Pulsed DC Transformer with Embedded Magnets

[bille]

I'm trying to bring myself up to snuff on this lead out theroy.
Its difficult beause its a whole new way of thinking.
I would like to present a new idea, a new way of thinking.
Its a lot about what I've been learning but taken to the next level.
Thankyou
BE

[Paul-R]

I'm trying to bring myself up to snuff on this lead out theroy.
Its difficult beause its a whole new way of thinking.
I would like to present a new idea, a new way of thinking.
Its a lot about what I've been learning but taken to the next level.
Thankyou
BE

If you are good with Mathematics and Quantum Mechanics, you should look into the Nobel Physics prize for 1957 and Hal Puthoff's (University of Stanford, CA) views on the amount of energy in the space occupied by a coffee cup.

[NerzhDishual]

Hi FLEET guys,

Thanks for you feedbacks.

@Itseung888:
Actually, I have made a couple of 'Joule Thieves' that work right. But it was the first time that I managed, thanks to Gadgetmail, to  build a JT that could also charge another bat. I was not able to replicate it.

@Bille:
I see what you mean about the oscillator that could stop working. Actually, I do not remember having tried to check this with my oscillo.
BTW: your are just smart.
--------------------
Anyway, I have, now, succeeded to get another working circuit with L3 having two 22 turns secondary (one CW and another CCW) (and not only one 22 turns).
This second circuit is not as efficient as my first one. Please, do not ask me why...

So, I maintain that some MOJO is necessary for achieving 'OU'....

Very Best

[nul-points]

aha - Mr Dishual, we meet again!

when - and i'm certain it will be 'when' and not 'if' - you get your latest JT to work to your satisfaction...

you should be able to charge TWO batteries simultaneously (and at the same time, too!), not just one as in your cct diagram - since the secondary produces an AC waveform

you can connect a second diode/battery arrangement in parallel and with reverse polarity to the first diode/battery and use the presently unused other polarity of the AC output waveform

and now for something completely different (remind me who used to say that?)...

here's a little MOJO to help you with your Quest for the Holy Grail:
   http://swampfish.org/mp3s/i_got_my_mojo_working.mp3

bien amicalement, A+
sandy

[ltseung888]

What kind of resonance are we talking about? Part 1

Nuclear magnetic resonance
From Wikipedia, the free encyclopedia

Nuclear magnetic resonance (NMR) is a property that magnetic nuclei have in a magnetic field and applied electromagnetic (EM) pulse or pulses, which cause the nuclei to absorb energy from the EM pulse and radiate this energy back out. The energy radiated back out is at a specific resonance frequency which depends on the strength of the magnetic field and other factors. This allows the observation of specific quantum mechanical magnetic properties of an atomic nucleus. Many scientific techniques exploit NMR phenomena to study molecular physics, crystals and non-crystalline materials through NMR spectroscopy. NMR is also routinely used in advanced medical imaging techniques, such as in magnetic resonance imaging (MRI).

All stable nuclides that contain an odd number of protons and/or of neutrons (see Isotope) have an intrinsic magnetic moment and angular momentum, in other words a nonzero spin, while all nuclides with even numbers of both have spin 0. The most commonly studied nuclei are 1H (the most NMR-sensitive isotope after the radioactive 3H) and 13C, although nuclei from isotopes of many other elements (e.g. 2H, 10B, 11B, 14N, 15N, 17O, 19F, 23Na, 29Si, 31P, 35Cl, 113Cd, 129Xe, 195Pt) are studied by high-field NMR spectroscopy as well.

A key feature of NMR is that the resonance frequency of a particular substance is directly proportional to the strength of the applied magnetic field. It is this feature that is exploited in imaging techniques; if a sample is placed in a non-uniform magnetic field then the resonance frequencies of the sample's nuclei depend on where in the field they are located. Since the resolution of the imaging techniques depends on how big the gradient of the field is, many efforts are made to develop more powerful magnets, often using superconductors. The effectiveness of NMR can also be improved using hyperpolarization, and/or using two-dimensional, three-dimensional and higher dimension multi-frequency techniques.

The principle of NMR usually involves two sequential steps:
•   The alignment (polarization) of the magnetic nuclear spins in an applied, constant magnetic field H0.
•   The perturbation of this alignment of the nuclear spins by employing an electro-magnetic, usually radio frequency (RF) pulse. The required perturbing frequency is dependent upon the static magnetic field (H0) and the nuclei of observation.

The two fields are usually chosen to be perpendicular to each other as this maximizes the NMR signal strength. The resulting response by the total magnetization (M) of the nuclear spins is the phenomenon that is exploited in NMR spectroscopy and magnetic resonance imaging. Both use intense applied magnetic fields (H0) in order to achieve dispersion and very high stability to deliver spectral resolution, the details of which are described by chemical shifts, the Zeeman effect, and Knight shifts (in metals).

NMR phenomena are also utilized in low-field NMR, NMR spectroscopy and MRI in the Earth's magnetic field (referred to as Earth's field NMR), and in several types of magnetometers.

Let us list some existing knowledge on various types of resonance first.