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#61
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On Sun, 28 Aug 2005 07:02:03 -0500, "hasan schiers"
wrote: Thanks Wes...done...btw the antenna is for 160 meters, not 80m, Sorry, I was just thinking about the subject of the thread, not reading what you wrote. so the loss is even less. It doesn't look to me like it's worth doing anything more than tuning out the mismatch in the shack. Exactly. As I said earlier, if it makes it easier on the someone's (not you, you get it) conscience or ego they can think of the transmission line as a bunch of distributed L and Cs (with a little R thrown in) that are part of a tuner. When they get this "tuner" to show 50 +j0, then they can call the length of line between the "tuner" and the transmitter, the "transmission line." In your case, you have a low-loss line, so the "R" part is low and the system is efficient. |
#62
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Frank,
Thank you. Is there any way you can forward the saved parameters. This is a screwdriver antenna, I will remeasure the coil and double check. My modeling of the free space antenna showed about 4 Ohms but it was with a much simpler program. It was that program I used to measure Q. Thanks, Dan Hi Dan, I have run the program to determine the precise resonance. The parameters are as follows: Inductor 89.3 uH, and resonant at 3.92 MHz. I can send you a zipped NEC output text file. It is about 190 kB. Also the NEC code I used. You can plug in the appropriate data into an Excel spread sheet. If you need any specific graphical output I can it as a JPEG file. I used the default input source of 1 V peak, which accounts for the low power values in the output file. The E-field data is far field, normalized to 1 meter. The inductor is described as a lumped element, complex impedance, of 4.9 + j2200 ohms. I arrived at this value based on your Q of 450, and just played around with the imaginary value to achieve resonance within the 75 meter band. Let me know if I can send the above information to the address shown in your posting. Regards, Frank |
#63
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Wes,
As a starter, look at this site: http://www.cbtricks.com/~ab7if/coax/coax.htm When a transmission line is terminated in it's characteristic impedance there is no voltage or current reflection from the line. The electromagnetic fields continue to flow into the termination as if the line were infinitely long. When a mismatch of impedance occurs, reflected waves will be produced and they will interact with the incident waves. The total voltage and current on the line are no longer the result of a single traveling wave from the source to the load. Instead, it is the algebraic sum of two waves traveling in opposite directions. This interaction results in what is known as standing waves. The waves remain in fixed positions along the line while they vary in amplitude and polarity. A wave of any shape can be transmitted along the line without any change of waveshape or magnitude. Looking at the gif below, we see a line driven with a sine wave generator, terminated with a short circuit to maximize the reflection. My first claim is a tuner at the source does not materially improve what is happening in the coax. That is a tuner does not recreate the condition above where the coax is functioning as a properly matched and terminated transmission line. All the tuner does is match the impedance at the coax source back to some known, usually 50 Ohm, value. My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself. Dan Wes Stewart wrote: On Sat, 27 Aug 2005 16:53:39 -0700, dansawyeror wrote: Let's take the case of a 50 Ohm line and some mismatched antenna. The result is a combination other then 50 Ohm with most likely a zero complex component. Surely you don't believe this do you? It is -much- more likely that the impedance is reactive than not. At one (fundamental) frequency the reactance is zero. At every other frequency it is reactive. All a tuner does is match 50 Ohm at the radio to the complex impedance presented to it at the source of the line. Isn't that enough? That the only place with 50 Ohms and zero inductance in the line - antenna system. The combination of cable and antenna presents something other then R = 50 ohms 0 reactance and the the transmission line see discontinuities. The result is it radiates. Oh dear me. |
#64
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Wes,
As a starter, look at this site: http://www.cbtricks.com/~ab7if/coax/coax.htm When a transmission line is terminated in it's characteristic impedance there is no voltage or current reflection from the line. The electromagnetic fields continue to flow into the termination as if the line were infinitely long. When a mismatch of impedance occurs, reflected waves will be produced and they will interact with the incident waves. The total voltage and current on the line are no longer the result of a single traveling wave from the source to the load. Instead, it is the algebraic sum of two waves traveling in opposite directions. This interaction results in what is known as standing waves. The waves remain in fixed positions along the line while they vary in amplitude and polarity. A wave of any shape can be transmitted along the line without any change of waveshape or magnitude. Looking at the gif below, we see a line driven with a sine wave generator, terminated with a short circuit to maximize the reflection. My first claim is a tuner at the source does not materially improve what is happening in the coax. That is a tuner does not recreate the condition above where the coax is functioning as a properly matched and terminated transmission line. All the tuner does is match the impedance at the coax source back to some known, usually 50 Ohm, value. My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself. Dan Wes Stewart wrote: On Sat, 27 Aug 2005 16:53:39 -0700, dansawyeror wrote: Let's take the case of a 50 Ohm line and some mismatched antenna. The result is a combination other then 50 Ohm with most likely a zero complex component. Surely you don't believe this do you? It is -much- more likely that the impedance is reactive than not. At one (fundamental) frequency the reactance is zero. At every other frequency it is reactive. All a tuner does is match 50 Ohm at the radio to the complex impedance presented to it at the source of the line. Isn't that enough? That the only place with 50 Ohms and zero inductance in the line - antenna system. The combination of cable and antenna presents something other then R = 50 ohms 0 reactance and the the transmission line see discontinuities. The result is it radiates. Oh dear me. |
