NASA: STILL FROM 16MM AUTOMATIC MOTION PICTURE
CAMERA. ANNOTATION ADDED BY UNKNOWN THIRD PARTY.
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Note A: One astronaut
casts a significantly longer shadow than the other. This could only
happen if they were being lit by a nearby light source, or possibly
from different light sources. Since the sun is the only significant
source of light on the lunar surface, their shadows should be equally
long. [David Percy]
We can reject the multiple light source theory without too much
difficulty. Notice that the astronauts are closely in line with each other
with respect to the light source. A light set to illuminate one could
hardly avoid also illuminating the other. This would cause each
astronaut to cast two shadows, one from each light source.
A very close light source would also cast shadows of different
length, but not as shown. As the picture below shows, the longer
shadow would be cast by the astronaut farthest from the light. In the
photo in question, the near astronaut casts the longest shadow.
Much of conspiracist photographer/filmmaker David Percy's argument
is based on lengths and directions of shadows cast in photographs.
His argument in this case and many others presumes a flat level
surface upon which to cast shadows. The foreground of the image is
darker than the background, indicating that the terrain is not at all
level. The ground slopes downhill away from the camera to roughly the
center of the image, then begins to slope upward again and receives
more direct sunlight.
CLAVIUS
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CLAVIUS
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With 3D graphics we can see the behavior of objects casting shadows
onto variously sloping surfaces. In the rendering on the left the two
cylinders are exactly the same height, but are on different sides of a
shallow depression. The light source shines at a low angle from some
distance away.
The rendering on the right is from directly overhead and shows clearly
that the shadow cast by the cylinder on the "downhill" side is
distinctly longer than the other shadow. Note also that the ground
exhibits exactly the same kind of variable lighting that we see in the
photograph, helping confirm that this (not some mysterious extra light
source) is the phenomenon at work, although we note that the variation
might also be caused by the astronauts churning up darker subsurface
soil.
Other frames from the
same film show the astronauts casting shadows of equal length as they
move about. They are obviously moving toward and away from a large
light source. [David Percy]
AULIS PUBLISHING, FROM NASA
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Again Percy relies heavily on his presumption that the ground is
essentially flat. The shadow of someone walking around on rough
terrain would also lengthen or shorten. A low sun elevation would
greatly amplify such differences in shadow length.
In this case, we look at the photo at the top of the page and
consider that the astronaut on the right is standing atop a small rise
and the astronaut on the right is at a lower elevation, casting his
shadow on roughly level ground.
In the second photo we consider that one astronaut has stepped
back while the other one has gone some distance away, probably to
take photographs. He is no longer on the small rise and is now also
casting a shadow onto relatively level ground.
Percy's argument that the shadow lengths are caused by variations
in illumination angles due to a nearby (versus infinitely distant)
light source would also require the shadows to diverge slightly in the
second photgraph. But we observe the shadows to be virtually
parallel, converging slightly due to the perspective we would expect
from such a camera angle. But if Percy is correct, the distant
astronaut's shadow should point farther away; the shadows should
appear to diverge.
Photos of the area show
it to be flat. [David Percy]
AULIS PUBLISHING, FROM NASA AS11-40-5905
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Percy presents the photograph on the right. His argument appears to
be, "It's flat because it looks flat to me." The horizon isn't flat,
but that's anywhere from a hundred feet to five miles away from the
area we're interested in. (Distances were very hard to judge on the
moon, and are impossible to judge from single still photos.)
The question to ask is whether we'd see any evidence variation if
it really were there. What would be sufficient evidence of terrain
variation? We might expect to see variations in the lighting.
Terrain less directly lit might appear darker, as we noted above. We
might also look for hard-edged discontinuities that represent the
crests of rises. We might also look for objects that disappear
abruptly as if behind rises. We might also look for shadows that
behave a bit differently than expected.
Observing some or all of these would suggest a variation in
terrain. But would failing to observe them prove that the
terrain was flat? No. In logic this is called the fallacy of inverse
implication, encapsulated by the maxim, "Absence of evidence is not
evidence of absence." Just because Percy fails to observe our
expected indicators of slope doesn't mean no such slope exists. There
are cases in which the slope exists without leaving indicators.
The general problem of contour extrapolation in these still photos
is covered here. For this specific photo, we note little color
variation, no hard-edged discontinuities. It's unclear whether the
flag pole disappears behind a rise or simply into the soil.
NASA: AS11-40-5873
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The shadow in the foreground is cast by the solar wind collector. As
shown, the collector is simply a rectangular sheet of material hung
on a pole to collect particles from the solar wind. The shadow shows
it was correctly deployed facing the sun as directly as possible.
Correctly aligned, the rectangular top should cast a
nearly-perfect rectangular shadow. But in Percy's proof photo we see
the tip of the collector's shadow become gradually thinner, as if it
were falling on a patch of ground sloping away from the camera.
The strongest evidence, however, of irregular terrain is the
shadow of the flag and flagpole. They are mostly invisible in Percy's
version of the photo, but we can examine it more closely in a larger
image.
NASA: AS11-40-5873, ANNOTATIONS ADDED
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The white line represents a theoretical straight line that would be
the shadow cast by a perfectly straight flagpole. But it is plain
that the shadow is not perfectly straight. Since Percy cannot argue
that the object casting the shadow is curved, nor can this effect be
produced by artificial light sources, we have no choice but to
conclude that the surface onto which this shadow is being cast is not
planar.
The evidence Percy presents to establish a planar surface is
ironically the best evidence of a non-planar surface. A
significant change in the angle of the lunar surface can be found in
the area onto which the shadows in question are being cast. In fact,
the flagpole shadow very closely resembles the theoretical model
explored above in our computer renderings. When viewed from a high
angle (e.g., the lunar module cockpit) shadows cast onto non-planar
terrain vary in length, but not necessarily in shape. Linear objects
cast linear shadows. But when viewed from a low angle, such shadows
display a change in shape or direction, such as we see in the proof
photo. Linear objects can cast curved or bent shadows.
The irregularity in the terrain corresponds exactly to the
location in which the variations in shadow length are observed. We
further note that the flagpole shadow cannot be produced by any of the
hoax methods Percy has suggested, and in fact can only be produced by
a lunar surface irregularity. This obvious irregularity has the shape
and orientation that would produce the shadows observed in the photo
in question.
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