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Parameter Variation Machines With focus on EPD FQToEW, JF Murray, Manelstam & Papalex
Hello everyone,
I am starting this thread in the hopes of creating a space where everyone who is interested can INELIGIBLY discuss Mr. Dollard's Four Quadrant Theory of Electric Waves, James F Murray's Lectures & Patents along with L Mandelstam and N Papaleksi written works. Along with pertinent references by CP Steinmetz and Oliver Heaviside. SPECIFICALLY, I would only like people to talk about PARAMETER VARIATION MACHINES or other devices that pertain to the concepts and understandings of the PEOPLE LISTED ABOVE, while other people and devices can be brought up, I feel the people listed above are the best source of information on the main subject and subsequently why I feel this thread should adhere to their works. Furthermore my personal explanations and usage of mathematics will be in accordance with the jargon and symbolic representation given by CP Steinmetz & Mr. Dollard in his written works through Borderland Science and more recent "transmissions" posted here on the "energetic forum", which regrettably may cause a language barrier for some. In my posts V & I will be replaced with e & E and i & I, terms Voltage and Current will be used when vagaries are sufficient to explain something or when e & E or i & I are merged one into the other, happens in quadrature waveforms (i.e. oscillations, forced or free). Eventually I would like to work into use, the versor math proposed by Mr. Dollard, but I don't plan on that happening very soon. Also, I will, when I get some more free time, put up a link to my Scribd account, where everyone can get the references and works of the people listed earlier. With that said, I am looking to keep things a bit more mathematically formal but at the same time have casual conversations. Which reminds me of a Talladega quote; "I like to picture Jesus in a tuxedo T-Shirt because it says I want to be formal, but I'm here to party". For what its worth, here's a reply I sent to a question Jpolakow asked me the other day, which got me interested in starting this thread. Quote:
Last edited by garrettm4 : 03-08-2012 at 05:23 PM. |
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Dave |
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Hey Garrett,
Recently, I purchased a digital storage oscilloscope that has waveform math functions and an xy display for use in determining the BH curve of the material in use. With this new equipment, it is much easier to determine what is going on in the circuit. I have revisited harmonic modulation and have been able to get some really good looking waveforms. However, I'm going out of town for a few days and won't be able to get anything posted on it until I get back. The only suggestion that I have to experimenters is to use a material with a highly square hysteresis loop and the power windings must be of a high magnification factor(ratio of energy stored to energy dissipated). Good luck, Dave P.S. Thanks for always taking the time to post everything in a very clear and organized manner. I don't have that kind of patience unless somebody is asking me for clarification. |
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Just wanted to pop in here and say that I will be coming back on-line next week and be able to contribute to this as well. The effect of negative resistance is of course as old as tubes.
There seems to be more than one way to "skin the cat" as they say. The capacitive plate and coil transformer setup I was working on has been producing very strange results and in digging into more texts and research I got to thinking about the ground side of the circuit, the plates either induce a negative resistance into the coil or the field induced within the self oscillation of the coil is the negative resistance, whats truly strange is that it's a passive component and thus a no-no from conventional theory. look into tube design and negative resistance, I'll get some titles together in a bit and post them up. |
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A while back I started a thread on this very topic, however I used solid state devices, both capacitive and inductive to achieve parameter variation. The information might be very relevant to what you guys are trying to accomplish.
Solid State Capacity switching Tube 2 - YouTube Charge conserving Capacitive Spring. Cheers, Andrew |
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Here is another interesting capacity switching device. What you see is a polar dielectric (water) which rearranges its polar orientation when a current flows through it perpendicular to the electric gradient created by the capacitor plates.
MOV03700 - YouTube |
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As promised, here is a bit of information about what I have been doing behind the scenes. It has not reached the stage of development that we are all seeking for yet, but it does provide some valuable insights to the beginning experimenter that could help save a lot of time.