#65
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On Sun, 28 Aug 2005 09:38:52 -0700, dansawyeror
wrote: My first claim is a tuner at the source does not materially improve what is happening in the coax. That is a tuner does not recreate the condition above where the coax is functioning as a properly matched and terminated transmission line. All the tuner does is match the impedance at the coax source back to some known, usually 50 Ohm, value. Hi Dan, As true as that may be, the results run the gamut from trivial to considerable as has been already discussed in this thread. My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself. This mismatch could arise for any number of reasons, and not all contribute to radiation from the coax. Wes has already demonstrated a deliberate mismatch at the end of a cable that exhibits absolutely no radiation from the coax. This is because he has contrived to contain the fields from emerging and coupling to the outside of the coax shield. You should be aware that the shield does support currents on the inside and outside that are wholly unaffected by each other - except at the drive point where the two conduction paths are joined. When you drive a dipole with a coax, the exterior conductive path of the shield (a separate circuit from the interior conductive path of that same shield) is in parallel with one arm of the dipole. This means you have a third radiator that has a length and termination that is undefined. It is THAT radiator that both causes a higher SWR AND radiation that is not a normal condition for an otherwise tuned antenna. Given that the length of the line's external conductive path, and its termination is largely undefined (unless you take great care to both measure and characterize such issues), the occurrence of mismatch and radiation is highly variable. Thus, anecdotal accounts of antennas being poor or good when they are driven by a simple coax are suspect (barring the reporter also supplying the conditions of the external path). To eliminate the effects of this third path, a choke is added to the drive point. The purpose of the choke is to add impedance to this path to reduce Common Mode current. Common Mode current is the current that flows due to an unbalanced system (the unanticipated third radiator does that in spades). It flows in two wire transmission lines too when the unbalance occurs for other reasons (and those are plentiful as well). 73's Richard Clark, KB7QHC |
#66
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On Sun, 28 Aug 2005 09:39:24 -0700, dansawyeror
wrote: Wes, As a starter, look at this site: http://www.cbtricks.com/~ab7if/coax/coax.htm snip My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself. Dan Well, Dan, responding to your second claim first, consider either of two situations, 1) center-fed dipole, fed with open wire line, or 2) a center fed dipole, fed with coax with an efficient choke balun. In either of these situations an impedance mismatch between the feedline and the dipole will NOT cause radiation from the feedline. And taking a look at the web site you referenced above, the writer is professing to clear some misconceptions concerning transmission line technique. However, although he does present some straight dope, he is also further spreading some misconceptions concerning SWR. As he stated, there is a lot of misunderstanding concerning the effect of line length on the amplitude of the standing wave, but he continued the incorrect information on the subject, rather than presenting a correction. The fact is, Dan, that with lossless line the SWR is NOT affected by the line length--it remains constant along the entire length of the line. And further, the ONLY affect of line length on SWR is line attenuation, which causes the SWR at the input to be less than that at the load. If you believe everything you read in that reference, you've been duped. Walt, W2DU |
#67
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dansawyeror wrote:
My first claim is a tuner at the source does not materially improve what is happening in the coax. That is a tuner does not recreate the condition above where the coax is functioning as a properly matched and terminated transmission line. All the tuner does is match the impedance at the coax source back to some known, usually 50 Ohm, value. No matter what the voltages and currents are, if they are balanced, the transmission line won't radiate (much). If the SWR is 100:1 and the currents are balanced, the transmission won't radiate (much). If the SWR is 1:1 and the currents are unbalanced, the feedline is likely to radiate. My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself. Please understand it is not impedance mismatches that cause radiation from the feedline. It is unbalance in the feedline currents that causes feedline radiation. Current imbalance and impedance mismatches are not necessarily related. Current imbalance in a matched system can cause feedline radiation. Impedance mismatches can exist with negligible feedline radiation. -- 73, Cecil http://www.qsl.net/w5dxp ----== Posted via Newsfeeds.Com - Unlimited-Uncensored-Secure Usenet News==---- http://www.newsfeeds.com The #1 Newsgroup Service in the World! 100,000 Newsgroups ---= East/West-Coast Server Farms - Total Privacy via Encryption =--- |
#68
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On Sun, 28 Aug 2005 09:38:52 -0700, dansawyeror
