Bedini-Lindemann 2013 Science & Technology Conference

Bedini SG - The Complete Intermediate Handbook

Energetic Forum  

Go Back   Energetic Forum > Energetic Forum Discussion > Renewable Energy
Homepage Energetic Science Ministries Register FAQ Calendar Search Today's Posts Mark Forums Read

Renewable Energy Discussion on various alternative energy, renewable energy, & free energy technologies. Also any discussion about the environment, global warming, and other related topics are welcome here.

Reply
 
LinkBack Thread Tools
  #1 (permalink)  
Old 03-07-2012, 11:00 PM
garrettm4's Avatar
garrettm4 garrettm4 is offline
Member
 
Join Date: Oct 2010
Location: Orbiting Sol somewhere in the Milky Way
Posts: 79
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:
John,

Thanks for the excellent question.

To give a decent answer would take up a lot of time and writing space, I am planing to start my own thread on the forum for more Technical discussion and advancement of Eric's Four Quadrant Theory of Electric Waves focusing on parametric machines and the mathematics used in their design.

But in a nitty gritty summary I would say that the Usage of E e I & i gives rise to the understanding of what is going on at any one moment in time, at any one place in time (in a circuit), such as the direction of vector forces, are they becoming a zero magnitude, do they add, subtract or orthogonally interact, what is the phase difference due to the hysteresis of the fields of Dielectric & Magnetic induction B & D to the applied fields of force E/G & H, what is the consequence of this on the Electric Field Flux Q (poyning vector S).

The beauty of what Mr. Dollard is all about is in looking at the micro and macro views along with distributed and lumped element analysis with views that voltage and current are composed of separate time-variant and time-invariant components, also the notion of versor operators is an amazingly useful tool, once understood, much like linear algebra or calculus.

Furthermore the insight that if there are losses in a circuit (specifically ones that produce heat) then the reverse instance must be true as well, or a GAIN in circuit power (from cooling) or an alternative Loss that doesn't accompany any accountable heat. This seen as a door way for Work or Power into and out of the circuit. NOTE THAT I DO NOT USE THE WORD ENERGY. I, counter to Mr. Dollards beliefs, believe energy is always conserved from the source, BUT WORK and subsequently POWER do not always have to be in proportion of the relative energy used of the source.

This may read off like a bunch of incoherent rambling, but instilled are a few of the things I like about Mr. Dollard's concepts and theory, with out all the formalism needed to be exact. I hope you get something of value out of it.

Garrett M
Garrett M

Last edited by garrettm4 : 03-08-2012 at 05:23 PM.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
Sponsored Links
  #2 (permalink)  
Old 03-08-2012, 02:55 AM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
Hey Garrett,

Thanks for starting this thread. I do not plan on becoming too active in discussion since I have experiments to run but figured that I would show some promising results regarding parameter variation. I have built a machine that consists of two alternators and a prime mover. The alternators are spinning at a ratio of 1:2 to give me a primary frequency and the 2nd harmonic of that frequency as per the instructions of Manelstam & Papalex, E.P. Dollard, and Steinmetz.

I am only using junk parts for my magnetic amplifier. It consists of laminations carefully chiseled away from a microwave oven transformer to equal roughly the same density as the iron in my alternator. The power windings of the magamp have been matched to the copper for a single phase in the alternator.

When I modulate the inductance of the magamp's power winding at the correct phase angle via the control winding, I get a waveform that looks like this:


Sorry about the small picture but I don't have time to go back and make it better.

Notice the positive power (Ei) relations versus the negative power (-Ei) relations. They seem to be of approximately the same as far as the energy storage and the energy return goes. The noteworthy component is the 1.5 ohms worth of resistance that the current is "flowing" thru each time, lighting the car headlamp to a brightness that I don't like to stare at. This is all being done for 13 watts worth of modulation from the 2nd harmonic wave which has much more room for increases in efficiencies.

By no means have I analyzed this as extensively as one would need to for a thorough scientific analysis, but it sure is interesting to see the beginnings of what has been proposed by the pioneers.



