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Re: Spark Gap Sustaining Current (fwd)
---------- Forwarded message ----------
Date: Sat, 29 Sep 2007 20:24:19 +0000
From: David Rieben <drieben@xxxxxxxxxxx>
To: Tesla list <tesla@xxxxxxxxxx>
Cc: drieben@xxxxxxxxxxx
Subject: Re: Spark Gap Sustaining Current (fwd)
Hi Bert,
All that I can say is, "WOW" ! That's a really superb
explanation of this subject matter for a "layman" as myself,
although my mind is still trying to "absorb" all that you've
said ;^) You should have been a professor, if you weren't.
David Rieben
-------------- Original message --------------
From: "Tesla list" <tesla@xxxxxxxxxx>
>
> ---------- Forwarded message ----------
> Date: Sat, 29 Sep 2007 14:16:17 -0500
> From: Bert Hickman
> To: Tesla list
> Subject: Re: Spark Gap Sustaining Current (fwd)
>
> Tesla list wrote:
> > ---------- Forwarded message ----------
> > Date: Thu, 27 Sep 2007 12:55:46 -0500
> > From: Crispy
> > To: tesla@xxxxxxxxxx
> > Subject: Spark Gap Sustaining Current
> >
> > Hello,
> >
> > I have a quick question about spark gaps. How much current is required
> > to sustain an established arc in a spark gap in "dead air"? Let's say
> > that there are two tungsten contacts about an inch apart, and an arc is
> > ignited by a voltage of a little over 20kV. Say that the ambient
> > temperature is room temperature and that there is not significant
> > airflow through the gap other than that which is generate by the gap's
> > heat itself. Is the sustainability of the arc purely a function of
> > current through it?
>
> Hi Chris,
>
> The short answer to your first question is YES.
>
> A somewhat longer answer:
> There's nothing simple about sparks, arcs, or plasma in general. The
> answer depends on current limiting by the external circuit, whether you
> have AC or DC and, if AC, the frequency. AC and RF arcs must be
> reignited after each current zero crossing. This makes low frequency AC
> arcs easier to extinguish than DC arcs. It also depends on the electrode
> shape and material, and the orientation of the gap (vertical arcs behave
> somewhat differently than horizontal ones).
>
> Arcs require the formation of a "cathode spot" - a small incandescent
> region at the cathode root of the arc - which injects large numbers of
> electrons to help sustain the arc. For most metals, a true arc occurs
> when the current reaches a level of amperes or, at most, tens of
> amperes. The actual electron injection mechanisms into an arc differs
> significantly between electrodes made from refractory metals versus non
> refractory metals. A refractory metal, such as tungsten, develops a
> stable incandescent cathode spot which liberates large numbers of
> electrons via thermionic emission. Non-refractory metals such as copper
> (with boiling temperatures below the point of substantial thermionic
> emission, ~ 3000 degrees C), are "cold cathode" materials. The cathode
> spots of these metals are in constant motion, with electrons being
> liberated via field emission. The high E-field is created between
> between the cathode and positive ions just above the cathode (called the
> cathode sheath).
>
> If you're able to limit short circuit current to tens of milliamperes,
> the voltage across the gap climbs sharply. Gap voltage vs current begins
> to follow a curve that is heading towards a low current glow (or corona
> discharge) or to the initial spark-over voltage of the gap. In an AC
> arc, the reignition voltage also begins to climb, ultimately approaching
> the initial breakdown voltage for the gap or a stable glow/corona
> discharge point. This phenomenon can be seen for low current AC arcs
> (such as from a low current NST's), where the arc really can't be drawn
> out much further than the point of initial breakdown before being
> extinguished.
>
> If the short circuit current from the power source is even further
> decreased, once the gap breaks down, the low impedance of the spark
> drops the voltage below the gap's instantaneous sustaining voltage.
> Without using a careful low capacitance design approach, this usually
> leads to unstable operation when short circuit current is limited to a
> few milliamperes or less. The result is usually repetitive spark-like
> discharges as the circuit operates as a relaxation oscillator. The
> discharge tries to follow the sharp negative resistance curve heading
> towards an arc, but the voltage across the gap collapses and kills the
> arc, so the circuit cannot achieve stable "arc-like" operating point.
>
> > If so, in such a theoretical gap, how much
> > sustaining current would normally be required?
> >
> > Thanks,
> > Chris
> >
>
> Again, it depends on the external circuit and whether you apply AC or DC.
>
> For a HV DC source, with little capacitance, resistively current
> limited, you can actually follow the progression of the gap breakdown
> process from the glow discharge, abnormal glow (for refractory metals),
> down to a full fledged arc discharge. Once you have exceeded the
> breakdown threshold for the gap, the "sustaining current" simply is
> either the stable or unstable operating point(s) defined by the external
> circuit. Simply stated - for a resistively current limited low
> capacitance DC HV source, there is no minimum sustaining current once
> you've successfully bridged the gap. Practically speaking, the discharge
> ceases being "arc-like" in air once you go below a few mA and, for most
> circuits, the discharge is no longer stable.
>
> For a low frequency HV AC source, reignition after each current zero
> becomes increasingly difficult as you begin lowering shirt circuit
> current, and a single failure to reignite after a zero crossing leads to
> almost complete dielectric recovery of the gap. Again this is with
> milliamperes of current - higher than for the DC case with an identical
> gap. Because of the shorter zero crossing intervals and capacitive
> effects, an RF arc is somewhat harder to extinguish, with "sustaining
> current" falling somewhere between low frequency AC and DC case.
>
> As with all things arc-ish and spark-ish, YMMV... :^)
>
> Bert
> --
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