Home |
Search |
Today's Posts |
|
#1
![]() |
|||
|
|||
![]()
In TV broadcasting reflections from the antenna back to the transmitter will
be reflected by the transmitter to the antenna and the signal will be rebroadcast albeit at somewhat less power. Then depending on the length of transmission line the viewer may see ghosting. In audio I don't know why and I have run my Collins 30S-1 into ladder line with a 14 to SWR with no one except me knowing! -- 73 Hank WD5JFR "Richard Clark" wrote in message ... On Sun, 5 Jun 2005 10:02:17 -0400, "Fred W4JLE" wrote: You have created an all encompassing case from the original SWR of 1.7:1 Thanx Fred, No one has ever been able to answer when the Transmitter rereflects energy, why they need a tuner. 73's Richard Clark, KB7QHC |
#2
![]() |
|||
|
|||
![]()
On Sun, 05 Jun 2005 21:58:06 GMT, "Henry Kolesnik"
wrote: In TV broadcasting reflections from the antenna back to the transmitter will be reflected by the transmitter to the antenna and the signal will be rebroadcast albeit at somewhat less power. |
#3
![]() |
|||
|
|||
![]()
On Sun, 05 Jun 2005 21:58:06 GMT, "Henry Kolesnik"
wrote: In TV broadcasting reflections from the antenna back to the transmitter will be reflected by the transmitter to the antenna and the signal will be rebroadcast albeit at somewhat less power. Hi Hank, That would pretty much reveal the SWR if we knew, wouldn't it? If "somewhat less power" was in 1.2:1 ratio, we wouldn't care so much, but how would the viewer feel about such service? Then depending on the length of transmission line the viewer may see ghosting. I think we, or another correspondent and I have dealt with that at one time. At the time I believe it was called "fringing," not "ghosts." The difference being that what were called ghosts at the dawn of the TV era were separated by fractions of an inch rather than fractions of a mm. As such, ghosts couldn't have been originated by anything shorter than mile length transmission lines that were poorly terminated at both ends. Instead, ghosts were actually transmission path length differentials in a multipath situation. In audio I don't know why and I have run my Collins 30S-1 into ladder line with a 14 to SWR with no one except me knowing! Well, if this is meant to be analogous to fringing/ghosting, I suppose its because a microsecond blur at AF is entirely inaudible. Or are we speaking of SSTV? However, this begs the question, How did you know? All the Collins equipment I taught at school didn't come with a SWR meter. It was wholly unnecessary if you performed the standard tune-up. Matter of fact, back then the only SWR meter I saw was for Ham gear. The finals' tank performed every function of matching as any tuner. However, with the KWT-6, we did use an external tuner, 180-V1 (although I may have this mixed up with another model), for coax feedlines. This was more for its automatic feature where the transmitter could be tuned up with a 50 Ohm load, and the automatic tuner simply did the job of presenting it with the transformed load. However, returning to the point of a transmitter rereflecting a reflection; I know the bare KWT-6 into ladder line employs its tank to protect its final tubes. Without that safeguard, I have seen plates melt - something no one here wants to call dissipation lest it be evidence of an internal resistance. The bare tubes with their native very hi Z would rereflect like nothing else - and this begs the observation - how could you get original any power out of them, past the tremendous mismatch? The tuner/final tank comes back into the equation, and rereflection goes out the window as a property of the transmitter and returns to the domain of matching. If anyone wants to constrain the entire crusade of the rereflecting transmitter to the tube set feeding ladder line - then feel free to do so. However, I don't think I've ever seen a mobile tube rig feeding ladder line - no doubt one day I will. We will probably talk about efficiency. :-) 73's Richard Clark, KB7QHC |
#4
![]() |
|||
|
|||
![]()
However, I don't think I've ever seen a mobile tube rig feeding
ladder line - no doubt one day I will. We will probably talk about efficiency. :-) It was done in 1936. http://web.wt.net/~nm5k/mobile36.jpg Cover pix from a 1936 QST...Forgot what month... But I still think I prefer coax... Their "ladder line" looked to be a twisted wire feeder. The call on that vehicle was W9MSY... With the short feedline run on a mobile, even coax is pretty low loss... I never used an SWR meter when I was a novice...I had an old viking valiant that would tune nearly anything...You didn't need a meter... You just loaded it up to full plate current and went with it...My TS 830 is like that to a lesser extent.. If it loads within the loading range, it's good nuff... No point in even putting a meter on it...Adding a tuner, would just add some loss...MK |
#6
![]() |
|||
|
|||
![]()
Hi Richard
