Kapanadze Cousin - DALLY FREE ENERGY

[itsu]

Hi Jeg,

good move.

I will do some tests these next days, including using 240V bulbs and measuring the current in severall places.

My last screenshot was with a 5W bulb, but also with feedback like the screenshot (21W bulb) before.
The fact that the input voltage raised somewhat is because its just a matter of time (minutes) the supercaps
start to drain, and with 5W it is slower then with the 21W bulb.

Looking at the current trace shape, it seems that something (ferrite?) is saturating with the 21W bulb)


Itsu

[Hoppy]

Hi Jeg,

Good move. I think we should ask V8carlo to post photos / video of his Q schematic bench setup and test results, so that accurate replications can be built by those wishing to do so. I think you will appreciate that from my comments on the other thread, I consider that these circuits / schematics from V8carlo are non starters, so I will not be building but will follow your tests and results with interest.

[Jeg]

Thanks guys.
Itsu
I use a yoke core. 12T primary, 24 turns secondary.

Hoppy
No worries my friend, your opinion on what happens is enough!

FYI this is the device that i am trying to apply the Q-topology. I find it very efficient by itself.

https://www.youtube.com/watch?v=manMnNOFdNI

[Void]

Hi Jeg. I am curious why you chose to post this V8Karlo stuff in the Kapanadze thread?
It has nothing to do with Kapanadze. Why not start a new thread and call it maybe the
"V8Karlo and Other Obviously Unworkable Schemes". ;-) You will most likely be waiting a
very long time if you actually expect v8Karlo to provide you with any actual measurements
and meaningful test results. See my comments in Wesley's thread on why this type of
arrangement will not likely at all even improve efficiency much. Resistive loads dissipate energy.
Feeding current though resistive loads and then back to the power source will not recover the
energy lost in those resistive devices (diodes and bulbs). Once energy is dissipated, it is dissipated.
Have a happy new year guys!

[color]

Best wishes for a Happy New Year.

---------------
Hi Jeg. I am curious why you chose to post this V8Karlo stuff in the Kapanadze thread?
It has nothing to do with Kapanadze. Why not start a new thread and call it maybe the
"V8Karlo and Other Obviously Unworkable Schemes". ;-) You will most likely be waiting a
very long time if you actually expect v8Karlo to provide you with any actual measurements
and meaningful test results. See my comments in Wesley's thread on why this type of
arrangement will not likely at all even improve efficiency much. Resistive loads dissipate energy.
Feeding current though resistive loads and then back to the power source will not recover the
energy lost in those resistive devices (diodes and bulbs). Once energy is dissipated, it is dissipated.
Have a happy new year guys!
---------------


Charge is the fundamental property of forms of matter that exhibit electrostatic attraction or repulsion in the presence of other matter. Electric charge is a characteristic property of many subatomic particles. The charges of free-standing particles are integer multiples of the elementary charge e; we say that electric charge is quantized. Michael Faraday, in his electrolysis experiments, was the first to note the discrete nature of electric charge. Robert Millikan's oil drop experiment demonstrated this fact directly, and measured the elementary charge. It has been discovered that one type of particle, quarks, have fractional charges of either −
1
/
3
or +
2
/
3
, but it is believed they always occur in multiples of integral charge; free-standing quarks have never been observed.

By convention, the charge of an electron is negative, −e, while that of a proton is positive, +e. Charged particles whose charges have the same sign repel one another, and particles whose charges have different signs attract. Coulomb's law quantifies the electrostatic force between two particles by asserting that the force is proportional to the product of their charges, and inversely proportional to the square of the distance between them. The charge of an antiparticle equals that of the corresponding particle, but with opposite sign.

The electric charge of a macroscopic object is the sum of the electric charges of the particles that make it up. This charge is often small, because matter is made of atoms, and atoms typically have equal numbers of protons and electrons, in which case their charges cancel out, yielding a net charge of zero, thus making the atom neutral.

An ion is an atom (or group of atoms) that has lost one or more electrons, giving it a net positive charge (cation), or that has gained one or more electrons, giving it a net negative charge (anion). Monatomic ions are formed from single atoms, while polyatomic ions are formed from two or more atoms that have been bonded together, in each case yielding an ion with a positive or negative net charge.

During formation of macroscopic objects, constituent atoms and ions usually combine to form structures composed of neutral ionic compounds electrically bound to neutral atoms. Thus macroscopic objects tend toward being neutral overall, but macroscopic objects are rarely perfectly net neutral.

Sometimes macroscopic objects contain ions distributed throughout the material, rigidly bound in place, giving an overall net positive or negative charge to the object. Also, macroscopic objects made of conductive elements, can more or less easily (depending on the element) take on or give off electrons, and then maintain a net negative or positive charge indefinitely. When the net electric charge of an object is non-zero and motionless, the phenomenon is known as static electricity. This can easily be produced by rubbing two dissimilar materials together, such as rubbing amber with fur or glass with silk. In this way non-conductive materials can be charged to a significant degree, either positively or negatively. Charge taken from one material is moved to the other material, leaving an opposite charge of the same magnitude behind. The law of conservation of charge always applies, giving the object from which a negative charge is taken a positive charge of the same magnitude, and vice versa.

Even when an object's net charge is zero, charge can be distributed non-uniformly in the object (e.g., due to an external electromagnetic field, or bound polar molecules). In such cases the object is said to be polarized. The charge due to polarization is known as bound charge, while charge on an object produced by electrons gained or lost from outside the object is called free charge. The motion of electrons in conductive metals in a specific direction is known as electric current.