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Re: secondary frequency problem (fwd)
---------- Forwarded message ----------
Date: Thu, 20 Sep 2007 19:58:55 -0700
From: Barton B. Anderson <bartb@xxxxxxxxxxxxxxxx>
To: Tesla list <tesla@xxxxxxxxxx>
Subject: Re: secondary frequency problem (fwd)
Hi Chris,
You've convinced yourself that classic TC's are built wrong? As you read
the CSN, keep in mind the application. Everything must be put into
perspective to the desired end result. For making "sparks", what we do
is perfect. Granted we do give them the nomenclature of a Tesla Coil. I
prefer "high voltage resonant transformer" since that is a far better
description and I think Bert Hickman actually was the first I heard
describe it as such.
As I mentioned, using DCR for Q is not accurate. But, sometimes
measurement is needed to prove it.
When your measuring frequency, drive the bottom of the coil with your
generator. Place a 5" wire in the scope probe and place it about a coils
length from the coil in mid air. Because you don't have a topload
installed, you may have to move it a little closer, but try to keep it
as far from the coil as possible. The ground side of the generator
should go to an artificial ground plane placed under the coil (I've even
used aluminum foil up until I found something better). Connect the scope
ground to the same place. And do it outdoors away from stuff.
A 555 will only get you to about 500kHz. I've only dealt with generators
for PWM applications (bread and butter stuff) for designing speed
controllers for motors. I don't have the experience with high frequency
in the MHz range. I usually stay away from the 555 unless I really need
to test something quickly. I usually use an opamp configuration in the
range of 5 to 20 kHz.
You might need to do some research to find a generator chip for the
frequency you want. The old ICL8038 won't do it. There might be
something newer out there these days? In the end, you might find it
easier to grab a signal generator capable of say 3MHz on eBay. That's
probably the easiest route.
Regarding the frequency; Javatc will likely pull out a 2.6MHz range
after all is said and done. This would put the 3rd harmonic near 860kHz
which is roughly what you thought. You should also see the 2nd lower
harmonic at 1.2 or 1.3 MHz.
For measuring Q you will need to provide a low impedance source (your
generator alone is too high). Terry Fritz designed and documented an
excellent low-z amp for just this purpose. I built one using his circuit
and use it for all my Q measurements. But don't cross that bridge until
needed. When your ready for the circuit just ask and I'll dig up the
files. The low-z amp will simply take the generator signal and convert
it to a low impedance output. There are a few various ways to do this,
but Terry's circuit is excellent and robust for this purpose.
Take care,
Bart
Tesla list wrote:
>---------- Forwarded message ----------
>Date: Thu, 20 Sep 2007 17:49:25 +0100
>From: Chris Swinson <list@xxxxxxxxxxxxxxxxxxxxxxxxx>
>To: Tesla list <tesla@xxxxxxxxxx>
>Subject: Re: secondary frequency problem (fwd)
>
>Hi Bart,
>
>
>
>>Wow, certainly a different coil than I had envisioned! 80 turns of 1/4"
>>wire with an 8" x 38" geometry is pretty cool and certainly the Q is
>>going to be high (higher than a typical coil).
>>
>>
>
>
>The coil I am designing is based on the CSN book based on what Tesla said.
>Though so far it turns out 100% backwards to how current classic coils are
>built. I have however convinced myself that classic tesla coils are built
>wrong, but I am keeping quiet until I can actually back it up with factual
>hardware ;-)
>
>One program calaculates the Q as 2,000. JavaTC about 1,000. Though saying
>that its not actually solid wire its coax cable so the surface area and skin
>effect may have a lower resistance. JavaTC assumes a solid wire so even so
>it probably will not be accurate for my coil anyway.
>
>
>
>
>
>
>>Regarding the 800kHz frequency: That indicates a lower 3rd harmonic of a
>>2.4MHz fundamental with a 2nd harmonic at 1.2MHz. The fundamental we
>>typically look at as a multiple of the fundamental (f) where the first
>>harmonic = 2 x f and it's amplitude is 1/2 of the fundamental. The 3rd
>>harmonic is 3 x f and it's amplitude is 1/3 the fundamental (and so on).
>>For lower harmonics, just divide with the same understanding and you
>>will find 800kHz is a 3rd lower harmonic.
>>
>>
>
>
>The odd thing is though, after 800khz the voltage gain just drops and drops
>until it gets to 2mhz (can't go any higher). going backwards from 2mhz it
>rises in voltage until you hit 800khz then it jumps, then starts to fall
>back down again... There is another small rise around 300khz also. I did not
>see anything past 800khz thats the odd thing.