Please tell me more about melting the finals and a bit more explanation of what was happening? tnx Hank "Richard Clark" wrote in message ... On Sun, 05 Jun 2005 21:58:06 GMT, "Henry Kolesnik" wrote: In TV broadcasting reflections from the antenna back to the transmitter will be reflected by the transmitter to the antenna and the signal will be rebroadcast albeit at somewhat less power. Hi Hank, That would pretty much reveal the SWR if we knew, wouldn't it? If "somewhat less power" was in 1.2:1 ratio, we wouldn't care so much, but how would the viewer feel about such service? Then depending on the length of transmission line the viewer may see ghosting. I think we, or another correspondent and I have dealt with that at one time. At the time I believe it was called "fringing," not "ghosts." The difference being that what were called ghosts at the dawn of the TV era were separated by fractions of an inch rather than fractions of a mm. As such, ghosts couldn't have been originated by anything shorter than mile length transmission lines that were poorly terminated at both ends. Instead, ghosts were actually transmission path length differentials in a multipath situation. In audio I don't know why and I have run my Collins 30S-1 into ladder line with a 14 to SWR with no one except me knowing! Well, if this is meant to be analogous to fringing/ghosting, I suppose its because a microsecond blur at AF is entirely inaudible. Or are we speaking of SSTV? However, this begs the question, How did you know? All the Collins equipment I taught at school didn't come with a SWR meter. It was wholly unnecessary if you performed the standard tune-up. Matter of fact, back then the only SWR meter I saw was for Ham gear. The finals' tank performed every function of matching as any tuner. However, with the KWT-6, we did use an external tuner, 180-V1 (although I may have this mixed up with another model), for coax feedlines. This was more for its automatic feature where the transmitter could be tuned up with a 50 Ohm load, and the automatic tuner simply did the job of presenting it with the transformed load. However, returning to the point of a transmitter rereflecting a reflection; I know the bare KWT-6 into ladder line employs its tank to protect its final tubes. Without that safeguard, I have seen plates melt - something no one here wants to call dissipation lest it be evidence of an internal resistance. The bare tubes with their native very hi Z would rereflect like nothing else - and this begs the observation - how could you get original any power out of them, past the tremendous mismatch? The tuner/final tank comes back into the equation, and rereflection goes out the window as a property of the transmitter and returns to the domain of matching. If anyone wants to constrain the entire crusade of the rereflecting transmitter to the tube set feeding ladder line - then feel free to do so. However, I don't think I've ever seen a mobile tube rig feeding ladder line - no doubt one day I will. We will probably talk about efficiency. :-) 73's Richard Clark, KB7QHC |
#7
![]() |
|||
|
|||
![]()
On Mon, 06 Jun 2005 15:05:43 GMT, "Henry Kolesnik"
wrote: Please tell me more about melting the finals and a bit more explanation of what was happening? Hi Hank, Direct observation offered a glowing plasma between the filament and the plate. It was football shaped rather than beam-like or an amorphous cloud. One point of the football touched the cherry red plate. Following a quick power-down, that point on the plate did not exist anymore as there was a hole. Couldn't really tell, but no doubt the grid suffered just as much in its own way. I suppose plates have become more robust over the years since that amazing demonstration. I helped fix one friend's Amp when it failed along with his antenna (or t'other way round as the chain of causality would suggest). His Amp simply quit working suddenly during bad weather. Fuses checked - OK. No interlocks were open - OK. The tube looked good at a glance - OK. HV Supply looked good - OK. The filaments failed to light up - odd, but consistent. Time to crack open the case. Pulled the tube and measured its filament continuity - OK. Measured filament supply - OK. Things were really getting strange. Time to bust the chassis open and really look. There on the baseplate were several small pools of solder in a circular pattern - how odd. Close scrutiny of connections revealed bright and soldered wires to everything - OK. Time to look at the tube again. Every pin was solder free - that was on the chassis base plate. [dirge played here] The filaments' wires were making enough contact to measure continuity, but no where enough to support real power. In other tubes I've seen the heat become so extreme that the glass envelope slumped into the vacuum and enclosed the plate structure like taffy. This didn't even crack the glass (or it had simply re-fused). Tube still worked afterwards though (so I would suppose the glass never cracked). One occasion was actually due to a bias problem created when the cathode load shorted. Lack of bias protection sent the circuit into massive conduction. Of course the short came about because of an initial excessive conduction (surprising in its own right because the common failure mode is to open). I've also seen stressed thyratrons so mismatched that they filled the workspace with their purple glow like a floodlight. Thankfully fuses work as I did not want to be near that final testimony. Now, that was the short list of Bottle failures. I have another list of melted state failures too, but their evidence is usually better hidden and less dramatic - heat sinking generally spreads the risk, so to speak. And speaking of heat sinks, I've drawn a number of blisters from those that normally only warmed my hand. Note there should be emphasis on normally warm and the obvious contradiction with blisters. Experience with failure has strongly correlated with heat and mismatch. Heat was born by resistance. Resistance is part of life and amplifiers. Heat comes in two forms. Slow-like, which is generally current based; and sudden, which is generally voltage based. I've felt along heatsinks immediately following failure that were as cool/tepid as usual, or ominously cooler! The sudden heat of arc-over in silicon can destroy just as effectively as the long slow broil of a plate turning to slag. Every mismatch in the Amateur experience is a probablistic spin of the wheel of misfortune. Sometimes the wheel stops on the slow bake that aborbs into heatsinks and you notice unusual smell, or your fan running on too long - Quick! do something, and you survive. Other times there's the snap of finality. Both of these examples are for those with keen senses, and often failure comes as a whimper. Most suffers usually discover what matching is for, even if they don't know how it works. 73's Richard Clark, KB7QHC |
