I’ve set the scene with a very short story because a mental picture
must be worth almost a thousand words.
——-
A space traveler heading to a destination on the Earth’s surface
approaches the Earth and the Moon, and while still some distance
away, will be drawn to the barrycenter of the Earth-Moon orbits,
which is of course the pivot point about which the two components
are in freefall around each other. That point being somewhere near
1700km beneath the Earth’s surface. But the traveler will be
increasingly drawn toward the Earth’s center as he approaches the
Earth.
The traveler’s destination is a point on the equator which is
exactly aligned through the barrycenter along a line which is
perpendicular to a line scribed between the Earth-Moon centers.
. . I
. I .
Earth. –I-.——————OMoon
. . I
^Destination
When the traveler arrives at his destination he knows that he is
not in freefall around the pivot point and thus expects that gravity
will not be pulling him directly to the Earth’s center, but will be
pulling him to a point slightly shifted toward the Moon, located
somewhere along the line joining the Earth-Moon centers.
With the apparatus described below, my intention was to pinpoint
the location of that point.
UP
Mirrors / – - / -<<<HeNe laser source.
. x
< WEST S = . . EAST >
c = = . .
r = = = ()=/ – - /
ee = = <->
n =
DOWN
" () " is a fiber optic collimator lense.
" x " represents the knife edge pivot point for the
pendulum that carries the movable mirror.
>From the diagram it should be fairly obvious that if the mirror
which is carried on the movable arm shifts 633nm, that action will
record one fringe shift on the screen. The arm length was .3 meters.
A 633nm shift over the .3 meter arm length expands to 13.5 meters
at the Earth’s center. Through one complete revolution of the
Earth’s surface (with the apparatus) I had expected to find **many**
more than one fringe shift across the screen.
Seismic activity was reasonably overcome by suspending the whole
apparatus between tension springs. The springs were covered with
grease to stop an endless resonance within the spring setup.
Induction motion dampeners succeeded in bringing the never ending
movement of the arm and the suspended apparatus into some sort of
order.
There were some positive readings, but they were canceled by just
as many negative readings. The inaccuracy could all be attributed
to temperature variation. With that problem under control, I could
now have confidence in what I was seeing.
As the apparatus passes through one alignment with the barrycenter
the pendulum will be leaning slightly toward the Moon, and will have
caused a fringe shift in one direction. The barrycenter alignment
on the other side of the Earth finds the apparatus pointing in the
opposite direction relative to the Moon, so the fringe shift is in
the opposite direction. In a 24 hour test, movement of the pendulum
couldn’t be detected, within the accuracy of the setup. The pendulum
was clearly pointing to a point near the Earth’s center which hadn’t
moved more than a few meters from the center. I found this quite
bewildering.
Disregarding the fact that the Moon’s influence on the arm would
be reduced according to the arm’s pointing angle when the apparatus
intersects with the barrycenter line. This is my rather simplistic
math justification for all of this;
Since there are 81 Moon masses per 1 Earth mass, the Moon’s gravity
rate at an Earth distance from the Moon is ((1/81)*9.8)/384403^2
= 8.188E-13 m/sec^2. The ratio between the pull of gravity
between the two is 8.188E-13/9.8 = 8.355E-14 to 1 . The mirror
at the end of a 1 meter pendulum would be shifted toward the Moon
by 8.355E-14m. That only represents 535 nanometers at the Earth’s
center, which isn’t even 1 HeNe laser wave length. It seems
ridiculously minute.
I’m posting this prior to dismantling the setup just in case I’ve
missed something.
–
Max Keon
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