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Overunity Machines Forum



Joule Thief

Started by Pirate88179, November 20, 2008, 03:07:58 AM

Previous topic - Next topic

0 Members and 85 Guests are viewing this topic.

gadgetmall

Quote from: Mk1 on November 27, 2009, 06:02:57 PM
@all

I also know this now ...

What could i have new to say ?

Nut much , but if i was to try this i would first try to find the best gauge for the jt side (bigger wire ) then try the match them gram for gram , since they will have the same mass and materiel they will share resonance at any freq.

The smaller you go on the secondary side , bigger resistance higher turn ratio for mass , same mass smaller gauge .

I think this will make sure that the current is not lost due to unmatched weight ...

Depending on the winding direction you get different sine wave .

Winding rotation direction , can help setting kick generation (+or-), when working with multiple core.

I hope this will help

Mark
I always work on lowest miilamp input .Mark, being were flashing to the past maybe post the best cap charger you made . this is second stage Level two . how fast can we charge LARGE  super /ultra caps .
Gadget
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Mk1

@gadget

You know it ...

Many turns on the jt side usually reduces the amp needed, i think the longer they are more chances to trap some energy within the coil between kick .

When i us the short ones is to make insure that the will be flushed out.
I believe that way the kick is not slowed down from the slow emptying of the longer ones .

So i do it to get a clearer kick.

I hope this makes sense to you .

I did get really low mili amps input on both types .

Now the same mass issue , you have the two jt coils kicking , how much energy can be stored in a coil(like a cap) the secondary needs to have the same potential , to minimize the losses .

That could be done many ways but the coils are from the same material and same weight , will have the same natural resonant response at any freq .

Like guitar strings tuned together pick one the other will move , if you had 2 exact same diameter strings you can tune them to any note pick one and the other will react much more violently , you get the idea ?

I still have not used your tank circuit .

I study coils for now ,lol i will get to other stuff like trany and circuit soon.

Mark

The kick is the same but the the loses form the secondary close to eliminated .


Edit btw i don't super caps or any thing close to it , but any cap will do.

you test for speed , smaller cap help wit faster evolution waiting over 10h to get results is my thing , but i can also compare the secondary  output compared to the pickup .

xee2

@ jeanna

Quote from: jeanna on November 27, 2009, 05:33:28 PM
Thanks xee2,
I was there yesterday, but I was unable to find a starting point of reference.
The tor-60 was not one of their numbers, because they discontinued it, and the dimensions 3.38" are no longer used for the same reason, and I don't have enough info to start.

You were the person who wrote way back what the mu value for this toroid is.
I did not save that,

I am glad you have shown up today.
What is the mu value for that bog toroid?

thank you,

jeanna

Part number for the 3.38" diameter toroid is:  OW48613TC which is their W material.

Most of the data I have was in the design guide which use to be at following URL (but now must have a different address for a new guide). This is the old URL which does not work now for me: http://www.mag-inc.com/ferrites/fc601.asp

Here is some data:


Mk1

Next step in basic jt true ringing .

Find a core made for metal ring , not any toroid shape !

You hang it from a string then hit it with something hard , if it doesn't make a sound you can hear then find another one for now .

One you got one connect a microphone to your scope , find the ring freq.

Built the jt with that precise freq in mind , then ring it !


innovation_station

love it !  ;D

well said!  ;D

ist!

mk1 you realize im gonna have to make a video of this now ... lol

i was just given a 1000 foot spool of 14ga solid coated green wire ..  i have like 40 of those steel cores ..  i will bang 1 and do as you reccomend ... 

;D ;D ;D ;D


To understand the action of the local condenser E in fig.2 let a single discharge be first considered. the discharge has 2 paths offered~~ one to the condenser E the other through the part L of the working circuit C. The part L  however  by virtue of its self induction  offers a strong opposition to such a sudden discharge  wile the condenser on the other hand offers no such opposition ......TESLA..

THE !STORE IS UP AND RUNNING ...  WE ARE TAKEING ORDERS ..  NOW ..   ISTEAM.CA   AND WE CAN AND WILL BUILD CUSTOM COILS ...  OF   LARGER  OUTPUT ...

CAN YOU SAY GOOD BYE TO YESTERDAY?!?!?!?!