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ISO longer sparks at less i




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From:  Dale Hall [SMTP:Dale.Hall-at-trw-dot-com]
Sent:  Wednesday, June 17, 1998 9:06 PM
To:  Tesla List
Subject:  ISO longer sparks at less i


ISO = In Search Of

MultiTap_MultiGap,  Multi<>Cap_Single_Tap,  Multi=Cap_Multi<>Tap

Progressive_Tap_MultiGap,  Progressive_Tap_Gap

To list:
I am pondering methods to achieve longer spark discharges (SD) while reducing
required input power.  My theory is that a long SD's may be achieved by
providing properly timed multiple close spaced primary energy dumps with a
delay before the next burst. The nature of the SD's will change from hundreds 
of widely varying in length to fewer, each of a longer length thus requiring less
overall average input power to achieve the fewer but max length SD's.  
(rates: DC=infinitely variable <1 to >20?,  ac=50/60 unipol or 100/120 bipol)

For the AC input case it would be nice for 2*120=2.4KW to provide SD's of 6' to
up to 20' maybe more. I think this can be achieved. The trade off should be the 
number of cap dumps per second must be redistributed (bunched) with the 
overall number reduced. In the RSG case increasing the break rate increases 
SD length provided there is adequate input power available. At 480 bps / 60 Hz 
= 8 SD's per cycle (4 in pos cycle 4 in neg cycle) or one every 16.67/8 = 
2.08ms which represents the time the Pri Cap has to charge before it is 
switched to the Pri inductor. The challenge is to come up with an approach that
allows multiple closely spaced switched charges (2 for now more later) in ~10us
up to ~1ms bursts occuring only once (all pos or all neg) or twice per cycle
(oneof ea polarity to see if bipolarity is a factor in producing longer SD's) -
separatedby 8.3ms or 16.7ms. The RSG implementation could be an inner row
for the extra cap positioned to align just after the outer row breaks.  
A differential concentric adjustment scheme would be desirable. 

The DC input case would allow more flexibility in time between bursts allowing 
further reduction of input power vs SD length as it needn't keep step with the 
varying sine wave. Its implementation could consist of vacuum switches and 
timed electronic activation. The DC case could be set up for unipolarity or 
bipolarity. DC should permit very long SD's at very low average input power
since the time between bursts is unconstrained.

The general approach is to use two (more later) primary charge sources to allow
two (or more) close spaced primary energy dumps. This requires two charge 
sources (NST's), two Discharge Caps of equal value and two (or more) switch 
paths to two spaced taps. The first dump at "before streamer" resonance is 
followed by a second at a little higher inductance tap (further along the turn
= lower Fres) to account for a slightly larger Sec top capacitance streamer
which slightly lowers Fres, corrected with a little more inductance.
The second streamer will hopefullly build onto and enlarge the first streamer.

Alternately two slightly different capacitances and two (or more) switch paths
to the same tap could affect the same result. 

Unknown for either is if it is possible to switch multiple dumps of high energy
close together without one triggering the other. Then again this coupled 
triggering might be usable and desirable in the quest for adding subsequent 
charge to the existing streamer. 

Has anyone tried this ? likely to ? comments ?   Dale,  Redondo Beach, Calif