>
>
>
>
>
>
>
>
>>I notice there is no ground plane inserted into Javatc (which "must" be
>>inserted for any type of accuracy). This is important. Also, any objects
>>around the coil will further lower the frequency (walls and ceiling
>>included). I like to test coils out in the middle of the yard where I
>>can remove as much external capacitance from affecting the measurement.
>>I also throw down a metal ground plane below the coil which I use as the
>>common signal ground (and I use it's dimensions as well for the ground
>>plane). Also, the bottom of the secondary is stated as 0. You should set
>>the actual bottom height value and then add 38" to that value for the
>>top height.
>>
>>
>>
>
>Thanks for pointing it out. I think it would be why it comes out higher than
>expected in frequency. It can be a tricky one to nail down but ballpark
>figures was all I was looking at.
>
>
>
>
>
>
>
>
>>Considering your 800kHz measurement and what you stated as a harmonic of
>>1.2MHz, I expect you are certainly in the 2.4Mhz range for the actual
>>fundamental frequency, but of course you can't measure that due to
>>equipment limitations. I run into those same limitations myself all the
>>time. One of my most frustrating times are frequency measurements
>>because I usually like to check the harmonics as well and often I can't
>>get past the 3rd harmonic.
>>
>>
>>
>
>
>Yes, its really annoying. I cruched it would work out pretty much at 2mhz,
>but at 2mhz there is no output there at all. I did try shuting the coil with
>100pf but the voltage rise was so small it was hard to get any real data
>from it.
>
>
>
>
>
>
>
>
>>Regarding AC resistance values from Javatc (and of course it's
>>associated Q value), there were hundreds of real world measurements in
>>which to compare. But Q measurements are difficult even for the most
>>experienced. Here's a quick chart of how Javatc held up against all
>>those measurements.
>>http://www.future-technologies.co.uk/temp/javatc.pdf
>>
>>
>>
>
>url typo there ? unless you have hacked my site and altered my files :P
>
>
>
>
>
>
>
>
>>Note that above h/d of 3, Javatc did very well for such a difficult
>>prediction, but below 3 the variation grew, yet still was in the
>>vicinity. These however are normal coil geometry's and wire size. Your
>>coil has a huge wire size for the coil geometry, so no telling since
>>it's so outside the norm. One thing I can say is true, don't rely on DC
>>resistances for Q. At RF, there "IS" an effect of resistance due to the
>>RF. Much higher than the DC resistance and especially in your case which
>>is going to have an incredibly small DC resistance. The AC resistance
>>will be at least 2 magnitudes greater at this frequency. Measure it and
>>you'll see.
>>
>>
>
>
>I've not measured Q before so will have a play once I got these other
>strange problems nailed down. It looks to me like Tesla used DC resistance,
>he always states less than 1ohm for a good Q, his Q factors in the order of
>10,000 or so according to his notes.
>
>
>
>
>
>
>
>>Anyway, I love coils that are truly out of the norm. Although ACR and Q
>>
>>
>
>This one will be for sure. Wait until you see the power supply behind it ;-)
>
>Its more of testing into Q factors, the norm is that it does not really
>matter, but I don't think it has been investigated correctly. Problems with
>high Q coils are high frequency, which needs a lower tank cap which results
>in less power thoughput or the need for 20KV+ drive voltages. Have already
>crunched over 100 pages of technical babble on it all.
>
>
>
>
>
>>is really an uncertainty, the remaining outputs are not related and
>>should be good. Just get the misc surroundings close and do the test
>>again far away from any objects (including the scope probe; position as
>>far away as possible) and you'll find Javatc will be really close to
>>measurement. I expect when doing that you'll find your 800kHz will
>>increase to about 870kHz indicating a fundamental near 2.6Mhz.
>>
>>
>>
>
>
>The freq may have been 850mhz not 800mhz, my bad for not making better
>scribbles on paper! May try and get a 555 to run at 3mhz. I think they do
>not go over 2mhz.. maybe if I run it on 50V and put a really big heatsink on
>it, it may work fast long enough to take readings ;-)
>
>
>Cheers!
