[Prev][Next][Index][Thread]

Modeling a magnifier




----------
From:  Malcolm Watts [SMTP:MALCOLM-at-directorate.wnp.ac.nz]
Sent:  Sunday, March 15, 1998 4:49 PM
To:  tesla-at-pupman-dot-com
Subject:  Re: Modeling a magnifier

CORRECTION (sorry)

> Hi Antonio, all,
> 
> > From:  Antonio C. M. de Queiroz [SMTP:acmq-at-compuland-dot-com.br]
> > Sent:  Wednesday, March 11, 1998 10:08 PM
> > To:  Tesla List
> > Subject:  Re: Modeling a magnifier
> > 
> > Malcolm Watts wrote:
> > 
> > >             It is beginning to look as if a number of aspects of
> > > Antonio's modelling is correct.
> > 
> > Well, physics cannot be so wrong... Your system uses L3>>L2, right?
> > (What are the inductance and capacitance values?)
> 
> L2 was 355uH,  L3 is about 5uH from memory (notes at home).

That should have been 5mH of course :(
    A little further information: The driver secondary has a 1:1 
aspect (lowest possible Cself for its diameter) and self-resonates at 
around 3.5MHz. It is wound with heavy 80-strand LITZ wire. Mean 
diameter is about 6.7".  Primary/s fit inside.

> > In this condition C2 is small, and the system can only resonate
> > producing beats while the primary is connected, as in the first model
> > that I proposed. As Jim McVey observed, it is impractical to have a 
> > distributed C2 such that L2*C2=(L2+L3)*C3, what would produce beats 
> > after the opening of the spark gap (second model, with C2), if L2<<L3.
> > There is another possible working behavior for the magnifier, that
> > is the primary/secondary system being used as a CW generator, but
> > most of the members appear to agree that this is practically impossible.
> > (Or not?)
> 
> Not in a cap discharge system because the primary decrements as the 
> cap empties. No reason why not if the primary is driven from a CW 
> source. In this case, system Q limits final amplitude.
> 
> Malcolm