Reply
 
LinkBack Thread Tools Search this Thread Display Modes
  #1   Report Post  
Old November 20th 04, 05:44 AM
Cecil Moore
 
Posts: n/a
Default

Reg Edwards wrote:
Or even more simple, for Zo to be purely resistive, G = C*R/L


In "Transmission Lines" by Chipman, he gives an example where
R = 0.1 ohm/m and G = 0.9 micromhos/m. For Z0 to be a purely
resistive 50 ohms, G would have to be 40 micromhos/m making
the transmission line considerably more lossy just to achieve
a purely resistive Z0. Real world transmission lines rarely
have a purely resistive characteristic impedance.

The formula for the attenuation factor is R/2*Z0 + G*Z0/2
That's 0.001 + 0.0000225, so you can see that G has negligible
effect on losses, i.e. virtually all losses in the above
example are series I^2*R losses.

The attenuation factor is 0.0010225 for both the voltage and
current so it's obvious that the current attenuation is caused
by the series I^2*R losses, the same thing that causes the
voltage attenuation.
--
73, Cecil, W5DXP
Reply
Thread Tools Search this Thread
Search this Thread:

Advanced Search
Display Modes

Posting Rules

Smilies are On
[IMG] code is On
HTML code is Off
Trackbacks are On
Pingbacks are On
Refbacks are On


Similar Threads
Thread Thread Starter Forum Replies Last Post
An easy experiment with a coil Cecil Moore Antenna 57 October 29th 04 04:18 AM
NEWS - Researchers invent antenna for light Antennas for Light Antenna 79 October 12th 04 10:51 PM
Lumped Load Models v. Distributed Coils Wes Stewart Antenna 480 February 22nd 04 02:12 AM


All times are GMT +1. The time now is 02:34 PM.

Powered by vBulletin® Copyright ©2000 - 2025, Jelsoft Enterprises Ltd.
Copyright ©2004-2025 RadioBanter.
The comments are property of their posters.
 

About Us

"It's about Radio"

 

Copyright © 2017