advancing the Solid state Tesla hairpin circuit

evostars

monopole
« Reply #225, on August 11th, 2019, 08:09 AM »
just tested the counter wound bifilar coil as L1, and it works. lower voltage needed, and naturally a higher current.

Magnetic field is south on both sides (or north if polarity is reversed).

If Ken Wheeler is right, the south pole is centripetal, a influwing vortex, north is a centrifugal outflowing vortex.
Both sides of the counterwound bifilar coil have a inflowing south vortex pole.
The north poles  are squashed in between the windings, and from what I have seen from the ferro cell, when two magnets are in opposition a new dielectric field is created in between them. so now we have a south pole vortex on each side of the pole and a dielectric field in between the windings.

Also could mean, with south on the inside, a inflowing dielectric field is generated bewtween the windings, and outlfowing north on each side...

the series connection can be chosen on the outside or inside rim of the bifilar coil. The voltage difference between the supplied voltage/current will create also a local dielectric field. but this one will probably neglect-able.

compass needle shows same poles on each side of the coil. at the outside rim, there the needle also deviates, showing a influx or out flux. interesting stuff...
.





evostars

Re: advancing the Solid state Tesla hairpin circuit
« Reply #228, on August 21st, 2019, 04:51 AM »
I worked out several scripts for new videos and have started recording new video material (for my master ivo channel).

stepping back from the research was a good choice.
my mind is becoming clearer again, and I have better perspective on whats going on.

no promises, but I intend to make multiple videos, showing/explaining
the fields of the coil
the series resonant bifilar coil
the impulsed series resonant coil

 :D


evostars

cap impedance change from impulse
« Reply #230, on September 18th, 2019, 11:35 PM »
I'm still working on a series of new videos. making good progress.
While in production, I do not experiment, and this bring my mimd into focus. A lot becomes clear.

One of the things I encountered, and showed in the radiant power video (master Ivo, youtube) is the reduced power draw when L1 and L2 are coupled. And still it produced large Impulses.

These Impulses are a representation of the magnetic field energy, So with the reduced power draw, they are over unity by them selve (I think, but need to test).

These Impulses can charge up caps really fast, as if the caps are much smaller.
Tesla has a patent on this 462418

I really like to see how this all works. I have many ideas, and will test in the future.
but for now, I stick to the videos production.

evostars

Tesla exta coil, as impulse amplifier, through higher harmonic
« Reply #231, on October 22nd, 2019, 06:56 AM »
First video is finished. Got several more im production.

meantime, I have been thinking about how to amplify the impulse voltage.

It seems Tesla's "extra coil"  holds the answer.

instead of magnetic coupling amplification, which loads down the source,
I will use the loose dielectric coupling.

this means using a resonant coupled coil(secondary) .
the resonant frequency of the "extra coil" will be a higher harmonic of the series resonant L2 coil (primairy)

due to the higher frequency, the impulse duration will be shorter, and the impulse voltage higher.

the L3 could be grounded, on the series resonant  L2, between the l2 coil and the series tuning cap (where the resonant voltage meets the impulse).

I wonder if L1 then also acts on a harmony of the l2 and l3. but thats for later.

evostars

Tesla's extra coil, as impulse magnifier
« Reply #232, on November 21st, 2019, 02:28 PM »
 I have kept my promise to myself  to produce 3 videos. I have a few more scripts. But first I need to do some experimemts.

Tesla's extra coil had very little capacity and the resonant frequency of it was much higher then the secondary.

I hooked up L3 (no parallel cap) to L2.
L3 (outer rim) connects between L2 and l2's series resonant tuning cap.

So L3 rings, from the impulse.

First test looks good. Indeed impulse is amplified in L3 (extra coil).

trick is to tune the impulse duration to L3's half period of its resonant frequency. Which is a lot higher around 600kHz. it needs a 700nS impulse to fit perfectly, and make it ring perfect, but my impulse right now is to slow. 1.2uS  but I can fix it.

L3 is ringing pretty hard already. But if the impulse matches it should be even better.


evostars

magneto dielectric ringing
« Reply #233, on November 21st, 2019, 02:43 PM »
To generate the impulse, I couple L1 and L2. as showenninnthe radiant power video, this reduces the current a lot. I suspect It also slows down the impulse a bit.

