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The fact that I have debated this subject
with a few scholars is somewhat surprising to me. I will try to summarize my opinion on the
subject. Those who argue with me say that no
energy is
transferred by gravity. No work is done. I disagree. I believe
they are arbitrarily picking a flawed external preferred point of reference when
they choose the source of gravity. An accelerated object can only use itself
as the judge of energy being transferred to it.
It is
my opinion that energy imust be expended/transferred to cause
an object to accelerate. Accelleration is deviance from a stable
inertial state. Motion or lack thereof is entirely relational to an
observer.
I will
postulate that an object in orbit around a gravity source would
immediately travel in a straight line and take on a stable inertial
state if gravity was removed. Additionally I will postulate that if
gravity were momentarily flashed on for a moment near an object in a
stable inertial state, that object's inertial state would change.
This is the same as saying a "still" object would begin moving
toward the gravity source and an object moving perpendicular to the
source would deviate from its course by a minute degree. All of
these actions require a transfer of energy.
An object in a stable orbit must constantly
have energy applied to it to cause it to deviate from a natural
straight-line course into space. It is easier to understand if
an orbit is broken into parts. In this first image, imagine a frictionless and
weightless environment. The object traveling is a billiard ball and
we instantly transfer an equivelent to the starting energy using another
billiard ball at each of the arrow points.
The
above model will help you segment an orbit into its constituent
parts. Because a circle has an infinite number of points, I
will give you a second diagram to help you start to make the
transition toward infinite.
The above model should allow you to see
how I have come to the conclusion that the energy that is
transferred to an object in a stable orbit during one revolution is
equal to the initial
energy required to accelerate the object to its orbit speed times
Pi. Given that orbits are not perfect circles I'm not
certain of the exacting accuracy of the calculation but I believe it is
a close approximation.
That's fine for orbits but what
about objects resting on the ground?
I believe energy is constantly being
transferred to objects at rest on the ground as well. I believe work
is being done by gravity to an object you believe only has a
balanced force applied to it. To say that you have a balanced force
you
must pick a preferential reference frame. Selection of a preferential
reference frame regularly confounds science and is a very large
part of why misconceptions about relativity are not cleaned up even in the
face of evidence.
Take for example that two rockets and
an
observer are the only objects in the universe. If the
two rockets thrust against eachother, without knowledge of the actual
thrust output of each of the rockets, the dominant rocket is determined by the motion
of the observer.
If you observe from the perspective of the
sun, the motion of an object on earth that we percieve to be
stationary you will see a
very odd and regularly changing path. An inertially changing object.
The question to be asked is: What is causing the
object to deviate from a straight-line path? What is doing the work of pulling
it through space?
Force =
Mass * Accelleration.
Work =
Force * Distance (preferential
inertial frame required)
I postulate that an object in a state of
acceleration is moving regardless of the viewer's reference
frame. All objects on earth, including those seemingly on the ground
are in a state of acceleration
measurable by an accelerometer. Regardless of that assumption, it is
undenaible that all objects held in Earth's gravity are being
pushed and pulled far outside of any straight line trajectory. Work is done.
Energy is transferred.
Well then how much energy is being
transferred to an object at rest on Earth?
I would assume that using an accelerometer
at a given point on the earth you could find the intensity of the
acceleration of a given object. Perhaps some pointing up and down to
find an average would be needed. Simply assume it is an
object under linear
accelleration by some force other than gravity. You should know
its mass already; so simply pick an interval and solve
for the energy required to accelerate an object of that mass for that
period of time.
Here's a little side thing just to tickle your fancy. I
call it Pi R Scalable.
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