Overunity.com Archives is Temporarily on Read Mode Only!



Free Energy will change the World - Free Energy will stop Climate Change - Free Energy will give us hope
and we will not surrender until free energy will be enabled all over the world, to power planes, cars, ships and trains.
Free energy will help the poor to become independent of needing expensive fuels.
So all in all Free energy will bring far more peace to the world than any other invention has already brought to the world.
Those beautiful words were written by Stefan Hartmann/Owner/Admin at overunity.com
Unfortunately now, Stefan Hartmann is very ill and He needs our help
Stefan wanted that I have all these massive data to get it back online
even being as ill as Stefan is, he transferred all databases and folders
that without his help, this Forum Archives would have never been published here
so, please, as the Webmaster and Creator of these Archives, I am asking that you help him
by making a donation on the Paypal Button above.
You can visit us or register at my main site at:
Overunity Machines Forum



Kapanadze Cousin - DALLY FREE ENERGY

Started by 27Bubba, September 18, 2012, 02:17:22 PM

Previous topic - Next topic

0 Members and 125 Guests are viewing this topic.

verpies

Quote from: Void on March 08, 2016, 02:51:21 PM
If it is a short winding, then we should just leave more space between each turn to make use of the entire toroid circumference?
That's one solution, but then you're left with uncancelled circumferential current.
A better solution is to parallel low-count windings.  This way even a one-turn winding can span the entire circumference of the core.

Quote from: Void on March 08, 2016, 02:51:21 PM
Thanks Verpies. Just to be sure I understand correctly, do you mean that for the purposes of reducing
leakage inductance, it is always better to use the whole toroid for windings than to wind multiple layers
on just one side of a toroid for a particular winding?
Below, I have listed the combinations from best to worst:

1) Spanning entire circumference, even number of forward&back layers,
2) Spanning entire circumference, odd number of layers,
3) Spanning part of the circumference, even number of forward&back layers,
4) Spanning part of the circumference, odd number of layers.

These winding rules apply any time a tightly coupled transformer with low leakage inductance and high coupling coefficient (k) is desired.
These rules are not specific to the lossless clamp windings, although they do help them to perform better, too.


See the illustration below.  The number of flux lines symbolizes the amount of magnetic flux.
Notice, that in Fig.1 and Fig.3, five lines of flux are leaking outside of the core and in Fig.4, six lines are leaking out.
This is what actually happens when narrow windings (not spanning the entire circumference of the core) are used.

BTW: The magnetic flux created by the circumferential current, is not shown on these illustrations because such flux is directed perpendicularly to the plane of the drawing ("out of the page").

Void

Quote from: verpies on March 08, 2016, 06:44:45 PM
A better solution is to parallel low-count windings.  This way even a one-turn winding can span the entire circumference of the core.

Hi Verpies. Thanks. That is interesting info. I don't understand what you mean by the line quoted above.
What do you mean by "to parallel low-count windings"?

stivep

In regards to  capacitance of the diode. T1000 is right.
In regards to   values of the resonance  circuit that would never be seen as capacitance  and inductance.
You must think of it as components of impedance at given frequency.
In the Smith chart you can easily calculate- see( with no calculation) the values of impedance.


1.The same resonance circuit (or element acting as resonating component e.g single capacitor or single  inductor ) will have components of impedance  at the same very time  corresponding to
-Equivalent Circuit Series
- Equivalent Circuit Parallel
- Equivalent Circuit Series-Parallel ( mix)


2.The same resonance circuit (or element acting as resonating component e.g single capacitor or single  inductor ) will have components of impedance 
-with  total impedance showing capacitive character ( below horizontal line of Smith Chart)
characterized by high voltage low current ( at that given frequency)
or
-with  total impedance showing inductive character ( above horizontal line of Smith Chart)
characterized by low voltage high current ( at that given frequency)


3. With change of frequency character of the circuit will change.

4. instrument that uses Smith chart is Vector Network Analyzer (VNE) or  Network Analyzer (NE)[/size]
https://en.wikipedia.org/wiki/Smith_chart




5. some older pieces of  tools similar to VNE  or NE    are using Polar  or rectangular  graph
very helpful is to have (  Phase , Gain Analyzer HP 4194A (50 Ohm)


6. it does not matter how big is the voltage and current in resonance circuit, just bring it down to level of millivolts and now safely measure or calculate  its values


7. parameters of impedance will always be made of:
- inductive reactance
- capacitive reactance
- resistive component
However pure resistive components can have reactances close to zero.
Calibration resistors (  50Ohm) are made this way. They act as  50 Ohm resistors  in all  spectrum frequencies  of the bandwidth of the instrument from 30kHz to 6GHz   

http://www.arrl.org/files/file/Antenna%20Book%20Supplemental%20Files/22nd%20Edition/Smith%20Chart%20Supplement%20-%20Corrected%20Jan%202012.pdf
Quote
This feature permits the use of the Smith Chart for any impedance values,



Wesley

SeaMonkey

This present discussion is quite interesting.  These
are the same sorts of problems the pioneer engineers
who worked with semiconductor switch-mode power
supplies had to discover and solve. :) ;)

Most switch-mode textbooks devote at least one chapter
to the techniques of minimizing transients and spurious
oscillation/ringing.  High speed switching introduces
several really difficult challenges. :o

You're on the right track guys! 8)

Jeg

What a great info Verpies. Thanks
Quote from: verpies on March 08, 2016, 06:44:45 PM
That's one solution, but then you're left with uncancelled circumferential current.
A better solution is to parallel low-count windings.  This way even a one-turn winding can span the entire circumference of the core.

Same question with Void. Do you mean to wind each turn perpendicular to the core axis? If yes, what about the secondary? Doesn't it need too to be wounded with the same manner so to have Lenz?

Quote from: verpies on March 08, 2016, 06:44:45 PM
Below, I have listed the combinations from best to worst:

1) Spanning entire circumference, even number of forward&back layers,
2) Spanning entire circumference, odd number of layers,
3) Spanning part of the circumference, even number of forward&back layers,
4) Spanning part of the circumference, odd number of layers.

Can we safely assume that case 3 is better than case 2 when diameter of the core is higher than a critical value? Or case 2 is better than case 3 in any way?