> a large range <strong>of</strong> microwave frequencies<br />
<strong>and</strong> amplitudes agrees very well with the numerical solution. As<br />
69