Wave Propagation in Linear Media | re-examined
Wave Propagation in Linear Media | re-examined
Wave Propagation in Linear Media | re-examined
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Chapter 3<br />
<strong>Wave</strong> propagation <strong>in</strong><br />
electromagnetic transmission l<strong>in</strong>es<br />
One cannot escape the feel<strong>in</strong>g that these mathematical formulae have an<br />
<strong>in</strong>dependent existence of their own, that they a<strong>re</strong> wiser than we a<strong>re</strong>, wiser<br />
even than their discove<strong>re</strong>rs, that we get mo<strong>re</strong> out of them than was orig<strong>in</strong>ally<br />
put <strong>in</strong>to them. He<strong>in</strong>rich Hertz, quoted <strong>in</strong> [1]<br />
As the historical <strong>re</strong>view shows, op<strong>in</strong>ions a<strong>re</strong> divided on the question of wave propagation.<br />
To ga<strong>in</strong> some further <strong>in</strong>sight, we shall explo<strong>re</strong> several examples <strong>in</strong> the sequel, rang<strong>in</strong>g from<br />
the simple case of a homogeneous transmission l<strong>in</strong>e to transient phenomena <strong>in</strong> wave guides.<br />
The ma<strong>in</strong> <strong>in</strong>te<strong>re</strong>st of the analysis lies on signals <strong>in</strong> the evanescent <strong>re</strong>gion or stop band of<br />
transmission l<strong>in</strong>es, and among the many de nitions of the propagation velocity, we shall<br />
concentrate on that of energy velocity. Not only is its de nition clear-cut and <strong>in</strong>tuitive, we<br />
shall also nd that it gives <strong>re</strong>asonable <strong>re</strong>sults whe<strong>re</strong> the concept of group velocity must fail.<br />
At the beg<strong>in</strong>n<strong>in</strong>g of the chapter, we study the homogeneous and lossless transmission l<strong>in</strong>e<br />
<strong>in</strong> the pass band and con rm the equality of group and energy velocity. We then dig<strong>re</strong>ss<br />
to explo<strong>re</strong> a classical delay l<strong>in</strong>e known from the literatu<strong>re</strong>, whe<strong>re</strong> this identity also holds.<br />
Gradually complicat<strong>in</strong>g the model, we consider evanescence <strong>in</strong> connection with a mismatched<br />
term<strong>in</strong>ation of a nitely long transmission l<strong>in</strong>e. The logical extension of this <strong>in</strong>vestigation is to<br />
consider a f<strong>re</strong>quency-dependent medium. We thus evaluate the behaviour of waves <strong>in</strong> a lossless<br />
plasma. A short section on an <strong>in</strong>homogeneous transmission l<strong>in</strong>e concludes the t<strong>re</strong>atment of<br />
monochromatic signals. A large part is then devoted to the evaluation of transients <strong>in</strong> a<br />
plasma and a <strong>re</strong>ctangular wave guide. In both cases we shall encounter the propagation of a<br />
wave front, whose velocity will be equal to the velocity of light. The <strong>re</strong>ma<strong>in</strong>der of the chapter<br />
explo<strong>re</strong>s the propagation of a Gaussian pulse <strong>in</strong> plasma. In connection with this comparatively<br />
small-band signal, we shall also touch upon the question of causality <strong>in</strong>evanescent media.<br />
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