It now runs at around 2.5W giving -700V impulses 1.2uS at aroumd 58kHz

that 700v impulse is amplified in L3 to around - 1200V due to its ringing, its lower capacity and thus higher frequency.

I wonder if the ringing is magneto dielectric in nature, meaning, longitudinal ringing, whereby the current and voltage are in phase. (also as shown in radiant power video).

I wonder how quick a cap will charge, if I tune L1 (impulse duration) L2 (base tone) L3 (higher octave ringing from impulse).

But first I need to tune. In the end Steinmetz was clear, I need a ringing oscillation that rises in amplitude.




evostars

parametric resonance
« Reply #234, on December 8th, 2019, 04:28 AM »Last edited on December 10th, 2019, 03:48 AM
instead of external created resonance, resonance can also be created, by varying inductance and or capacitance.
Capacitance can be changed by impulse the capacitor.
The capacitor appears smaller, as it charges faster. The impedance of the capacitor changes under influence of the impulse.

The coils capacitance needs to be charged by high voltage, so the series tuning capacitor can not be big, it need to be small to get high enough voltages to charge up the dielectric field of the bifilar coils capacitance.

The parametric resonance can create a rising ring in the output, rising in amplitude, when it the impulse is twice per period. One for the positive half one for the negative half.  With a single coil this would result in twice the frequency for the impulse sine. But I feel there is another way.

I tried it before, but need to look into it again. Make 2 impulse systems, which are 180 degrees out of phase. Maybe this time, I should also include the positive impulse, for the second half period of the output sine.

The output sine, might still be higher in frequency, but ideal it would have the same frequency. I dont see how it could be, without tuning with an external capacitor.

I made a quick drawing of the new circuit I need to make. It's a inverse of what I have been using, this time, L1 is low side switched (which is easier) and the impulse thus created is positive, and needs to enter series resonant L2 at its maximum negative voltage.
The DC offset of L2 now will be negative.

So, in total this creates 2 dc offsets:
 one set of L1+L2 (close coupled) has L2 positive DC offset
the other set of L1+L2 (close coupled) has L2 negative DC offset

If L1 is in the middle, they can be opposing, creating stronger impulses. and making the center neutral (earth ground L1).
the output would then be on the outside, 2 coils together one. I have strong doubts about that.

If L1 is on the outside, the positive and negative dc offset l2's would be in the center, creating a strong dielectric field, where in the middle of that field would be the (single) L3 output coil, recieving the alternating impulses on both sides of L3.

the impulses make the dielectric field between the 2 L2's (a and b) collapse. this collapsing field travels from left to right, and then from right to left.
creating a longitudinal energy back and forth in L3

L3 ideal would be the same frequency as L2, but as sad would need tuning. If not tuned, It would still work, as the higher octave resonance of L3 would work as the extra coil, the impulses of L2 a and b would both have the duration of half of the sine wave of L3. 
Still in this scenario, I would think the ringing would fade, instead of grow. The growing sine ring of L3, would be best when the sine wave is syncronous with the impulses of L2a+b.

A lot to test, A lot to build.
Back to work.

 positive impulse circuit.png - 41.58 kB, 1152x648, viewed 77 times.

 double system.jpg - 70.51 kB, 1152x648, viewed 71 times.

 L2 voltages.jpg - 46.55 kB, 625x291, viewed 45 times.


evostars

low side gate driver
« Reply #235, on December 10th, 2019, 12:15 PM »Last edited on December 12th, 2019, 11:24 AM
I finished building the low side SiC mosfet gate driver. it is powered by a buck boost converter.

driver IC is the same isolated one as I used before:

1EDI60I12AF

for this SiC mosfet:
2m0160120d

gate source voltage recomended, 20V, this is set by my boost buck converter

 20191210_211144.jpg - 1913.32 kB, 2560x1440, viewed 62 times.


evostars

Low side circuit ready for testing
« Reply #236, on December 11th, 2019, 11:07 AM »
Re used one of my first boards, needed to mirror yhe circuit and rewire everything

didn't add 12V to the gate driver board, but fan could hook up to high sigh circuit 12V.