Dave
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #3 (permalink)  
Old 03-08-2012, 02:08 PM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
Quote:
Originally Posted by garrettm4 View Post
Dave,

What I find very interesting in your demonstration, is that the MMF waveform, during the "spike portion", is always in opposition of the applied EMF, that would imply that you are having a reversal in the power factor or a PF of +1 abruptly changing to a PF of -1 during a portion of the waveform period, presumably during the modulation of inductance from the MagAmp. Yes, the power factor is changing from +1 to a - 1. If you integrated the Ei waves, you would see that there is approximately the same amount of energy occurring in the positive region as well as the negative region. Since there is real power being dissipated as heat in the resistor, I believe that the resistive element, R, and the receptive element, H, are of equal magnitude and opposite polarity, thus delivering real power while the circuit looks like a +j reactive circuit with a PF of zero. That of course is if the probes are connected correctly, if you were to flip the orientation of the oscilloscope probes it would invert the waveform. The probes are connected so that when the magamp modulation is ceased, the current is shown to lag the EMF or it is shifted towards the right side of the CRT BUT it would seem that the MMF, before the modulation of inductance takes place, going through the 1.5ohm resistor is mostly in phase with the EMF with a slight phase shift from the small relative inductance of state L0, this would imply that the probes are connected properly. An interesting experiment to perform, would be to try to remove work from the system, by modulating to a maximum inductance when MMF is at its lowest and reduce the inductance to a minimum when the MMF is at its maximum. This would show you that the circuit is working as well, but in a bizarre state of loss of work that is conventionally uncountable for. Something else to look for is the quantity of heating or cooling of the iron core of the MagAmp. I have yet to see any signs of consumption or the destruction of energy with no accompanying heat loss, but that is due to the fact that I am severely underfunded in my experiments and do not have wattmeters that need to exist in several places in the circuit. The cooling of the magamp would confirm some of the stuff that has been confusing me about John Bedini's claims.

I have a few questions if you would like to answer them. One, how are you modulating the inductance of the MagAmp, more specifically what type of waveform are you using and what is (if you want to divulge) the design of the MagAmp magnetic circuit structure. The magamp control winding is being modulated with the 2nd harmonic alternator's sine wave. In order to get any sort of effect, I had to bias the 3 legged core (Power windings wound in opposite direction on the outer legs and the control winding in the middle) with two large neodymium magnets. Otherwise, the power windings were seeing a minimum inductance four times per one time period of the primary frequency.

I might be able to lend some assistance in your design if your interested. Personally I have found a square wave control signal to be very UNNATURAL and to cause lots of EMI noise. Subsequently a sine wave gives much more natural power waveforms. I am not here to be a hero. I want to see a better future. Any advise that you can offer will be taken into account.

Furthermore the excerpts I posted of Jim Murray's 1990 & 1983 articles are VERY VERY important to read. Convert all the mechanical analogies he gives to terms of electrical circuits and you will see some amazing insight into your experiment. Knowledge of calculus is highly recommended in grasping what he means by "constant", "linear" and "nonlinear", remember there are always two plots, differentiation and integration, the relationship of the two is what he is referring to. I have always felt that the Veljko Milkovic 2 stage mechanical oscillator was indeed a mechanical analog of successful energy amplification via parameter variation. I tried to look into Jim Murry once but the page didn't load correctly so I got distracted by something else. I'll look into it.
Obviously my response is in red. I just finished a new control winding of twice the number of turns as well as a bigger wire gauge so I am about to see what happens when I get more magnetism into the control winding. I have a feeling that this material is crap for this type of work because I plotted the inductance versus the control winding ampere turns and it never quite fully saturates as Mr. Dollard suggested.

Dave
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #4 (permalink)  
Old 06-30-2012, 05:23 PM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #5 (permalink)  
Old 07-05-2012, 03:26 AM
madhatter's Avatar
madhatter madhatter is offline
Senior Member
 
Join Date: Nov 2010
Posts: 427
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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #6 (permalink)  
Old 07-09-2012, 04:56 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #7 (permalink)  
Old 07-09-2012, 05:05 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #8 (permalink)  
Old 07-13-2012, 01:00 AM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #9 (permalink)  
Old 07-13-2012, 02:44 AM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #10 (permalink)  
Old 07-21-2012, 05:49 PM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #11 (permalink)  
Old 07-23-2012, 09:03 AM
lamare's Avatar
lamare lamare is online now
Senior Member
 
Join Date: Oct 2008
Posts: 1,173
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:
Figure 1 is a standard pancake coil (many Tesla coil builders are familiar with this style). Figure 2 is a bifilar coil, the crux of the patent is where Tesla winds a dual wire and then connects the ends in a series (an interesting experiment for coil builders).

