Home |
Search |
Today's Posts |
#11
![]() |
|||
|
|||
![]()
On Thu, 3 Jun 2004 14:56:44 -0400, "Jack Painter"
wrote: Bruce, you're making a totally off the wall argument now, with opposite assumptions that were never asserted or offered by any of the posters to this thread. Taking your questions literally as you phrased them would generate a laugh by all, indeed. If a laugh was your intention, we'll all have a good one. But I doubt that you are confused about skin effect, or why a faraday cage works, and specifically what would defeat it's protection (ie: an opening). So if you seriously think that for instance, a c-clamp applied across an open end of thin walled copper tubing, contacting the inner and outer wall in it's grip, would apply voltage differently to the inside versus the outside of this tubing, then it will be easy to explain your error in thinking. And since I did not make a joke of your obvious geometry and math errors in determining the surface area of an object, one which you continue to be confused about, I would suggest that we either: end the thread if you do not desire pleasant and professional discussion, or, omitting the snide comments that do not reflect well on the group or it's interested participants. Respectfully, Jack Painter Virginia Beach, Va Oh boy! I just got back from vacation and am just now reading this stuff. Jack, Bruce and the others are entirely right. I once had a hard time figuring out why RF would not flow on the inside of a tube too. It would seem logical that it would do as you say but it doesn't. Look up "wave guide beyond cutoff". That will answer your question about why rf dose not flow on the inside of a tube. It will flow on the inside for only a very short distance from the opening. Then it gets canceled. This is how many signal generator attenuater work. They use a tube of 6 or so inches long with a sliding probe inside fed from one end. On the other open end is a fixed pickup probe. When the movable probe is close to the fixed probe on the other end, maximum signal coupling is obtained. As the other probe is moved away inside the tube the signal becomes highly attenuated. It is operating as a wave guide that is much too small for the frequency involved. If the tube diameter was made large enough to be a quarter wave length in diameter then the rf would propagate through it. But that would be in a different mode than the skin effect conduction being discussed. By the way did you know that skin effect even comes into play in 60 hz distribution systems? Regards Gary |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
SSB Antenna theory | Electronics | |||
Notes on short SSB antennas, for Larry | Cruising | |||
Notes on short SSB antennas, for Larry | Electronics | |||
How to use a simple SWR meter and what it means to your VHF | Electronics |