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RE: Gap Question
Original poster: "Luke" <Bluu-at-cox-dot-net>
If the current goes up and the channel widens would that give the
channel less resistance because it now has a larger cross section to
travel through?
Like a piece of 28Awg wire having a higher resistance than a piece of
10Awg wire. The larger cross sectional area decreases its resistance.
Thanx
Luke Galyan
Bluu-at-cox-dot-net
http://members.cox-dot-net/bluu
-----Original Message-----
From: Tesla list [mailto:tesla-at-pupman-dot-com]
Sent: Monday, February 23, 2004 5:01 PM
To: tesla-at-pupman-dot-com
Subject: RE: Gap Question
Original poster: "Malcolm Watts" <m.j.watts-at-massey.ac.nz>
Hi Luke,
Nice try:
On 23 Feb 2004, at 7:28, Tesla list wrote:
> Original poster: "Luke" <Bluu-at-cox-dot-net>
>
> Bart:
> I thought about what you said with the negative resistance thing. May
> I lay something out that does not use real values but values
> arbitrarily picked out to make the example simple. I may be way off
> base but would like some in put. I think the idea has merit.
>
> I was thinking it may appear to be negative resistance but may not
> really be. Maybe it is like having a gap that has different
> dimensions when it heats up.
>
> Let me try to explain. And before anyone starts quoting some actual
> values try to look past that for about 30 seconds just to get the
idea
> I am getting at. Then fire away with all the real value stuff.
>
> Let's pretend for the example that:
> 1: The breakdown voltage of air is 100 volts per inch. And
> 2: That an arc has a certain amount of resistance per length.
> But that resistance follows a logarithmic curve or spiral.
> What I mean by this is like that of a logarithmic spiral.
> Where the curvature gets tighter and tighter as the spiral
> Curves inward.
> Now draw a line from the center outward. Measure the distance
> from center to where the line intersects each turn of the
> spiral.
> So say 0.5=3, 1=6, 1.5=12, 2=24, 2.5=48, 3=96, 3.5=192 etc.
>
>
> Imagine only the spark gap the primary coil and the capacitor.
> And all this is at the time of break down for the gap.
>
> Ok say we have a gap of 3" that would give 300 volts for break down
> and
> >From the curve above the resistance of that arc would be 96 ohms.
> Using plain old ohms law you would get a current of 3.125 amps.
>
> Now let's say the electrodes get hot. Instead of just looking at it
> like The voltage breakdown got lower, lets assume it acted as though
> it made the distance between the electrodes closer, which would have
a
> lower breakdown voltage. I think of it like the hot air/ions
whatever
> might act as an extension of the electrodes making them have a larger
> diameter and therefore be closer together.
>
> So lets say that the heat involved made the gap ACT as though the
> distance was 2.5" even though the measured distance might actually be
> 3".
>
> This would give a break down voltage of 250 volts and a resistance of
> 48 ohms. So the current would be 5.2 amps. So the voltage the cap
> charged to was 50 volts lower but the current went up. Not because
of
> negative res. but because the electrodes in a way are now closer.
>
> So is it that the gap has a negative resistance?
> Or is it that the heat makes the gap act as though it has,
> different dimensions (a closer spacing)?
> so the gap acts different?
>
> I know this might be reaching a little but I think there is some
logic
> in it I would like some opinions on.
>
> If what I am saying had some truth to it then if one did not take
into
> account the gap acted as if the distance were closer it would seem
> that there was indeed negative resistance.
>
> Any thoughts? And keep in mind I am no math whiz. Just laying out a
> concept and hoping to get some qualified people thinking / talking so
> I can hear bout it.
What really happens is that as gap current goes up, the width of the
arc increases. A spark tries to keep to as narrow a channel as
possible at "normal" atmospheric pressure. The width of the channel
at a particular current is defined by the number of ions (current
carriers) that can be formed in the channel cross-sectional area, the
molecular density of air being the arbiter. In effect, the arc
behaves in a saturable manner, extending no wider than it has to. If
the available current goes up, the channel widens to boost the cross-
sectional area. So it is the fact that the channel is able to widen
without limit that gives an arc the negative-resistance
characteristic. In an inductor analogy, it is as though the inductor
core increased in cross-sectional area as the applied magnetizing
force tried to take it beyond saturation. In a camera flashtube
however, the ability of the arc to widen is restricted by the
diameter of the flashtube (ions that can be formed per unit area) so
after initially exhibiting a negative resistance, the tube truly
saturates and stays there meaning that beyond a certain current, the
arc reverts to a positive or normal characteristic, highly desirable
since you don't want the storage capacitor seeing voltage reversals.
The short distances involved in Tesla spark gaps don't have a
huge influence on the gap dissipation.
Malcolm
<snip>