Sep 07,
2006
Lunar Craters—a Failed
Theory
When seeking to test a
hypothesis, it is helpful to start with clear and undeniable
facts. But when the impact theory is applied to the
prominent lunar “rayed crater,” Tycho, the theory fails even
the most obvious tests.
Certainly the most conspicuous
crater on the Moon is Tycho in the southern hemisphere. (For
context, we have placed a full Hubble Telescope image of the
Moon
here). The crater is some 85 kilometers in
diameter, displaying enigmatic “rays” that extend at least a
quarter of the way around the moon.
The central
peak, said to have been formed by a “rebound” of
subterranean material, rises about 2 kilometers above the
crater floor. Planetary scientists suggest that the flat
floor of the crater (seen
here) was formed by the pooling of melted
material.
But the idea
that an impact would create such an extensive pool of molten
rock finds no support in impact experiments or in
high-energy explosions. Not even an atomic explosion creates
a flat melted floor of this sort. The force of the explosion
shocks and ejects material. It does not hold the material in
place to “melt” it into a lake of lava.
When the
brilliant engineer, Ralph Juergens, considered the lunar
craters Tycho and Aristarchus, he noted the distinct
features of electrical discharge. He wrote in 1974, “…If
Aristarchus and Tycho were produced by electric discharges,
their clean floors would be just about what one would
expect. The abilities of discharges to produce melting on
cathode [negatively charged] surfaces and generally to
‘clean up’ those surfaces have been remarked upon since the
earliest experiments with electric discharges”.
Juergens
envisioned an interplanetary arc between the Moon and
an approaching body (for his analysis, he summoned the
planet Mars). While an instantaneous explosion does not have
time to create a lava lake, an electric arc involving a
long-distance flow of current between two approaching
bodies, “would persist beyond the instant of any initial
touchdown explosion”, leaving material melted in place.
Juergens saw
Tycho as a “cathode crater”, and he drew special attention
to Tycho’s “spectacular system of rays”. These, he
suggested, are the very kind of streamers an electrical
theorist would look for—a signature of the electron pathways
that triggered the Tycho discharge.
Of course, the
astronomers’ consensus today is that the streamers are the
trails of material ejected from the crater into narrow paths
over extraordinary distances. But the “rays”, Juergens
noted, have no discernible depth, while material exploding
from a Tycho-sized crater “would at least occasionally fall
more heavily in one place than in another and build up
substantial formations. But no one has ever been able to
point out such a ray ‘deposit’”.
The presence of
the narrow rays over such long distances, according to
Juergens, is “all-but-impossible to reconcile with ejection
origins. Enormous velocities of ejection must be postulated
to explain the lengths of the rays, yet the energetic
processes responsible for such velocities must be imagined
to be focused very precisely to account for the ribbon-thin
appearance of the rays”. In fact, this challenge has found
no answer in more recent scientific exploration. No
experimental explosion at any scale has ever produced
anything comparable to the well-defined 1500-kilometer
“rays” of Tycho.
Even more
telling is the fact that the rays are punctuated with
numerous small craters. An early explanation was that "some
solid material was shot out with the jets and produced
'on-the-way' craters". But such narrow trajectories for
secondary impactors are an absurdity under the mechanics of
an explosion. And the total volume of ejected material
needed to form the secondary craters along Tycho's rays,
would amount to some 10,000 cubic kilometers – an amount of
material entirely inconsistent with careful measurements
indicating that practically all material excavated from
Tycho's crater has been deposited in its rim. However, the
ray elements, terminating on small craters, are the very
markers that today’s electrical theorists have cited
repeatedly as definitive evidence of an electrical discharge
path. As Wallace Thornhill has so often observed, such
discharge streamers frequently terminate at a crater.
In fact, this is exactly what Gene Shoemaker found when
investigating the puzzles of Tycho—"...many small secondary
craters, too small to be resolved by telescopes on earth,
occur at the near end of each ray element."
When compared to
an imagined sphere of the Moon’s average radius, the
surrounding highland region occupied by Tycho is more than
1200 meters above the “surface” of that sphere. The crater
site appears to be at the summit, or very close to the
summit, of terrain that trends downward in every direction
away from the site for hundreds of kilometers. For the
impact theory, this location can only be an accident. But
for the electrical theorists, the elevation on which Tycho
sits is not accidental. Lightning is attracted to the
highest point on a surface. (That is, of course, the
principle behind lightning arrestors placed on the pinnacles
of tall buildings).
Though
astronomers see Tycho’s rays as material ejected from the
focal point of an impact, a mere glance at the picture above
is sufficient to make clear that not all of the streamers
radiate from a central point. Is this surprising? A
mechanical impact has a single focal point and
cannot explain these offset rays. Juergens noted that
they "diverge from a common point, or common focus, located
on or buried beneath the western rim of the crater." The
electrical interpretation of Tycho sees the streamers as
paths of electrons rushing across the lunar highlands to the
highest point, where it launches into space to form the
lightning "leader" stroke. The high point is destroyed in
the process. The powerful lightning "return stroke" that
forms the Tycho crater comes minutes afterwards and focuses
on the nearest high point, a few kilometers to the east. In
support of this explanation, the crater Tycho is surrounded
by a dark halo of ejecta that blankets the extensive ray
system, laid down earlier.
Tycho's crater
rim rises about one kilometer above the surrounding terrain
and the crater walls exhibit terraces (shown
here) that are not characteristic of high
energy explosions. However, such terracing is
observed in innumerable instances of electrical discharge
machining. (See the large terraced crater in the picture on
the right
here). This terracing may be due to the fact that
electrical current flows in plasma in the form of twisted
filament pairs – rather like a double helix. So the
terracing is caused by the cutting action of the rotating
current filaments on the crater wall. Indeed, some lunar
craters exhibit bilateral corkscrew terracing –
another observation inexplicable by the impact model, but
remarkably consistent with the principle of an arc
constituted of twin rotating “Birkeland Currents”.
While it is
possible to get a “rebound peak” close to the center of an
explosion, such a peak is not typical. In the electrical
cratering experiments by plasma physicist CJ Ransom, (as
seen
here) central peaks were often the norm. As long
ago as 1965, attention was drawn to the similar incidence of
craters with central peaks in lunar craters and laboratory
spark-machined craters. They seem to be an effect of the
rotating current filaments, which may leave the center of a
crater relatively untouched.
The electrical
theorists find great irony in the many examples of earlier
researchers who pointed to the electrical properties of
phenomena that official science eventually learned to
ignore. In 1903, W. H. Pickering, in his book The Moon,
suggested that electrical effects could account for the
narrow paths of Tycho’s “rays”, and he drew a direct
comparison to the streamers seen in auroral displays. But as
occurred so frequently in the twentieth century, evidence of
electrical activity in space was ignored because it found no
place in gravitational cosmology or in the curricula of
astronomers and geologists.
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