First of all, let us examine what direction Eric Dollard has been pointing us towards. Examine the waveforms presented in the following diagram: ![]() Notice that the power wave, P, in watts has an unequal amount of area underneath the curve. In the first diagram, the energy is being produced (the negative area under the power wave is greater than the positive area under the power wave) and in the second diagram, energy is being consumed (the positive area under the power wave is greater than the negative area under the power wave). Analyzing the sinusoidal waves in the graph shows that if the circuit did not have the parameter variation denoted by the wave labeled x, it would exhibit an induction factor of 100% and a power factor of 0%, meaning that this circuit would be a purely reactive circuit, a very high if not infinite magnification factor. This graph clearly shows that under certain conditions of synchronous parameter variation that a negative power factor can manifest in a circuit, meaning that energy is being externally supplied from the varying parameter. Where does the energy come from? That is the million dollar question... As suggested by Eric Dollard, how do we construct a magnetic amplifier circuit to use as a means of synchronous parameter variation at the 2nd harmonic of the power wave? If you just simply connect up a circuit like this, complications will occur. ![]() The above circuit will have the following waveshapes where the function shown in black is the power wave (carrier wave) and shown in blue is the modulation wave: ![]() The above graph seems like it is suited to be the correct waveshape that we want for our modulation, HOWEVER, if you start taking DC inductance measurements for both polarities of ampere-turns in the control winding, you will see that the inductance of the power windings decreases with each half cycle of the modulation wave, giving 4 minimum inductance peaks rather than 2 as shown by Steinmetz's diagram above. A graphical representation can be seen below, inductance colored red: ![]() As can be seen by the series capacitor in the "Simple Second Harmonic Magamp Modulation Circuit", the modulation portion needs to be in resonance to effectively deliver enough current into the impedance (control winding) that will in turn deliver the ampere-turns of magnetism into the core. After many, many hours of trying every damn thing that I could to overcome this problem of the 4x inductance crests/troughs, I found a simple solution. Two identical control windings and a couple of diodes! So easy... ![]() *R4 is the 1 ohm resistor for current detection. This arrangement allows for unidirectional current only in the control winding of the magamp under study. It still doesn't have the sinusoidal shape that Steinmetz's has, but the inductance variation becomes isolated to only two out of the four quadrants of rotation. It has produced the best looking waveforms that I have seen on my scope to date. ![]() This configuration would be best used on a four phase electrical system. Then all diverted control winding current could be utilized to modulate another core, creating a balanced system. This sums up how I have been running my modulation experiments, and I'll be posting some data to accompany this when I can stand to sit down at the computer again. Until then... Dave Last edited by Web000x : 07-13-2012 at 01:39 AM. |
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This is the test circuit that the following data is based off of:
![]() *Note the capacitance in the diagram is not correct, for Moderate Modulation 10uF was used and for Heavy Modulation, 40uF was used. ![]() ![]() ![]() ![]() ![]() While this information is nothing to 'call home about', it does show some interesting features of the electrical circuit using synchronous parameter variation. First, take note that in heavy versus moderate modulation, it took less energy to coerce the energy into as a negative power factor than as a positive power factor, possibly opening up question to the Newtonian action/reaction idea. Second, notice how negatively biased the power factor is of the (red wave in the oscilloscope pics, figure 1 & 5) under proper conditions. Just imagine what might happen if a highly-square-hysteresis-loop core was being used. (The core under study was mapped out to be fairly round). Lastly, notice that you cannot just 'yank' the energy out with brute force, the heavy modulation was much worse than the moderate modulation as far as efficiency. There is obviously a balancing act with power consumption and core material. In my observations, I have found that if the carrier wave saturates the core before the modulation wave can saturate the core, the negative power factor will not manifest as strongly. The modulation wave must be the prime mode of core saturation or positive power sneaks into the mix. I'm sure I missed some relevant info so feel free to call me out. Good Luck, Dave Last edited by Web000x : 07-13-2012 at 03:10 AM. |
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Interesting Results
@All,
Sorry but it turns out that I had a connection issue going on that interlinked the two control windings. This interfered with the measurements which makes these results null and void. I didn't mean to get anybody excited... Dave Last edited by Web000x : 07-25-2012 at 01:38 AM. Reason: Data was not correct |
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Bifilar wound coils - switch series/parallel?