#8
![]() |
|||
|
|||
![]()
Richard Clark wrote:
Every mismatch in the Amateur experience is a probablistic spin of the wheel of misfortune. Sometimes the wheel stops on the slow bake that aborbs into heatsinks ... Current maximum, Ifor+Iref in phase. Vtot = |Vfor|-|Vref| Other times there's the snap of finality. Voltage maximum, Vfor+Vref in phase. Itot = |Ifor|-|Iref| -- 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 =--- |
#9
![]() |
|||
|
|||
![]()
Richard
I've seen 3-500Z where the solder had melted out of the filament pins. I have some 811 from my 30L-1 that have holes in the plates, they still work quite well. It's been 15 years since I recall finding the holes in the plate sides and replacing. In additon I can't recall the reason for the holes but it had to be either 1. overdriving (which I don't think I did, 100 watt Icom) 2. high swr which I know has been over 10 to 1, but I can't see how that could do it.. 3. Light loading But in any event for something to melt we need dissipation and only resistance can do that! -- 73 Hank WD5JFR Still learning, un-learning and re-learning |
#10
![]() |
|||
|
|||
![]()
On Mon, 06 Jun 2005 20:52:52 GMT, "Henry Kolesnik"
wrote: But in any event for something to melt we need dissipation and only resistance can do that! Hi Hank, Unfortunately as much as you and I agree on that bedrock principle, others with Simpson Ohmmeter in hand would glare goggle eyed at us and say that plate has no resistance to speak of and that no amount of current through its Ohmic resistance could ever bring about enough heat to produce the effects so obviously witnessed. One of the most enraging questions I've asked "If it is not the value I've offered, what value is it?" Well, I've never been given a quantitative answer, however I've seen enough carefully crafted mathematical proofs in this group to replace substantive results so easily seen. There is some irrefutable logic in circulation that clearly reveals that what we've experienced just couldn't be. Glasses will be need to be readjusted for such extreme myopic aberrations. There are two principles involved in what is called Plate Resistance, and the first and foremost is not even related to the plate at all. It is called the work function of the cathode emissivity. So, in fact it is more proper to refer to this usual loss as Cathode Resistance, not Plate Resistance. The cathode is the fundamental limit on power generated. What Plate Resistance is, is the ill termed substitution for Plate dissipation. If folks want to work their Simpson, they would blow an aneurysm trying to measure the resistance from cathode (filaments have the same work function issue too) to plate. In fact, the hobby horse argument of it is not resistance at all, but some figurative charting artifice called a "load line" usually appears in the last gasp. Plate Dissipation is resistance clear and simple in spite of the failure of conventional tools to measure a common physical property. Newton would have recognized it, it is called inertia. Once the work function is overcome (the job of the grid), then Plate voltage dominates through the acceleration of charge beyond the grid, toward the plate. That stream of electrons (and there is no doubt about actual current flow in easily counted, significant populations of electrons) is elevated to 90% the speed of light. This current flow is entirely different from what current flows in the remainder of the Plate load. That is also known as displacement current and electrons are shuffling along at a placid meter per second rate. Plate current and displacement current are equal in amplitude and phase, but not in motion nor kinetics. NOW. When that same stream encounters the Plate - WHAM! If anyone here has walked into the wall, and NOT encountered resistance, then we will call you Casper. Inertia reveals that to slow a mass in a distance results in acceleration (negative in this instance) and that property is called Force. Force over time expends calories and is expressed in any number of systems and units - Watts is one, Degrees is another. We could abstract to Horsepower and Candelas (the plate glows too). We know the speed, not many here would give it much though, but none would know the length interval of going at that speed to going zero (0). It is roughly two atoms distance into the metal of the plate. I will leave those calculations of Force to the student to compute or I can provide it from notes of correspondence with Walt Maxwell and Richard Harrison from a round robin discussion several years ago. Hank, does this fulfill your earlier question as to "what" is happening? I first gave you many examples, I hope this segue into real physics fills in their actuality. Too many correspondents demand that I open the source and point at a 50 Ohm carbon composition resistor that is the "source resistance." 73's Richard Clark, KB7QHC |
Reply |
|
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
Questions -?- Considering a 'small' Shortwave Listener's (SWLs) Antenna | Shortwave | |||
Building a Matching Transformer for Shortwave Listener's Antenna using a Binocular Ferrite Core from a TV type Matching Transformer | Shortwave | |||
Question...mobile antenna "thinking out of the box"... | CB | |||
Help Please! Extremely Poor Reception In Turkey | Shortwave | |||
Poor quality low + High TV channels? How much dB in Preamp? | Antenna |