Selfrunning Free Energy devices up to 5 KW from Tariel Kapanadze

[cosmoLV]

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[stivep]

Biasing the core can be done with PM also, like this guy shows it in yt:
http://www.youtube.com/watch?v=pGOFNrlVm1Q
I see 2 LC circuits.
maybe the thin winding is a original winding from this tv deflection core.

@EMdevices .Why can not the ferrite rod be biased by a permanent magnet???

1.soft ferrite rods are used extensively in high energy storage designs, inductive components, antennae and RFID applications. They can also be used in components where temperature stability or large DC bias is required

2. bringing permanent magnet of high strength near ferrite will damage only cheap Chinese ferrite  but  it is time dependent that means that exposure time = demagnetization time factor( there is no time equality but time dependability)
http://www.overunityresearch.com/index.php?topic=237.0
I partially agree with that  statements from the link.


3.Materials that can be magnetized, which are also the ones that are strongly attracted to a magnet, are called ferromagnetic (or ferrimagnetic).


4.To demagnetize a saturated magnet, a certain magnetic field must be applied, and this threshold depends on coercivity of the respective material. "Hard" materials have high coercivity, whereas "soft" materials have low coercivity.
but
ferrite core demagnetization depends on size of grain(sand) metal oxide and bonding material thickness.

5.  A good permanent magnet can have a magnetization as large as a million amperes per meter...do not get confused  with that.. that is only analogy.

6.permanent magnet can lift up to 1000 times its own weight.

7.Ferrites: 800u permeability "J" type low-medium frequency ferrite rods of 0.62-inch diameter size. These are best for use in the frequency range between 10 KHz to 3 MHz


2000u permeability "T" type very low frequency ferrite rods of 0.845 inch diameter size. These are new 2nd generation solid core rods and are best for use in the frequency range between 0 Hz to 500 KHz.
2000u is a material that works at extremely low frequency, super low frequency, ultra low frequency, very low frequency, and low frequency.
http://www.stormwise.com/page26.htm
This link will give you  informations about ferrite (from HAMS)

http://docs.google.com/viewer?a=v&q=cache:nr0ZsrAbMnkJ:citeseerx.ist.psu.edu/viewdoc/download?doi%3D10.1.1.131.3545%26rep%3Drep1%26type%3Dpdf+Why+can+not+the+ferrite+rod+be+biased+by+a+permanent+magnet&hl=en&gl=us&pid=bl&srcid=ADGEESi38TyZjHKc1i3DBXf1PmC0fSwBB4VTSfrIsrtB1uOH8Z9C6p1_h4NLwTKU95xgqsXpcxjrqDcLHqY5Qw-m0rM2MVv6DyOLLh773SdH9hmNzr-oXhguIApIAgVXtIzGAxVFBvfD&sig=AHIEtbSdU6uJBqheMrGP3JmT8a1nvWfzww&pli=1

This link is abut antennas but explains bias.

8.Bias applied causes saturation it might be the way to control HV .
9. Saturation is always temporary stage till the material is permanently damaged
10. Saturation because of impedance change allow only little amount of  voltage to flow.

11. Quote from:
http://jap.aip.org/resource/1/japiau/v99/i8/p08M908_s1?isAuthorized=no

"Ferrite material properties may vary depending on the grade and manufacturer: there are differences between batches and also the production process may change in time. On the other hand, in power applications, the usual voltage wave forms are closer to square wave than to sine wave, and moreover they contain a dc bias component that can easily more than double the ferrite losses. Therefore, in loss critical applications it is good to be able to both test and model the losses of the actual ferrite cores under the same conditions as in the actual power application. In this paper, experiments were carried out at different induction levels and dc bias currents. Losses were measured at frequencies of 20, 100, and 500 kHz on a ferrite core with Ferroxcube 3F3 material, a Mnâ€"Zn ferrite. We observe that mainly the lower frequencies are sensitive to dc bias. A model including wide ranges in amplitude, frequency, and also dc bias is proposed. In this model, the losses are separated in three terms: a hysteresis dependent term, an additional loss term depending on dc bias, and a high frequency term."



All said above stays of the mechanism and dependency of bias being applied to ferrite.









bias is for the purpose of canceling any residual magnetism in the ferrite.
bias is for the purpose of controlling gain in the certain number turns per square Ampere

I see 2 quotes:so I respond into it:

Magnet create temporary stage of alignment of dipoles within ferrite

If the capacitor is connected in parallel to winding  around the  ferrite core than this will induce electromotive force in the winding.
Notice on the video
http://www.youtube.com/watch?v=pGOFNrlVm1Q
He is moving magnet slightly inside the core.
If he was holding magnet in the core steady the energy induced would be consumed by LED.
After  removal of the magnet light is off.

when we dealing with magnet than we dealing with  polarization.
depends on the angle  when introducing magnet  inside the core notice that gentleman kept it near one side of the ferrite core.

That experiment could be done with air core as well.
Q of  air =1
Q of ferrite can go up to 22 000 ( permeability dependent)

so ferrite here is only amplification device.
Apart from the facts mentioned above I do not see anything strange.


Wesley

[Paper]

Thank you.

[penno64]

Hi All,

In PVA9's youtube -

http://www.youtube.com/user/PVA9#p/a/u/0/lxCCGNfD2cg

can someone identify the long black/white component at 1:19 on the right side of the PCB. closest to his thumb.

Also, the device at the end on the black/white component, before the cap.

Kind Regards, Penno

[stivep]

Hi All,

In PVA9's youtube -

http://www.youtube.com/user/PVA9#p/a/u/0/lxCCGNfD2cg

can someone identify the long black/white component at 1:19 on the right side of the PCB. closest to his thumb.

Also, the device at the end on the black/white component, before the cap.

Kind Regards, Penno

interesting
Do not take my words as accurate explanation i might be wrong in my assumption..


Radio field (RF)waves rectified  and
generator  made  from  microchip
frequency stabilized and tuned using Cristal oscillator (next  to  vertical capacitor)
voltage doubler made on transformer ( one in the middle)
output voltage 110V
Transistor used as signal amplifier.
The small long withe black object looks like ferrite antenna from  Radio receiver

total output 1W 110V

objections:
1.I do not see how strong radio waves say HF could be received without presence of tuning capacitor ( or maybe I do not see that)
2. generator could be delivering signal   to create one step heterodyne receiver where IF( product of mixing signal from antenna and signal from generator) so than amplified and delivered to the load instead of speaker.

3. function of powering transistor and microchip must be made as means of delivering DC. That will explain presence of Graetz bridge and capacitor in the corner.

Anyone wants to take stand ?

Wesley


PS: that what makes me confuse is presence extended wires  V shape from left side of the board ( when flipped)

What is the role of these two wires connected at the end.?
would that be  instead of tunning capacitor just to tune to the strongest RF signal  around?

Second what confuse me is presence of second toroid with the thick wire.
If the first one in the middle is the step up transformer than what is the role of the second one?

from the other hand if that circuit is tuned to 60Hz than he is utilizing energy from his own  electrical supply to the apartment.

but  The lower the frequency the more winds is required for resonance circuit to tune to that frequency. From antenna(long shiny ferrite with possible coil inside) it looks like coil was taken from  mass production RF AM radio. With no ability to tune( slide it  on ferrite)
If amplification  factor because of use of ferrite  is up  Q up to 22 000
we may  analyze it as ferrite that is permeability 800 that may give Q of 160-300
Still sufficient enough.

Wesley