>Chris
>
>
>
>
>
>
>
>>Take care,
>>Bart
>>
>>Tesla list wrote:
>>
>>
>>
>>>---------- Forwarded message ----------
>>>Date: Wed, 19 Sep 2007 07:21:32 +0100
>>>From: Chris Swinson <list@xxxxxxxxxxxxxxxxxxxxxxxxx>
>>>To: Tesla list <tesla@xxxxxxxxxx>
>>>Subject: Re: secondary frequency problem (fwd)
>>>
>>>Hi Bart,
>>>
>>>
>>>
>>>
>>>
>>>>2.7MHz is closer to 3 than 2. If you build a coil that with a
>>>>fundamental frequency at 2.7MHz (calc), then you must have some means of
>>>>driving it with 2.7MHz if using a signal generator and scope setup. If
>>>>you can't get past 2MHz on your generator, how can you say that it
>>>>doesn't ring at 2.7MHz? This must be an really small coil. Do me a
>>>>
>>>>
>>>>
>>>>
>>>Its going by other coils I have tested. normally just after the Fres the
>>>voltage just keeps falling. I would knock up a 555 circuit though I don't
>>>think they go past 2mhz. Saying that, If I was driving it on 800khz as a
>>>harmonic, then my voltage gain experiments will not be valid. My x17 would
>>>be based on the 800khz harmonic.... that's a good question, *is* 800khz a
>>>harmonic of 2.7mhz ?
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>>favour, send me a Javatc output so I can see the details. Your probably
>>>>just reading lower harmonics at the moment.
>>>>
>>>>
>>>>
>>>>
>>>http://www.future-technologies.co.uk/temp/javatc.pdf
>>>
>>>It looks like you fixed the DC resistance in the update too, I think last
>>>time it came out as 3ohms.
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>>A resonant transformer isn't a typical turns ratio transformer such as
>>>>an NST or other iron core transformer. This is a resonant transformer
>>>>where the output potential is a function of the resonant condition which
>>>>exist at the fundamental frequency. If you want to calc output, use the
>>>>capacitances or inductances as follows:
>>>>
>>>>Vout = Vin x sqrt(Cpri/Csec)
>>>>
>>>>
>>>>
>>>>
>>>Thanks for that. I know about the calculations, I am just doing some low
>>>voltage experiments just to collect some bits of data.
>>>
>>>
>>>
>>>
>>>
>>>
>>>>Typically, coil potentials range from 200kV to 500kV. Imagine if the
>>>>number of turns (pri and sec) were used. Say for example an average 1000
>>>>turn coil with 350kV output. This means the primary would have to have
>>>>350 turns! Can you imagine that? So, how do we get to 350kV with only
>>>>say 10 turns? The answer is resonance (or that point where the inductive
>>>>and capacitive reactances are minimum). At that point, we then get a
>>>>high current characteristic due to reduced overall impedance which in
>>>>turn provides the high output potential, so think of it as a function of
>>>>the coils reactances.
>>>>
>>>>
>>>>
>>>>
>>>I have in part been trying to get my head about it. I think of it as when
>>>the tank dumps its energy, it takes time to discharge. It creates a field
>>>which pumps the secondary. The longer the field is there more "time" the
>>>secondary is being pumped. However in order to pump efficiently they have
>>>to
>>>be in tune. Probably a few technicalities more to it, but its how I look
>>>at
>>>it.
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>>As far as the Q output? Way off for your coil I expect (and is why I
>>>>would really like to see your detail). Q is calc'd from the Fraga AC
>>>>resistance and it's this AC resistance which is probably off. The value
>>>>is usually good for coils greater than 3:1 h/d as stated in the help
>>>>output of Javatc. But, your coil I'm sure is small and there are no
>>>>actual Q measurements for a coil that small. If I were you, I would
>>>>ignore those two outputs and simply measure it yourself. Just click on
>>>>the Q text in front of the output box. I describe in the help file popup
>>>>how to measure Q. It is a difficult measurement as far as accuracy and
>>>>takes some practice. In my opinion, the greatest difficulty is equipment
>>>>resolution.
>>>>
>>>>
>>>>
>>>>
>>>Q seems a bit of a problem to me. I wrote my own calculator to crunch the
>>>numbers, though I used DC resistance for the Q measurement. I am not sure
>>>but I am sure Tesla used DC resistance for Q. He had factors in 10,000 or
>>>more. My coils is actually pretty large as you will see from the data.
>>>
>>>btw, as a suggestion, could the blue background be changed back to what it
>>>was before the update, I think it was a light grey. The blue is a bit
>>>harsh
>>>to the eyes and the red text turns into a bit of a blur. Sorry to be picky
>>>:P
>>>
>>>Cheers,
>>>Chris
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>>Take care,
>>>>Bart
>>>>
>>>>
>>>>
>>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>
>>
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