recategorized by
242 views
0 0 votes

Transmission line transformation of a load $Z_{L}$ to $Z$ is given by

\[Z=Z_{0} \frac{Z_{1}+j Z_{0} \tan (\beta l)}{Z_{0}+j Z_{\mathrm{L}} \tan (\beta l)}\]

  1. Show that the above transformation implies that the impedance $Z$ gets transformed to $Z_{L}^{*}$ for real $Z$.
  2. What is the importance of the result derived in (a) ?

Please log in or register to answer this question.

Position:
Show:

Related questions

0 0 votes
0 0 answers
286
286 views
admin asked Sep 27, 2022
286 views
In an impedance Smith chart, a clockwise movement along a constant resistance circle gives rise toa decrease in the value of reactancean increase in the value of reactanc...
0 0 votes
0 0 answers
264
264 views
admin asked Sep 27, 2022
264 views
The $\text{VSWR}$ can have any value between$0$ and $1$$-1$ and $+1$$0$ and $\infty$$1$ and $\infty$
0 0 votes
0 0 answers
267
267 views
admin asked Sep 27, 2022
267 views
The phase velocity for the $\mathrm{TE}_{10}$ – mode in an air-filled rectangular waveguide isless than $c$equal to $c$greater than $c$none of the above( $c$ is the veloc...
0 0 votes
0 0 answers
127
127 views
gatecse asked Feb 23
127 views
A complex load (in $\Omega$ ) is represented as $\Gamma_{L}=0.5 \angle 30^{\circ}$ on the Smith chart. A co-axial cable with a characteristic impedance of $50 ~\Omega$ is...

Add Synced Question

×