Home |
Search |
Today's Posts |
|
#1
![]() |
|||
|
|||
![]()
David Robbins wrote:
"Cecil Moore" wrote: Does (R+jXL)/(G+jXC) really equal 2500 for RG-174 on 12m? The specs say the Z0 of RG-174 is a nominal 50 ohms. of course its not exactly 2500, otherwise there would be no loss. but its close, maybe 2500+j10 or something like that. and even the resistive part may not be exact, the nominal 50 ohms could be 45 to 55 depending on the tolerances of the manufacturer. Comparing the 6dB loss of RG-174 to the 0.14 dB loss for hardline - is all that extra loss accounted for in the +j10 term? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#2
![]() |
|||
|
|||
![]()
You've got to be careful with cause and effect. There's not a direct
correspondence between loss and characteristic reactance. A transmission line can be very lossy, yet have a completely real characteristic impedance. Such a line doesn't have any reactance term in its characteristic impedance to "account for" its loss. To learn more about these, look up "distortionless line" in the index of your favorite transmission line text. The converse, however, isn't true. Any line which has a reactive Z0 does have loss. You can find the equations needed to calculate Z0 and loss coefficient alpha from R, G, L, and C in _Reference Data for Radio Engineers_. Deriving from them an equation directly relating alpha and Z0 should give you something to do for a number of long winter evenings. Maybe even give you a break from thinking about waves of average power bouncing about. Roy Lewallen, W7EL Cecil Moore wrote: David Robbins wrote: "Cecil Moore" wrote: Does (R+jXL)/(G+jXC) really equal 2500 for RG-174 on 12m? The specs say the Z0 of RG-174 is a nominal 50 ohms. of course its not exactly 2500, otherwise there would be no loss. but its close, maybe 2500+j10 or something like that. and even the resistive part may not be exact, the nominal 50 ohms could be 45 to 55 depending on the tolerances of the manufacturer. Comparing the 6dB loss of RG-174 to the 0.14 dB loss for hardline - is all that extra loss accounted for in the +j10 term? |
#3
![]() |
|||
|
|||
![]()
Roy Lewallen wrote:
A transmission line can be very lossy, yet have a completely real characteristic impedance. That's what I thought. Is RG-174 one of those transmission lines? Maybe even give you a break from thinking about waves of average power bouncing about. At least with average power, one cannot violate the conservation of energy principle by creating instantaneous energy in a passive load. :-) -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#4
![]() |
|||
|
|||
![]()
Cecil Moore wrote:
Roy Lewallen wrote: A transmission line can be very lossy, yet have a completely real characteristic impedance. That's what I thought. Is RG-174 one of those transmission lines? No. Distortionless lines are specially made, or periodically loaded with fixed components to achieve distortionless characteristics. Incidentally, I recently carefully measured the Z0 of nine pieces of RG-58 type cables at 10 MHz. R varied from 48.1 to 57.2 ohms, and X from -0.67 to -2.32 ohms. I made one measurement at 1 MHz, on a cable whose Z0 at 10 MHz was 49.0 - j0.69 at 10 MHz. That cable's Z0 at 1 MHz was 50.7 - j2.05 ohms. I wasn't able to make good measurements below 1 MHz with my setup. . . . Roy Lewallen, W7EL |
#5
![]() |
|||
|
|||
![]()
Roy Lewallen wrote:
Cecil Moore wrote: Roy Lewallen wrote: A transmission line can be very lossy, yet have a completely real characteristic impedance. That's what I thought. Is RG-174 one of those transmission lines? No. Distortionless lines are specially made, or periodically loaded with fixed components to achieve distortionless characteristics. Incidentally, I recently carefully measured the Z0 of nine pieces of RG-58 type cables at 10 MHz. R varied from 48.1 to 57.2 ohms, and X from -0.67 to -2.32 ohms. Assuming 57.2 - j2.32 ohms Z0, our 50 ohm SWR meters may be off by 15%? Could this be the answer to Richard C's SWR readings? I suggested that as a possibility early on but he dismissed it. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#6
![]() |
|||
|
|||
![]()
There could be quite a number of reasons Richard's readings aren't
indicating what he thinks, and this is certainly one of them. Of one thing I'm certain -- the reason is something other than actual SWR being modified by source impedance. And yes, our SWR meters can easily be that far off when attempting to measure the real SWR on real cables. Good thing it doesn't matter, huh? Roy Lewallen, W7EL Cecil Moore wrote: Assuming 57.2 - j2.32 ohms Z0, our 50 ohm SWR meters may be off by 15%? Could this be the answer to Richard C's SWR readings? I suggested that as a possibility early on but he dismissed it. |
#7
![]() |
|||
|
|||
![]() "Cecil Moore" wrote in message ... David Robbins wrote: "Cecil Moore" wrote: Does (R+jXL)/(G+jXC) really equal 2500 for RG-174 on 12m? The specs say the Z0 of RG-174 is a nominal 50 ohms. of course its not exactly 2500, otherwise there would be no loss. but its close, maybe 2500+j10 or something like that. and even the resistive part may not be exact, the nominal 50 ohms could be 45 to 55 depending on the tolerances of the manufacturer. Comparing the 6dB loss of RG-174 to the 0.14 dB loss for hardline - is all that extra loss accounted for in the +j10 term? no, its more complicated than that. the attenuation constant (usually alpha) = Re(gamma) where gamma is sqrt((R+jwL)(G+jwC)) Zo is sqrt((R+jwL)/(G+jwC)) so there is not a simple way to relate the characterisitic impedance to loss. for a low loss line the approximation for alpha is (R/2Zo)+(GZo/2) which can probalby be applied for most normal cases, but again, you have to get the R and G values of the line which can not be directly calculated from Zo. |
#8
![]() |
|||
|
|||
![]()
However, if you have coax with good dielectric (polyethylene or
Teflon), at HF and below the loss is strongly dominated by the R term. You can verify through measurements, if you are careful, that G can be assumed zero unless you've done something to degrade your line's dielectric. BUT...it's much easier to measure the line's attenuation directly than to measure (accurately) the impedance's real and imaginary parts anyway, so why would one try to do it that way? Cheers, Tom (Example: RG174 at f=30MHz will have a bit more than 3.4dB/100 feet loss because of R, and probably well under .025dB/100 feet loss because of G. See Roy's suggested reading for the source of those numbers.) "David Robbins" wrote in message ... "Cecil Moore" wrote in message ... David Robbins wrote: "Cecil Moore" wrote: Does (R+jXL)/(G+jXC) really equal 2500 for RG-174 on 12m? The specs say the Z0 of RG-174 is a nominal 50 ohms. of course its not exactly 2500, otherwise there would be no loss. but its close, maybe 2500+j10 or something like that. and even the resistive part may not be exact, the nominal 50 ohms could be 45 to 55 depending on the tolerances of the manufacturer. Comparing the 6dB loss of RG-174 to the 0.14 dB loss for hardline - is all that extra loss accounted for in the +j10 term? no, its more complicated than that. the attenuation constant (usually alpha) = Re(gamma) where gamma is sqrt((R+jwL)(G+jwC)) Zo is sqrt((R+jwL)/(G+jwC)) so there is not a simple way to relate the characterisitic impedance to loss. for a low loss line the approximation for alpha is (R/2Zo)+(GZo/2) which can probalby be applied for most normal cases, but again, you have to get the R and G values of the line which can not be directly calculated from Zo. |
#9
![]() |
|||
|
|||
![]() |
Reply |
Thread Tools | Search this Thread |
Display Modes | |
|
|