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Other
researcher's published
literature on Brown's Gas states that 1 liter of
water would make 1866.6
liters of
Brown's Gas. Normal di-atomic H2:O2 is 933.3
liters of gas per liter of water and Brown's Gas
displaces more volume than normal because of
it's mon-atomic constituent. The above example
proves the volume increase and my experiments
with my machines and Yull Brown's own machines
prove it. Further, an old researcher in Brown's
Gas just came up with a further method to prove
the volume increase caused by the mon-atomic
portion of the gas. He weighed it in a fixed
volume at a fixed pressure and
temperature.
If we assume
that we are getting significant amounts of H and
O in our torch gasses, what would happen to them
when they burn?
If we had all H
and all O, our flame wouldn't have to be very
hot to "self propagate" because the flame
wouldn't have to be putting all that energy into
splitting the H2 and O2, before it could burn.
So we'd have a "cold" flame, right? And it is
universally
noted that Brown's Gas burns with a very low
temperature flame.
If we had all H
and all O with no H2 and O2, and we reduced
straight to water. We would go from a greatly
expanded gas to liquid, a reduction of 1860
times, with little of the expansion caused by
heat. This would produce quite a vacuum, don't
you think? And if our "flame" was doing this,
the reaction would be an "implosion",
right?
And if the H and
O went directly into forming water, we'd have
(for four moles of H and two moles of O) 442.4
Kcal of available energy, instead of only 115.7
Kcal available from 2H2:O2.
The extra
available atomic-level energy could account for
some of the strange effects of Brown's Gas, like
sublimating tungsten, which requires
temperatures close to those found on the surface
of the sun. "Normal" 2H2:O2 flames can't reach
these temperatures.
The special
imploding high energy reaction could be tapping
unknown effects, explaining some other effects
of Brown's
Gas, like its ability to make clean laser-like
holes in wood, metal and
ceramics. As
well as the capability of changing temperature
when applied to different materials.
During a Brown's
Gas mon-atomic hydrogen (H) and mon-atomic
oxygen (O) flame, we don't have to add any
energy because the molecules are already in
their simplest and highest energy atomic form.
This means that "perfect" Brown's Gas can have
3.8 times the possible 'heat' energy that an
"ordinary" H2 and O2 flame has (442.4 Kcal/115.7
Kcal).
Thus we can get
'plasma' type temperatures and effects as we
weld, because the potential atomic energy is
there, even if it doesn't show up as
heat.
  
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