 20191211_171535.jpg - 1994.09 kB, 2560x1440, viewed 57 times.


evostars

Re: advancing the Solid state Tesla hairpin circuit
« Reply #237, on December 12th, 2019, 12:05 PM »
tested the new low side circuit and it works. It shows the same current reducing ability when L1 and L2 are coupled. While maintaining a positive impulse.

Next step... windings coils

 20191212_210157.jpg - 2357.2 kB, 2560x1440, viewed 59 times.


evostars

5 stacked bifilar pancakes
« Reply #238, on December 12th, 2019, 02:26 PM »
the higher the better
:yodel:

I made life easy, I had the coils already.

L3 is 2.5mm2
l2's and l1's are 1.5mm2

hook m up and pump them

l3 in the center 15mm from the l2's

 20191212_232139.jpg - 1945.37 kB, 2560x1440, viewed 54 times.

 20191212_232532.jpg - 1469.98 kB, 2560x1440, viewed 67 times.



evostars

Full setup ready for test
« Reply #240, on December 12th, 2019, 03:24 PM »Last edited on December 12th, 2019, 05:12 PM
I got 4 new 9v's lucky me.
setup is ready for full test.
highside circuit on the left
full right is capacitor switch board hooked to L3 (fully open as Tesla extra coil)

middle low side circuit and TTA square wave gen (out of phase signals)

lots of room for improvement. impulse is 1.2uS - 800V in the high side circuit

should be able to get it faster and more negative, by reducing resistance of cable couplings (will replace by silver soldered wire)

12V battery is charging, so ar the nimh 9V batts. They quickly turned their polarity and reached capacity much to soon, I'll keep them over night at this level, and then see how much charge they hold. or if the voltage drops down to fast

 20191213_002006.jpg - 2351.71 kB, 2560x1440, viewed 61 times.


evostars

impulse charging nimh 9V batteries (negative voltage after completely dry)
« Reply #241, on December 12th, 2019, 05:17 PM »
Since, I have a circuit that is perfect for charging like this... why not hook one up, and see if I can restore the battery in its full glory?
Im talking about impulse charging. 9V... mmm lets tune it down to 14V and then rise the impulse level. Positive or negative impulses? hmmm I'd say positive. since that connects to the inertia.

evostars

Re: advancing the Solid state Tesla hairpin circuit
« Reply #242, on December 13th, 2019, 02:34 AM »
9V nimh batteries are charged back up to 10V and holding charge. Nice!

I realized the quick test with 800v impulses 1.2uS was with a mosfet gate switching voltage of 12.7V (lead acid battery only) and with the depleted nimH in series.

Gate to source voltage now will be 13.5 +10=23.5V

Curious how this influenced the impulse voltage and duration.

evostars

First run of double system
« Reply #243, on December 13th, 2019, 03:16 AM »
looks good. 0.17A 32V input
700V impulses positive and negative alternating each other at 53 kHz

untuned setup.
high side circuit has 40nf
low side circuit has 45nF
as series L2 tuning cap.

Impulse duration of low side circuit is shorter (faster). could fix by adding capacity over L1. But better to first decrease overall resistance, to get max speeds. and higher impulse voltages.

So far a very good start!

scope shows both L2 coils voltages

 20191213_121141.jpg - 1119.47 kB, 2560x1440, viewed 51 times.

 20191213_121128.jpg - 1221.46 kB, 2560x1440, viewed 46 times.


evostars

Re: advancing the Solid state Tesla hairpin circuit
« Reply #244, on December 13th, 2019, 03:28 AM »
L3 sine wave also is present. many octaves higher.(extra coil)
I added 600pF in parallel (that should be series) to lign up the l2 impulses with it.
even added a 28W lamp. showed dim glow at cost if 8w input (0.25A 32V input).

this is untuned! Looks very promising.

 20191213_122314.jpg - 1486.27 kB, 2560x1440, viewed 54 times.




evostars

Variables in the setup
« Reply #247, on December 14th, 2019, 04:07 AM »
I need to consider all the possibilities in the setup.

for instance, Do the 2 circuits work together, or against each other in their fields.
In other words, do the two L1 coils magnetic fields attract, or repulse?
This automatically also will hold for the two L2 coils, as they are series resonant, and also produce magnetic fields.

