![]() |
Shorted 1/4 wave stub ?
I know that a shorted 1/4 wave stub exhibits a very high impedance. But
for the 2nd harmonic it's a 1/2 wave stub and exhibits a very low impedance or a short. There are claims that this can be used to filter the even harmonics. Shorts can't diisipate power and must reflect, so how does a stub work? -- 73 Hank WD5JFR |
"Henry Kolesnik" wrote in message ... I know that a shorted 1/4 wave stub exhibits a very high impedance. But for the 2nd harmonic it's a 1/2 wave stub and exhibits a very low impedance or a short. There are claims that this can be used to filter the even harmonics. Shorts can't diisipate power and must reflect, so how does a stub work? 73 Hank WD5JFR Put a Tee on a coax line and connect the stub there. At the H2 there is a short and reflectinonback up-stream. Common filters you see everywhere are "reflective" by nature / design as well. They have other than Zo off frequency and therefore reflect the unwanted stuff back to the source. It has to be able to handle it. Help any? -- Steve N, K,9;d, c. i My email has no u's. |
I know that a shorted 1/4 wave stub exhibits a very high impedance. But
for the 2nd harmonic it's a 1/2 wave stub and exhibits a very low impedance Shorts can't diisipate power and must reflect, so how does a stub work? Hi Hank, A 1/2 wave shorted stub looks like a series resonant circuit. It makes a good notch filter, which is one of the Amateur applications that I have used. You are right, they don't dissipate any power since Power=I**2*R and R equals zero. 73 Gary N4AST |
Hi Hank, A 1/2 wave shorted stub looks like a series resonant circuit.
It makes a good notch filter, which is one of the Amateur applications that I have used. You are right, they don't dissipate any power since Power=I**2*R and R equals zero. 73 Gary N4AST ============================ R is not zero. It can be several ohms. And lots of amps can flow. Just to add a 1/2-wave shorted stub also makes a mess of the tuning of the remainder of the antenna system at all other frequencies. It must be designed "in". |
R is not zero. It can be several ohms. And lots of amps can flow.
OK Reg, but in this ideal rf environment we Amateurs live in R is zero. Just to add a 1/2-wave shorted stub also makes a mess of the tuning of the remainder of the antenna system at all other frequencies. It must be designed "in". That should be fairly obvious to the most casual observer. :-). In the receive applications that I have used a 1/2 wave shorted stub as a notch filter, I can assure you I did not have lots of Amps flowing. 73 Gary N4AST |
Henry Kolesnik wrote:
I know that a shorted 1/4 wave stub exhibits a very high impedance. But for the 2nd harmonic it's a 1/2 wave stub and exhibits a very low impedance or a short. There are claims that this can be used to filter the even harmonics. Shorts can't diisipate power and must reflect, so how does a stub work? Consider the following configuration: Source----ideal 1 WL feedline-----------+-----matched load | |Stub | | open If the stub is 1/4WL, the forward voltage and reflected voltage in the stub is the same as on the feedline. At the mouth of the stub, they are 180 degrees out of phase and superpose to zero volts which obeys Ohm's law and delivers zero power to the load. Double the frequency. That makes the stub 1/2WL. The forward voltage and reflected voltage are essentially the same as in the 1/4WL stub but this time they are in phase and superpose to a maximum value which obeys Ohm's law and delivers maximum power to the load. Absolutely nothing except superposition and interference happens at the mouth of a stub. All the reflected action happens at the physical open circuit. Virtual impedances are only a V/I ratio and CANNOT cause reflections. Absolutely no reflections are happening at the mouth of the stub (unless a physical impedance discontinuity exists there). Consider this. If a stub really presented an infinite impedance, you could simply remove it and nothing would change. Something inside the stub happens to cause that infinite virtual impedance. Hint: Stubs have a near-infinite SWR. To understand that assertion, consider how much voltage exists at a voltage minimum inside a stub. It is nearly zero. -- 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! =----- |
JGBOYLES wrote:
Hi Hank, A 1/2 wave shorted stub looks like a series resonant circuit. It makes a good notch filter, which is one of the Amateur applications that I have used. You are right, they don't dissipate any power since Power=I**2*R and R equals zero. Stubs dissipate the maximum amount of power possible since the SWR on a stub is nearly infinite. If you don't believe it, hang a Bird Wattmeter halfway down a stub. The ratio of Vmax/Vmin and Imax/Imin is very high. If the stub were lossless, the SWR inside a stub would be infinite. After all, a stub is merely a shorted or open piece of transmission line. -- 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! =----- |
JGBOYLES wrote:
That should be fairly obvious to the most casual observer. :-). In the receive applications that I have used a 1/2 wave shorted stub as a notch filter, I can assure you I did not have lots of Amps flowing. Have you ever measured it? Have you any idea of the magnitude of current measurable at the shorted point in a stub during transmit? -- 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! =----- |
Have you ever measured it? Have you any idea of the magnitude of
current measurable at the shorted point in a stub during transmit? No Cecil I don't, should I? The only experience I have with a shorted 1/2 wave stub is in receive applications. I have swept them with a homebrew spectrum analyzer and tracking generator and can say they look like series resonant circuits. At the micro watt level will I still have several Amps in the stub? How would you measure the current in the stub during transmit using equipment the average ham (like me) has laying around the shack ? 73 Gary N4AST |
JGBOYLES wrote:
Have you ever measured it? Have you any idea of the magnitude of current measurable at the shorted point in a stub during transmit? No Cecil I don't, should I? The only experience I have with a shorted 1/2 wave stub is in receive applications. I have swept them with a homebrew spectrum analyzer and tracking generator and can say they look like series resonant circuits. At the micro watt level will I still have several Amps in the stub? Of course not for receive. Here's the statement to which I was objecting: "... they don't dissipate any power since Power=I**2*R and R equals zero." R is not zero half-way into a shorted 1/2WL stub. For a lossless stub, R is infinite at the half-way point. Stubs have considerable I^2*R losses during transmit. Of course, if you are using them to notch filter out unwanted receive signals, you want them to be lossy. How would you measure the current in the stub during transmit using equipment the average ham (like me) has laying around the shack ? Wrap ten turns of pickup wire on a ferrite toroid. Use a dummy load to calibrate it by running the dummy load wire through it. Then install the shorted stub wire through the ferrite toroid and make the measurement. Roy Lewallen describes how to measure RF current in his article in "The ARRL Antenna Compendium", vol 1, in "Baluns: What They Do and How They Do It." Or install a one ohm resistor at the stub short and measure the voltage. An oscilloscope will do. You don't need super high accuracy. For the following stub, we can estimate the value of the current at the short in the stub assuming a lossless line. The source is a 100W Signal Generator equipped with a perfect Circulator and Load 100W SGCL----50 ohm feedline-----------+---50 ohm load | |1/2WL Stub |50 ohms | short No current reaches the load. The forward current is 1.414 amps and the reflected current is 1.414 amps on the feedline and inside the stub. 100 watts of reflected power is being dissipated in the circulator load resistor. The RMS current at the short is 2.828 amps, the in-phase sum of the forward and reflected currents. The peak-to-peak current at the short is 8 amps. The only reflection point in the entire above system is at the short at the end of the stub. No reflections occur at '+'. -- 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! =----- |
All times are GMT +1. The time now is 12:30 AM. |
Powered by vBulletin® Copyright ©2000 - 2025, Jelsoft Enterprises Ltd.
RadioBanter.com