Tesla explains that a standard coil of 1000 turns with a potential of 100 volts across it will have a difference of .1 volt between turns. A similar bifilar coil will have a potential of 50 volts between turns. In that the stored energy is a function of the square of the voltages, the energy in the bifilar will be 502/.12 = 2500/.01 = 250,000 times greater than the standard coil!"
Exotic Research | Vol 2 No 2 | New Generation of Radiant Energy Devices
Quote:
Tesla's US Patent No. 512,340- "Coil for Electromagnets"- is a very special coil design because, unlike an ordinary coil made by turning wire on a tube form, this one uses two wires laid next to each other on a form but with the end of the first one connected to the beginning of the second one. In this patent Tesla explains that the double coil will store many times the energy of a conventional coil.

Measurements of two coils of the same size and with the same number of turns, one with a single, the other with a bifilar winding, show differences in voltage gain. These bifilar coils can be explained solely on the basis of their electrical activity. A bifilar coil is capable of holding more charge than a single wound coil. When operated at resonance, the distributed capacitance of the bifilar coil is able to overcome the counter electromotive force (emf) normal to coils - inductive reactance.

Because of the electrical activity, a bifilar coil does not work against itself in the form of a counter - emf, the potential across the coil quickly builds to a high value. The difference between the turns becomes great enough that the energy is practically all potential, at this point, the system becomes an electrostatic oscillator.

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:
The same amount of voltage, from the same battery, produces twice as much energy in the bifilar wound coil as in the single wound coil. This is just one of the many techniques Nikola Tesla used to make his inventions highly efficient.

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...
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
Sponsored Links
  #12 (permalink)  
Old 07-23-2012, 09:18 AM
lamare's Avatar
lamare lamare is online now
Senior Member
 
Join Date: Oct 2008
Posts: 1,173
Quote:
Originally Posted by garrettm4 View Post

For some more fun reads on the subject (via HathiTrust) check out:

Self-Saturating Magnetic Amplifiers 1960 by Gordon E. Lynn

Magnetic Amplifiers, Theory and Application 1958 by Sidney Platt
There's also a patent by Lynn on magnetic amplifiers:
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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #13 (permalink)  
Old 07-23-2012, 01:28 PM
lamare's Avatar
lamare lamare is online now
Senior Member
 
Join Date: Oct 2008
Posts: 1,173
Quote:
Originally Posted by lamare View Post
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...
One could also think in the direction of adding a second layer on top of the bifilar wound coil, with the same number of windings.

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...
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #14 (permalink)  
Old 07-25-2012, 05:24 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
Quote:
Originally Posted by garrettm4 View Post
Andrew,

Thank you for sharing your information on the subject. I have avoided the variable dielectric circuits due to my lacking in funds and resources, but what you have presented gives me much excitement to pursue that route.

You may have already thought of this, and some A-hole will probably steal this idea, but for the sake of discussion I will give a basic outline of the idea you gifted me with you demonstrations.

If one were to unite a variable magnetic storage element with the variable water-capacitor, and then drive them from an outside source as an LC tank, with the proper phasing of the control signals, you would have a very efficient and possibly over-unity hydrolysis system.

If both elements exhibit a negative resistance/conductance characteristic that is greater than the average natural logarithmic decrement, the resonant oscillations would continue to grow until a breakdown in the water capacitor occurred or some other non-linearity in the circuit limited the growth.

However, if you balanced the total systems exhibited negative resistance (from parameter change) with that of the water capacitors shunted conductance (water conductivity), you would have minimal power supplied from the source supply, except for the control signals and other system losses.

