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#1
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On 25 Oct, 09:38, Cecil Moore wrote:
art wrote: At first I was considering the actual wire length in the braiding b ut that influence became little compared to the current pertabutations. Sounds like you are working on a self-resonant coil and need to know the length of time for the current to flow from end to end. Both sides of the argument are wrong on that one. The current does not jump from one end of a coil to the other in a very small number of nanoseconds as one "expert" has asserted which implies a VF close to 1.0. Neither does the current follow the wires directly round and round the coil as asserted by the other side which would imply a VF around 0.01. The actual measurable VF of a coil seems to be just about double the round-and-round argument side as there is indeed some coupling between adjacent coils. A typical 75m Texas Bugcatcher 6" dia, 6.5" long, 4 tpi coil has a VF of around 0.02 making it about 40 degrees long at 3.8 MHz. -- 73, Cecil http://www.w5dxp.com No Cecil you are following a fatal aproach by using lumped loaded circuitry which is a no no when measuring current speed. Especially when you are following a path of zero standing waves. To obtain a voltage doubling you can only solve by using distributed loading aproach where a single wire has approx length when measured close to the ground short of two wavelengths . Unfortunately by using braid to get extra current perbutatation the length extends quite a bit longer even tho braiding electrical length is longer that the physical measurement. Ofcourse the introduction of a flyback transformer would be exciting but we must not run before we walk Regards Art |
#2
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![]() "art" wrote in message ups.com... On 25 Oct, 09:38, Cecil Moore wrote: art wrote: At first I was considering the actual wire length in the braiding b ut that influence became little compared to the current pertabutations. Sounds like you are working on a self-resonant coil and need to know the length of time for the current to flow from end to end. Both sides of the argument are wrong on that one. The current does not jump from one end of a coil to the other in a very small number of nanoseconds as one "expert" has asserted which implies a VF close to 1.0. Neither does the current follow the wires directly round and round the coil as asserted by the other side which would imply a VF around 0.01. The actual measurable VF of a coil seems to be just about double the round-and-round argument side as there is indeed some coupling between adjacent coils. A typical 75m Texas Bugcatcher 6" dia, 6.5" long, 4 tpi coil has a VF of around 0.02 making it about 40 degrees long at 3.8 MHz. -- 73, Cecil http://www.w5dxp.com No Cecil you are following a fatal aproach by using lumped loaded circuitry which is a no no when measuring current speed. Especially when you are following a path of zero standing waves. To obtain a voltage doubling you can only solve by using distributed loading aproach where a single wire has approx length when measured close to the ground short of two wavelengths . Unfortunately by using braid to get extra current perbutatation the length extends quite a bit longer even tho braiding electrical length is longer that the physical measurement. Ofcourse the introduction of a flyback transformer would be exciting but we must not run before we walk Regards Art Art I think you cannot rely on calculating the braided length as being longer than the physical length. While it is true that the braided wire if unravelled would likely be considerably longer, RF waves propagate along the surface of the wire. They will jump from one wire to the next where the braids cross, following the path of least resistance. You would probably need to use braided Litz wire, where each strand is individually enamelled to achieve what you appear to be trying to do. Regards Mike G0ULI |
#3
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On 25 Oct, 11:32, "Mike Kaliski" wrote:
"art" wrote in message ups.com... On 25 Oct, 09:38, Cecil Moore wrote: art wrote: At first I was considering the actual wire length in the braiding b ut that influence became little compared to the current pertabutations. Sounds like you are working on a self-resonant coil and need to know the length of time for the current to flow from end to end. Both sides of the argument are wrong on that one. The current does not jump from one end of a coil to the other in a very small number of nanoseconds as one "expert" has asserted which implies a VF close to 1.0. Neither does the current follow the wires directly round and round the coil as asserted by the other side which would imply a VF around 0.01. The actual measurable VF of a coil seems to be just about double the round-and-round argument side as there is indeed some coupling between adjacent coils. A typical 75m Texas Bugcatcher 6" dia, 6.5" long, 4 tpi coil has a VF of around 0.02 making it about 40 degrees long at 3.8 MHz. -- 73, Cecil http://www.w5dxp.com No Cecil you are following a fatal aproach by using lumped loaded circuitry which is a no no when measuring current speed. Especially when you are following a path of zero standing waves. To obtain a voltage doubling you can only solve by using distributed loading aproach where a single wire has approx length when measured close to the ground short of two wavelengths . Unfortunately by using braid to get extra current perbutatation the length extends quite a bit longer even tho braiding electrical length is longer that the physical measurement. Ofcourse the introduction of a flyback transformer would be exciting but we must not run before we walk Regards Art Art I think you cannot rely on calculating the braided length as being longer than the physical length. While it is true that the braided wire if unravelled would likely be considerably longer, RF waves propagate along the surface of the wire. They will jump from one wire to the next where the braids cross, following the path of least resistance. You would probably need to use braided Litz wire, where each strand is individually enamelled to achieve what you appear to be trying to do. Regards Mike G0ULI- Hide quoted text - - Show quoted text - I see where you are coming from but braid wicks like mad so a good dose of quick drying polythene