The distance,
I now use 15mm between the L2 and L3 coils. This is not enough, it distorts the wave forms, and diminishes the impulse voltages.
What is the perfect distance? error and trial, L3 needs to be able to ring, and what is ringing? The volume of Aether surrounding it.

Fusion reaction:
The volume of Aether between the L2 coils and the L3 coil, is where the magnetic fields and dielectric fields come together, and create a form of Electric FUSION. Whereby the dielectric and the magnetic fields become one, to form electricity, Electric POWER.

This is still the theory... so It might not work at all... but, we'll see.

The impulse duration.
L3 should have a very high resonant frequency, being untuned. It acts as a " extra coil" the impulse should match the half period of the resonant frequency of L3. Duration can be tuned, by adding a parallel capacitor over one winding (half) of L1

Impulse voltage.
The positive and negative impulses When equal in duration, should be equal in voltage as well.
I see no way to tune this. The L1 coils that produce the impulses are equal in size, are switched by the same mosfet types, so It is what it is.
The voltage level, represents the change in the dielectric field strength between the two L2 coils (that act as capacitor plates, setting up a dielectric field).

DC offset voltage
The dc offset voltages of the two L2 coils (positive and negative DC) set up a dielectric field between them.
But due to the distance, between the L2 coils, and the L3 being in the middle of this field, the capacitance is very low. This would need a very high voltage to set up a proper field strength. 

L2 resonant voltages.
the L2 coils series resonant voltages are charging the L2 coils up as capacitors. The resonant voltage is higher, when the series capacitor is smaller.
When the cap is smaller, the frequency is higher, when the frequency is higher, the impulse voltage is lower.
So, It might need a higher DC input voltage. I am now limited to 32V, and I would like it to work of 24V (2x12V battery).
Luckily the power drain is low.

Power supply.
Ideally It should work off 24V power. But I might need much higher voltages to get enough impulse voltage out of the L1 coils at higher frequencies.
I could use a step up  boost converter, to get for example 48V from the 24V.

L3 tuning.
I strongly believe L3 should not bet tuned. But adding small capacitances might help tune it. Parallel tuning, is not an option, it creates high impedance, (but I should explore it once again) Adding series capacitance might do the trick, in the order of 100pF. Maybe on both sides of the L3 coil, maybe on only one side (center rim tap). Very doubt full about all this, untuition says, no L3 tuning. As it works as a resonant step up transformer, by resonating on a higher octave.
This also should mean, the L2 series resonant coils should resonante, at a lower octave of L3, whereby the impulses of L2 match up with the right fase of L3.
positive l2 impulse at positive max L3 voltage,
negative l2 impulse, at L3 negative max voltage.

L3 grounding
I feel L3 should not be grounded. but... I should try it, outside rim to EARTH ground.

L3 output.
if rectified to DC, with mur1660ct diode full bridge rectifier, the high voltage DC can be stored in capacitors (combination of elco and polypropylene, to deal with the high frequencies). Then a resistive load can be added and power can me measured.
The DC voltage also can be transformed into 50/60cycle 230V or 115 V AC.  Even 3 phase. And produce work...
The output then can aslse be used to couple back to the input side...

output input coupling.
Since a higher voltage input probably is needed, the output which is already high voltage, might easily be coupled back to the input, but voltage regulation is a must...





carbon sugar

Re: advancing the Solid state Tesla hairpin circuit
« Reply #248, on December 14th, 2019, 09:02 AM »
Hi, masterivo, how are you? I am from arg and I have been doing your experiences but I use a poe vortex coil, assemble your circuit because I liked the negative pulse, just add a diode to the mosfet for the back emf, so that it does not burn, well the pancake coil if it is great, but many better results achieved with a poe vortex coil, the fields, the magnetic and the radiant can be unified and a field self-induction is generated, the magnetic is the static field, and when we grow that field the radiant flow is the that flows and greater radiant flow greater energy, free energy is obtained easily and on unit too, I have a scalar wave machine too, which is better with this coil, the interpretation of the fields is much easier :D :D :D

evostars

impulse voltage and duration equal
« Reply #249, on December 15th, 2019, 02:10 AM »
my rigol probes show a voltage difference. need to recalibrate or get new probes.
more importantly, the impulses are equal in voltage and duration