In principal, it would work like an LC tank that canceled its own internal resistance/conductance. However, in a practical situation, you would need a small amount of positive resistance in the system to limit the magnitude of the oscillation, because if there is no effective resistance in the system, the oscillation will continue to grow logarithmically until something failed.
YOU have it 100% Absolutely correct, and its being built right now, along with Michael John Nunnerly's 185 percent above Faraday system. Another approach was to use two water capacitors isolated from each other in terms of conductance through the water, so one discharges and changes the capacity of the other in a flip flop fashion. Introducing Mag amp as a parameter changing device would increase this further if the phasing is right as you alluded to previously. Problem is it is VERY difficult to get mag amp cores of any significant size from anywhere. I have contacted Hitatchi metals one of the larger distributors several times. told them everything about research and development, used my company name as a guise which is a huge company, and they were very excited to supply them...Then I never heard back, lol. Now they wont answer or return emails or phone calls from me.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #15 (permalink)  
Old 07-25-2012, 05:45 PM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
Quote:
Originally Posted by Armagdn03 View Post
YOU have it 100% Absolutely correct, and its being built right now, along with Michael John Nunnerly's 185 percent above Faraday system. Another approach was to use two water capacitors isolated from each other in terms of conductance through the water, so one discharges and changes the capacity of the other in a flip flop fashion. Introducing Mag amp as a parameter changing device would increase this further if the phasing is right as you alluded to previously. Problem is it is VERY difficult to get mag amp cores of any significant size from anywhere. I have contacted Hitatchi metals one of the larger distributors several times. told them everything about research and development, used my company name as a guise which is a huge company, and they were very excited to supply them...Then I never heard back, lol. Now they wont answer or return emails or phone calls from me.
Yeah, I am starting to run into that problem too. Many of the emails that I send to the magamp core providers are never responded to...
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #16 (permalink)  
Old 07-25-2012, 07:39 PM
gyula gyula is offline
Senior Member
 
Join Date: Apr 2007
Posts: 639
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:
Originally Posted by Armagdn03 View Post
...
Problem is it is VERY difficult to get mag amp cores of any significant size from anywhere. I have contacted Hitatchi metals one of the larger distributors several times. told them everything about research and development, used my company name as a guise which is a huge company, and they were very excited to supply them...Then I never heard back, lol. Now they wont answer or return emails or phone calls from me.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #17 (permalink)  
Old 07-26-2012, 09:13 AM
Raui's Avatar
Raui Raui is offline
Senior Member
 
Join Date: Dec 2008
Location: New South Wales, Australia
Posts: 279
Quote:
Originally Posted by Web000x View Post
Yeah, I am starting to run into that problem too. Many of the emails that I send to the magamp core providers are never responded to...
I tried getting some custom metglas cores back at the start of the year when I had a bit of money to throw around and I never heard back so that makes 3 of us..dare call it conspiracy?

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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #18 (permalink)  
Old 07-26-2012, 11:22 AM
lamare's Avatar
lamare lamare is online now
Senior Member
 
Join Date: Oct 2008
Posts: 1,173
Quote:
Originally Posted by garrettm4 View Post
In the meanwhile, here's the first two pages of a book I have been reading regarding this general topic. While its oriented towards radio/microwave circuits, it is still definitely worth taking a look at.

Semiconductor-Diode Parametric Amplifiers 1961 by Lawrence A. Blackwell and Kenneth L. Kotzebue (compliments of HathiTrust)



For some more fun reads on the subject (via HathiTrust) check out:

Self-Saturating Magnetic Amplifiers 1960 by Gordon E. Lynn

Magnetic Amplifiers, Theory and Application 1958 by Sidney Platt
I found a way to download these books from HathiTrust. It takes a while for my computer to download all the individual images and make a pdf from it, but it works.

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:
In 1935 a Russian paper was published by L. Mandelstam, N. Papalexi, A. Andronov, S. Chaikin and A. Witt. The title of the paper was “Report on Recent Research on Nonlinear Oscillations”. In this paper, the authors discuss many types of nonlinear oscillations. One chapter is dedicated to parametric excitation of nonlinear circuits. I came across references to this paper two different times. Once was when professor Denardo mentioned that one of his books referenced it. The other time was when I was doing a Google search for parametric excitation. The website, The Tom Bearden Website (29 APR 05) seemed unreliable due to its content, which mostly consisted of claims for free energy without proof. I nevertheless decided to investigate the reference. I found a few more references to the paper on-line but no directions where to find it. After consulting with NPS librarian Michaele Huygen and searching many online resources of the library, I found a copy of the paper in English. The paper had been translated from Russian to French to English. The copy that I had found was produced by NASA Technical Translation.

Janssen also discusses the Rotary Electrostatic Converter, which has actually been built in practive by Chris Carson based on Eric's theory:

Quote:
B. THEORY OF A CAPACITANCE-MODULATED CIRCUIT

To modulate the capacitance of an LC circuit, we consider a bank of n parallel sectored plates, where every other plate is electrically connected, and where one set of plates is rotated (Fig. 10). This configuration amounts to n – 1 identical variable capacitors in parallel (n = 10 in Fig. 10).