wrote: Wes, As a starter, look at this site: http://www.cbtricks.com/~ab7if/coax/coax.htm When a transmission line is terminated in it's characteristic impedance there is no voltage or current reflection from the line. The electromagnetic fields continue to flow into the termination as if the line were infinitely long. When a mismatch of impedance occurs, reflected waves will be produced and they will interact with the incident waves. The total voltage and current on the line are no longer the result of a single traveling wave from the source to the load. Instead, it is the algebraic sum of two waves traveling in opposite directions. This interaction results in what is known as standing waves. The waves remain in fixed positions along the line while they vary in amplitude and polarity. A wave of any shape can be transmitted along the line without any change of waveshape or magnitude. Looking at the gif below, we see a line driven with a sine wave generator, terminated with a short circuit to maximize the reflection. I am certainly not the sharpest guy in this forum, however, I have been a ham for almost 47 years and I've been working with antennas from the beginning. I retired after 33+ years in the aerospace business where a good deal of my work involved rf design, measurements, failure analysis and the writing of specifications for rf/microwave devices and assemblies. I regret having to even bring this up, but it seems that you're willing accept something written on a CB radio site as fact while ignoring anything you hear in this forum from professionals in the field. Why is that? My first claim is a tuner at the source does not materially improve what is happening in the coax. Please show me the place where I claimed anything different. That is a tuner does not recreate the condition above where the coax is functioning as a properly matched and terminated transmission line. All the tuner does is match the impedance at the coax source back to some known, usually 50 Ohm, value. Please show me the place where I claimed anything different. My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself. This I've already proved to be wrong by example. Let me try one last time. Since antennas are reciprocal, you don't even need a transmitter. Connect any length of coax to your receiver input. Terminate the far end with a dummy load (50 ohm resistor). Tune around the bands. What do you hear? Nothing, if the coax is any good and the receiver and dummy load are well shielded. So I suppose this proves one of your claims, a matched line doesn't radiate. Remove the dummy load and replace it with a short circuit. What do you hear now on this totally mismatched line that by your reckoning should radiate like crazy? |
#69
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Frank,
My e-mail address is above. Thank you for all your help. I will try this. Dan Frank wrote: Frank, Thank you. Is there any way you can forward the saved parameters. This is a screwdriver antenna, I will remeasure the coil and double check. My modeling of the free space antenna showed about 4 Ohms but it was with a much simpler program. It was that program I used to measure Q. Thanks, Dan Hi Dan, I have run the program to determine the precise resonance. The parameters are as follows: Inductor 89.3 uH, and resonant at 3.92 MHz. I can send you a zipped NEC output text file. It is about 190 kB. Also the NEC code I used. You can plug in the appropriate data into an Excel spread sheet. If you need any specific graphical output I can it as a JPEG file. I used the default input source of 1 V peak, which accounts for the low power values in the output file. The E-field data is far field, normalized to 1 meter. The inductor is described as a lumped element, complex impedance, of 4.9 + j2200 ohms. I arrived at this value based on your Q of 450, and just played around with the imaginary value to achieve resonance within the 75 meter band. Let me know if I can send the above information to the address shown in your posting. Regards, Frank |
#70
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Somone wrote:
"My second claim is when the mismatch condition at the coax destination, i.e. antenna that may result in significant radiation from the coax itself." Responses already show this is untrue. Radiation from the external coax surface comes from launching a signal on that surface. Good coax does not let signals penetrate its shield. A mismatch between a transmission line and its attached antenna affects both transmitting and receiving from the antenna, but does not launch signals on the outside of the coax. A mismatched transmitting antenna does not accept all available power incident upon it and reflects a portion back toward the sender depending on how bad the mismatch is. A mismatched receiving antenna has a source resistance (radiation resistance) and may also have reactance. A conjugate match is needed for maximum power transfer to the feedline. The mismatched antenna will either not extract all the power available to it in the passing wave or else reradiate more than 50%, (with full extraction, the minimum possible reradiation is with a perfectly matched antenna). Consider a short circuit across the antenna feedpoint. 100% of the energy extracted by the antenna is reradiated. Consider an open circuit at the antenna feedpoint. Little if any power is extracted from the wave sweeping the receiving antenna. The most power is received by a receiving antenna when its radiation resistance is matched to the Zo of the feedline. In this case, 50% is the best possible received carrier power in the receiver input. Nobody tells the antenna it is a receiving antenna. It is a conductor carrying a current, never mind where it came from, so it is going to radiate. When matched resistances are involved in source (radiation resistance) and load (Zo matched), the power is split 50-50 between source and load. The radiation resistance, is the source resistance for the receiver load, and it represents the reradiation from the reeiving atenna. 50% of the received power accepted by the load is the best possible performance. Mismatch means less. Either less power accepted by the antenna or more power reradiated by by the antenna. A transmatch can make the feedline appear as a matching load at the antenna junction for receiving. If matched for both transmitting and receiving, all available power will be transmitted and received. Best regards, Richard Harrison, KB5WZI |
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