27.12.2012 Views

Wave Propagation in Linear Media | re-examined

Wave Propagation in Linear Media | re-examined

Wave Propagation in Linear Media | re-examined

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

3.5 A dispersive system: the lossless plasma<br />

0<br />

0.66<br />

ve/c 0.4 .4<br />

0.2 .2<br />

0<br />

100<br />

2<br />

4<br />

X<br />

6<br />

10<br />

8<br />

10<br />

1<br />

ρ<br />

0.1<br />

0.01<br />

Figu<strong>re</strong> 3.7: Evaluation of the energy velocity (3.46) <strong>in</strong> the pass band of a lossless plasma depend<strong>in</strong>g<br />

on the spatial coord<strong>in</strong>ate X and the term<strong>in</strong>ation factor . The length of the l<strong>in</strong>e is L = 10, the signal<br />

f<strong>re</strong>quency is given by !p=! =0:8. Note the partially logarithmic scale.<br />

0<br />

100<br />

2<br />

10<br />

4<br />

X<br />

6<br />

1<br />

ρ<br />

8<br />

10<br />

0.1<br />

0.01<br />

0.2<br />

0<br />

0.6<br />

0.4<br />

ve/c<br />

Figu<strong>re</strong> 3.8: Evaluation of the energy velocity (3.47) <strong>in</strong> the evanescent <strong>re</strong>gion of a lossless plasma<br />

depend<strong>in</strong>g on the spatial coord<strong>in</strong>ate X and the term<strong>in</strong>ation factor . The parameters a<strong>re</strong> L = 10 and<br />

!p=! =1:25 . Note the partially logarithmic scale.<br />

43

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!