Tuks Unsorted KieknWatTWordt Stuff : Energetic Form Posts
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #19 (permalink)  
Old 07-26-2012, 05:03 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
Quote:
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
Hello again!
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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #20 (permalink)  
Old 07-26-2012, 08:02 PM
lamare's Avatar
lamare lamare is online now
Senior Member
 
Join Date: Oct 2008
Posts: 1,173
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/
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #21 (permalink)  
Old 07-26-2012, 10:53 PM
gyula gyula is offline
Senior Member
 
Join Date: Apr 2007
Posts: 639
Quote:
Originally Posted by Armagdn03 View Post
Hello again!
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.
Hi Andrew,

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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
Sponsored Links
  #22 (permalink)  
Old 07-27-2012, 12:48 AM
Raui's Avatar
Raui Raui is offline
Senior Member
 
Join Date: Dec 2008
Location: New South Wales, Australia
Posts: 279
Quote:
Originally Posted by Armagdn03 View Post
Hello again!
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.
I remember reading on their site that they had cores for magamps, are these not suitable? I just did another quick search and found that I was directed to hitachi about these "square loop" metglas cores although last time I could view the information directly from the methods site. Are these the same cores you were looking to buy from hitachi: MAGAMP Square Loop Cores : Amorophous Products : Hitachi Metals America
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #23 (permalink)  
Old 07-27-2012, 02:15 AM
Gestalt's Avatar
Gestalt Gestalt is offline
Member
 
Join Date: Feb 2011
Location: Edmonton, AB
Posts: 46
Quote:
Originally Posted by Raui View Post
I tried getting some custom metglas cores back at the start of the year when I had a bit of money to throw around and I never heard back so that makes 3 of us..dare call it conspiracy?
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....
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #24 (permalink)  
Old 07-27-2012, 03:21 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
Quote:
Originally Posted by Raui View Post
I remember reading on their site that they had cores for magamps, are these not suitable? I just did another quick search and found that I was directed to hitachi about these "square loop" metglas cores although last time I could view the information directly from the methods site. Are these the same cores you were looking to buy from hitachi: MAGAMP Square Loop Cores : Amorophous Products : Hitachi Metals America
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
OH gotcha, yes they do have square loop cores, I thought you were referring to their normal amorphous ones which do not behave this way, sorry for misunderstanding.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #25 (permalink)  
Old 07-27-2012, 03:35 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
Quote:
Originally Posted by garrettm4 View Post
I was able to sample a core from MetGlas, this was before Hitachi took them over, and ironically the amorphous metal team were originally a division of Honeywell. I happen to know a guy who knows the guy who was over that division of Honeywell.

Strangely, the only saturable reactor sample, of which they were willing to send my way (paid sample or not), was a tiny little toroid; OD 25.658mm, ID 18.512mm, Ht 11.049mm. Which was of the amorphous alloy type 2714A, of which you can buy by the tape reel rather than the pre-wound toroids. (If I were to contact them again I would now ask for the tape reels as opposed to pre-wound cores. Thanes B Heinz seems to use the metal tape from these guys as well.)

The MP2410M4AS type 2714A alloy tape wound toroid, once received, was tested by myself to be fairly square and saturate quite easily. Cobalt based alloys seem to be superior to the nickle based alloys from what I have seen, low hysteresis losses and good squareness ratios.

Due to the small core I received, and the alloy used, it literally took milli-amps to effectively saturate the core, with the proper turn count or ampere-turn product. Important, you don't want the power winding to saturate the core for you! So for those who are going down this route (of using pre-made toroids), use the minimal ampere-turns tolerable for the power winding and as many cores as tolerable, connected in series or parallel. I have seen people stack multiple cores together as a single unit, which is another way to better utilize them. You want to run the reactor cores at about 70% or less of their saturation points on the power side and 100% on the control winding when its energized, this way the core actually looks like a stable inductance to the ac source when you aren't driving it.

Also, you may or may not need a non-saturable reactor in front of your saturable reactor, this is to limit the current in-rush from the end of the zero-crossing when the core is saturated, to the peak of the current node. The current magnitude allowed to flow through, when the reactor is saturated, is VERY important! This value needs to be LOWER than the saturating ampere-turn product or saturating current sheet value. As Dave has seen in his work, there is a sweet spot in setting the MAX current flow through the saturable reactor for excess energy return.