There appear to be interesting effects when using bifilar wound coils:
Tesla Bifilar Coil patent - Bedini Bifilar Coil usage in Schoolgirl Radiant Motor Charging devices | MERLib.org Quote:
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What is very interesting, is that there appears to be a stronger magnetic field when using bifilar coils, even when using D.C.: Bifilar Electromagnet Quote:
If these interesting effects indeed have something to do with inter-turn voltage differences, then this could be very useful in parametric variation machines, because the bifilar windings can be switched from series to parallel at will. In series, you get additional inter-turn voltages, which you don't get when switched in parallel... |
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http://www.tuks.nl/pdf/Reference_Mat.../US2953751.pdf And what seems to be an interesting book on the subject of magnetic amplifiers: http://www.themeasuringsystemofthego...amplifiers.pdf And a more recent one "On Magnetic Amplifiers in Aircraft Applications": http://kth.diva-portal.org/smash/get...312/FULLTEXT01 Magnetic Amplifiers - Principles and Applications Magnetic Amplifiers - Principles and Applications : Paul Mali : Free Download & Streaming : Internet Archive Update: There seems to be a lot of interesting information at DTIC Home Page Found these two papers by searching for "mandelstam papalexi", both from 2005: http://www.dtic.mil/dtic/tr/fulltext/u2/a435509.pdf INVESTIGATIONS OF PARAMETRIC EXCITATION IN PHYSICAL SYSTEMS http://www.dtic.mil/dtic/tr/fulltext/u2/a439353.pdf INVESTIGATIONS OF NONLINEAR WAVES AND PARAMETRIC EXCITATION Last edited by lamare : 07-23-2012 at 01:51 PM. |
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By switching either the bifilar strands in series, or one of the bifilar strands in series with the extra layer, one can modulate the inner-turn (or self) capacitance of the coil and switch this Tesla effect on of off at will. While one would theoretically expect the inductance to be independent of such switching, it would not surprise me if that would turn out not to be the case. Either way, such switching definitely modulates a parameter of the system... |
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Hi Andrew,
I found a reference to elnamagnetics where there may be a chance to get metglas cores or you can inquire for specific types: Elna Magnetics | Search Results Sorry if you have been aware of this already. I do not know them, have never ordered any from them. Gyula Quote:
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Asked a lecturer what he thought of the idea of changing inductance/capacitance and it's implications on the systems energy and he seemed to really like to idea say that the idea was really interesting (his emphasis not mine) and gave me great encouragment in my idea of making a generator based on parametric principals for my final engineering project. Unfortunately he didn't point me in the direction of anything interesting but he did think the idea was quite viable. Not that his word is gospel but it is good to get some input from them. I wonder if I'd be able to work something core wise out through university, I'll see what I can do. PS: Garrett do you have pdfs of those books you referenced on hathi-trust? If not I might be able to help you 'extract' them. PM me if interested, invitation goes to anyone for that matter. Raui |
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Already finished the Blackwell book, which I uploaded together with some other info I could find to my server: Directory contents of /pdf/Reference_Material/Parametric_Excitation/ Will upload the other two books in the coming days to the "Magnetic Amplifiers" section: Directory contents of /pdf/Reference_Material/Magnetic_Amplifiers/ Also renamed the "report" file I had on Mandelstam and Papalexi. This is a 60 page NASA translation of a 1935 article in Russian: http://www.tuks.nl/pdf/Reference_Mat...ion%201969.pdf This appears to be the paper referred to by Janssen in his "Investigations of Parametric Excitation in Physical Systems" (2005): http://www.tuks.nl/pdf/Reference_Mat...20-%202005.pdf Quote:
Janssen also discusses the Rotary Electrostatic Converter, which has actually been built in practive by Chris Carson based on Eric's theory: Quote:
Tuks Unsorted KieknWatTWordt Stuff : Energetic Form Posts |
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I contacted those guys first as they are a distributor for Hitatchi, but they referred me back to the parent company because all they had were very very small ones, for the larger ones I needed to go to the big guys, I got the run around for a very long time even though promising a possible purchase of over 10,000 which any salesman would jump on and send samples out for, even if I have to pay for the samples I would have done so. P.S. Raui.... Regular MetGlass cores are not what we want. I have several of those which are very nice indeed, (over 200$ a core) but the deal is that they do not have the square B-H loop we are looking for. We want a very small input to wildly change the inductance of the core, these are almost like the mosfets of magnetism. |
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Found a great resource on Mandelstam, Papalexi, etc.