varnish solves that problem IF it were to occur, tho the current will not jump but follow the path of resonance. What I am doing now is a combination of insulated wire with doped braiding and it appears so far that the braid is required to be much longer. When time permits I will make seperate models using wire and then with braid on a higher frequency where the single wire form is easily calculated as a datum As far as Litz wire goes there is a frequency transition line when you use that (skin factor) so I am not anxcious to introduce another variable or spend the required extra money. Regarding travelling on the surface of the wire I have often pondered that the use of braid for grounding wire is subject to question compared to a copper wire or ribbon. As I see it the braid is heavily inductive even tho it has the appearance of the field balancing out since the current must still traverse the windings, but that is another subject all together deserving of its own topic title. I know it may sound wierd but I am trying to slow down the current by half so that for the tank circuit I will have four pulses of energy release over the existing two.Single wire windings are just a hair to fast to accomplish that In other words double the power of a particle generator which is what radiation is all about, at least in my mind, since I see the attributed gain of a helix being controlled by the voltage increase in sync with the current flow which I see as not quite correct when using single wire since. I am still seeing standing vaves which are small but does not prevent full traverse of all amateur frequencies using a single antenna with a variometer for use when resistance levels drop below 20 ohms. It just blows my mind how just applying a time varying field to a static field is providing so much more info with respect to radiation assuming one has a true understanding of what equilibrium is really all about and which the majority deride Cheers Art. KB9mz |
#4
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art wrote:
No Cecil you are following a fatal aproach by using lumped loaded circuitry which is a no no when measuring current speed. Nope, I'm arguing against that approach, Art. Some "experts" seem to like lumped load concepts but not I. Dr. Corum warns against using lumped load concepts for large coils and I agree with him. -- 73, Cecil http://www.w5dxp.com |
#5
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On 25 Oct, 12:45, Cecil Moore wrote:
art wrote: No Cecil you are following a fatal aproach by using lumped loaded circuitry which is a no no when measuring current speed. Nope, I'm arguing against that approach, Art. Some "experts" seem to like lumped load concepts but not I. Dr. Corum warns against using lumped load concepts for large coils and I agree with him. -- 73, Cecil http://www.w5dxp.com Good for him. It appears that constant use of lumped circuit analysis is gaining more votes against true science of today especially in amateur radio. Soon it will be promoted to a Law disregarding that it is only theory based. Something akin to a poll Regards Art. |
#6
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![]() Umm a velocity factor of .50 might be attainable with a variation on leaky coax... Some of the cheap stuff is already as slow as .66... Off the top of my pointy head braided wires wrapped on your form (same as you are currently doing) then potted in an appropriate dielectric material for filling the braid interstices should slow things down some more... The question extant is what material for potting (or for adding to your potting resin) will further slow progression of the wave front along the braid... We know that solid polyethylene dielectric on coax results in a lower vf than the foamed materials.. So it appears that denser material results in slower wave progression... Perhaps UHMW, or similar might suffice... Other thoughts come along, such as a flat ribbon with a deeply embossed pattern then filled with dielectric might be slower than braided wire... Or even a ribbon of screening material similarily filled... Dunno... Interesting problem... denny / k8do |
#7
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Denny wrote:
Dunno... Interesting problem... Not really - a helix can slow down a wave by a factor of 50 or more. Approximately a foot and a half of 75m Texas Bugcatcher stock will be self- resonant at 4 MHz. That's 90 degrees of antenna stuffed into about a foot and a half of coil. 90 degrees at 4 MHz is 61.5 feet. The VF of that coil is 1.5/61.5 = 0.024. Actually, pretty simple. -- 73, Cecil http://www.w5dxp.com |
#8
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On 25 Oct, 14:47, Cecil Moore wrote:
Denny wrote: Dunno... Interesting problem... Not really - a helix can slow down a wave by a factor of 50 or more. Approximately a foot and a half of 75m Texas Bugcatcher stock will be self- resonant at 4 MHz. That's 90 degrees of antenna stuffed into about a foot and a half of coil. 90 degrees at 4 MHz is 61.5 feet. The VF of that coil is 1.5/61.5 = 0.024. Actually, pretty simple. -- 73, Cecil http://www.w5dxp.com Yes Cecil I see where you are coming from but and it is a big but the turns must be exposed to radiate and it is that that one must not lose sight upon Art |
#9
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![]() "art" wrote in message ups.com... On 25 Oct, 14:47, Cecil Moore wrote: Denny wrote: Dunno... Interesting problem... Not really - a helix can slow down a wave by a factor of 50 or more. Approximately a foot and a half of 75m Texas Bugcatcher stock will be self- resonant at 4 MHz. That's 90 degrees of antenna stuffed into about a foot and a half of coil. 90 degrees at 4 MHz is 61.5 feet. The VF of that coil is 1.5/61.5 = 0.024. Actually, pretty simple. -- 73, Cecil http://www.w5dxp.com Yes Cecil I see where you are coming from but and it is a big but the turns must be exposed to radiate and it is that that one must not lose sight upon Art try a ctha that may do what you want. |
#10
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art wrote:
Yes Cecil I see where you are coming from but and it is a big but the turns must be exposed to radiate and it is that that one must not lose sight upon I can only wish that my 75m Bugcatcher coil had all of its losses going into radiation. :-) -- 73, Cecil http://www.w5dxp.com |
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