(I am but an egg.)
On Friday, June 30, 2023 at 11:37:37 AM UTC-7, vallor wrote:
Thought experiment:
Einstein's elevator.
In an elevator sitting on the ground on Earth, gravity would be measured
as higher near the floor than the ceiling, given sufficiently sensitive
equipment. (1/d^2)
The strength of gravity is equal in contractile curvature.
There is no inner gravity drop off. Feynman was a problem
where he replaced original GR by inner drop off.
At a BH how can there be Feynman's inner drop off gravity?
He said it would go to zero. So how could gravity in a BH
do it?
Accelerating the elevator at 1G, there won't be the difference in "gravity" from
the ceiling to the floor.
Accelerating is increased speed it is not the force of gravity.
Motion is like force. It can get weight.
Mitchell Raemsch
What does that mean with regards to "locality"? Is that just a measure of
how sensitive the instruments you're carrying are? Or...?
(I am but an egg.)
--
-v
[ This is a repost of the following article:
]
[ From: vallor <vallor@cultnix.org>
]
[ Subject: Question regarding an elevator
]
[ Newsgroups: sci.physics
]
[ Message-ID: <u7n7da$2jpl7$1@dont-email.me>
]
Thought experiment:
Einstein's elevator.
In an elevator sitting on the ground on Earth, gravity would be measured
as higher near the floor than the ceiling, given sufficiently sensitive equipment. (1/d^2)
Accelerating the elevator at 1G, there won't be the difference in
"gravity" from the ceiling to the floor.
What does that mean with regards to "locality"? Is that just a measure
of how sensitive the instruments you're carrying are? Or...?
(I am but an egg.)
Perhaps the concept of "locality" might have something
to do with "how sensitive are your instruments"... What do you think?
Thanks,
-Scott
cc: comp.ai.shells, where the discussion first began
fu2: sci.physics
[ This is a repost of the following article: ] [ From: vallor <vallor@cultnix.org> ] [ Subject: Question regarding an elevator ] [ Newsgroups: sci.physics ] [ Message-ID: <u7n7da$2jpl7$1@dont-email.me> ]
Thought experiment:
Einstein's elevator.
In an elevator sitting on the ground on Earth, gravity would be measured
as higher near the floor than the ceiling, given sufficiently sensitive equipment. (1/d^2)
Accelerating the elevator at 1G, there won't be the difference in
"gravity" from the ceiling to the floor.
What does that mean with regards to "locality"? Is that just a measure of how sensitive the instruments you're carrying are? Or...?
I was referring to the observation that Einstein made that one
couldn't tell the difference from within an elevator in either
situation. I was pointing out that with sensitive enough instruments,
you can tell the difference.
So, it seems to me that for such
gedanken-experiments one uses elevators of infinitesimal size!
vallor <vallor@cultnix.org> writes:
I was referring to the observation that Einstein made that one couldn't >>tell the difference from within an elevator in either situation. I was >>pointing out that with sensitive enough instruments,
you can tell the difference.
The gravitational potential at the bottom of the elevator is
V( x )= -GM/x, where
x is the distance from the center of the Earth to the bottom
of the elevator,
G is the gravitational constant, and M the mass of the Earth.
At the top, it's
V( x + h )= -GM/( x + h ), where
h is the height of the elevator.
So the difference is
-GM/( x + h )-( -GM/x )= GMh/( x^2 + hx )~ GMh/x^2.
This difference can be made as small as wanted by reducing the height
of the elevator. We also should reduce the size of the floor as
otherwise the direction of the force differs between different points
of the floor. So, it seems to me that for such gedanken-experiments
one uses elevators of infinitesimal size!
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