This site has quite a lot of translations of the Mandelstam and Papalexi articles:
National ElectroDynamics, LLC : Translation Publications Currently uploading them to my archive: Directory contents of /pdf/Reference_Material/Parametric_Excitation/ |
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Maybe for just as a 'remote substitute' you could consider testing toroidal ferrite cores manufactured with square loop B/H curve. Ferroxcube has such and designates them as 3R1 material. Data sheet: http://www.ferroxcube.com/prod/assets/3r1.pdf Ordering is from Newark or Farnell TN36/23/15-3R1 - FERROXCUBE - TOROID | Newark This OD=36mm seems to be highest diameter, and there are smaller ones. rgds, Gyula |
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http://www.hitachimetals.com/product...magamp_opt.pdf From the data sheet they seem to have a decent b/h loop. I know that any old core will not do but I thought these cores would be suitable? Raui |
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Make that 4. I have contacted several dozen companies trying to get high permeability core material, and it's very difficult to get a response. One of these days I'll fly over to India (where the Metglas plant is) and go to the factory direct....
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There is a very interesting experiment I tried recently using a few cores I had laying around. which may solve the problem you are describing, and give some direction on how to use saturable reactor cores. This was basically the setup. However in one iteration I used a toroidal core which was split into two C sections with with a paper in-between to create a small gap. This setup is very similar to the Alexanderson setup, in that the two windings are not inductively coupled in the traditional sense. A change in B field with respect to time in one does not create an EMF in the other. Placing an alternating current through the black winding does not affect the red winding, until there is an external magnetic field applied. When the external field is applied it saturates to some degree the core. When the alternating current in the black winding around the toroid is excited, this changes the permeability of the core, thus affecting the B field that the red winding sees. Now you have an EMF generated, however this is more through the action of permeability affecting an external B field than through standard induction. What was interesting is that I found the cores to have a preferred frequency at which they couple the best. One core was only 200hz. With a gap in the core, the total inductance was less, but it could be switched faster. This is almost like a macroscopic version of NMR where we are looking at how the core as a single domain can respond to a "flip" b field orientations. If I were going to build a machine around these principles, i would find out the preferred characteristics of the core you are using, and build all else around this. |
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Hi Andrew,
Would like to know what is advantage of using C cores i.e. having a small air gap between the two C shapes? Without splitting a toroidal core, the same principle would work in a much less desirable way? Thanks, Gyula |
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You are playing two factors against each other however, one is that the overall inductance drops dramatically, and the other is speed of switching (deta T) giving rise to higher EMF. |
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Gestalt might possibly have found the material source that will really bring the theme of this thread to life. Check out the BH curve of this material:
![]() It has a high saturation, low coercive force, and it is available in ranges from 12 to 2400 Volt-Ampere Cores, the most expensive core being $68. Silicon Steel Toroidal O-Cores - In Stock I ordered two of the 300-600 VA units so we'll see. Dave |
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Found a better way of downloading the books from the University of Michigan. First, I downloaded images, but I can also download the books in pdf format, albeit page by page, which gives a much better quality. It doesn't like downloading more than 1 page a minute or so, so it took quite some time to download the three books by Platt, Lynn and Blackwell.
So, I updated these three books on my server and also added Minorsky's "nonlinear oscillations" from 1962, which appears to be an excellent book and includes some of his work om parametric excitation based on Mandelstam and Papalexi: http://www.tuks.nl/pdf/Reference_Mat...20-%201962.pdf Further, it seems to me that the circuit known as "the Tesla switch" is also supposed to be a parametric variation device, a solid state version of Cap's Parametric Electric Machine: http://www.tuks.nl/pdf/Reference_Mat...0US4622510.pdf This one has also been built by Chris Carson: Tuks Unsorted KieknWatTWordt Stuff : Energetic Form Posts If you can get such an "electrostatic converter" working by mechanically changing the capacitance of an LC oscillator, one should also be able to do this solid state, by switching the capacitor in series/parallel and thus modulating the capacitance that way. When you want to use large capacitances and thus would like to use polarized electrolytic capacitors, it seems to me that the Tesla switch circuitry may use 4 capacitors instead of 2 in order to avoid problems with electrolytic caps being charged negatively. If this is correct, one should adapt the switching frequency to the natural LC resonance frequency of the circuit, and the "on time" of each of the series switches should be 25% of the whole cycle. Macpherson describes this cycle in his book (page 15 and on), whereby the modulation (==switching in the Tesla switch) of the capacitor, the "pumping", needs to occur at twice the natural resonance frequency of the system: http://www.tuks.nl/pdf/Reference_Mat...20-%201964.pdf Last edited by lamare : 07-30-2012 at 09:03 AM. Reason: updated link to Minorsky's book |
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