However there is no magic here, if the core remains saturated when the control winding is off (due to over current in the power winding), you obviously will get less than maximum energy back because there wasn't enough room to store the energy present let alone the energy the ferromagnetic material would have been able to impart from the artificial saturation by the control winding. So when designing a setup make ample room for the flux density of the power winding. This was something I found out the hard way, through much trial and error. So I hope this brief discussion helps someone achieve faster results and better success than what I was able to do.

I want to note, that with a mechanical parameter variation machine, built using standard grain oriented silicon steel, the operational characteristics are vastly different from a static satureable reactor using a cobalt or nickle alloy, don't confuse the two as to how they operate. Mr. Dollard has given a tour de force series of recent transmissions, "Law of Electro-Magnetic Induction", which in the latter parts describes the operational differences between the two distinct modes. Also, when employing higher flux densities, a mechanical unit might be more desirable than the static saturable reactor design, this from what I have seen on the bench. However, when operating at higher frequencies, the static saturable reactors are the better design. Each have their respective merits, so don't get hung up on one over the other.

One more thing, the Gorden E Lynn and Sydney Platt book references I gave, in a prior post, cover the static saturable reactor subject intimately. I highly suggest reading both of them before building a unit.

*On a side note, "ferro-electric capacitors" with a highly square hysteresis loop are the equivalent of a "dielectric magamp". The company that sold these parts in the USA signed an agreement with the USN (navy) that prevented them to sell any of their square loop ferro-electric capacitors to anyone but the USN. I don't want to say this is a conspiracy in the sense that people are being silenced, but realistically, AVAILABILITY is what's being regulated here. The same thing is seen with saturable reactors, the availability to customers is very limited and may most likely be under observation. Whereby the quantity sold and samples given by each company may have to be reported to some sort of "agency", what that hypothetical agency does with this information is beyond me. While I'm not in to conspiracies, it is interesting however, to see the correlations on the poor availability and also the possibilities these materials posses when used in an unorthodox manner, i.e. over-unity electrical systems.

Good Luck,
Garrett M

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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #26 (permalink)  
Old 07-27-2012, 05:56 PM
gyula gyula is offline
Senior Member
 
Join Date: Apr 2007
Posts: 639
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #27 (permalink)  
Old 07-27-2012, 07:59 PM
Armagdn03 Armagdn03 is offline
Senior Member
 
Join Date: Oct 2007
Posts: 853
Quote:
Originally Posted by gyula View Post
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
The advantage can be found in the explanation of Fly-back transformers. In essence you have two macroscopic domains rather than one, and the consequence is quicker release of the B field from its "locked" position. This is almost literally the opposite of the Permanent Magnet Holder by Ed Ledksakalnin.

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.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #28 (permalink)  
Old 07-28-2012, 04:24 PM
Web000x's Avatar
Web000x Web000x is online now
Senior Member
 
Join Date: Apr 2009
Posts: 455
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #29 (permalink)  
Old 07-28-2012, 05:13 PM
Gestalt's Avatar
Gestalt Gestalt is offline
Member
 
Join Date: Feb 2011
Location: Edmonton, AB
Posts: 46
Quote:
Originally Posted by Web000x View Post
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:
The problem with any Electrical Steel material is frequency. One of the core material reps informed me that if you are running it at anything much greater than >60Hz, you will begin having issues.
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
  #30 (permalink)  
Old 07-29-2012, 02:40 PM
lamare's Avatar
lamare lamare is online now
Senior Member
 
Join Date: Oct 2008
Posts: 1,173
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
Digg this Post!Add Post to del.icio.usBookmark Post in TechnoratiFurl this Post!Live Bookmark this Post!Google Bookmark this Post!Yahoo Bookmark this Post! share on MyspaceShare on FacebookTweet this thread
Reply With Quote
Reply



Thread Tools

Posting Rules
You may not post new threads
You may not post replies
You may not post attachments
You may not edit your posts

vB code is On
Smilies are On
[IMG] code is On
HTML code is Off
Trackbacks are On
Pingbacks are On
Refbacks are On



All times are GMT. The time now is 04:39 PM.


Powered by vBulletin® Version 3.6.4
Copyright ©2000 - 2013, Jelsoft Enterprises Ltd.
Search Engine Optimization by vBSEO 3.0.0 RC8
2007 Copyright ? Energetic Forum? A Non Profit Corporation - All Rights Reserved