On the noton of reference frames force and acceleration

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Discussion Overview

The discussion revolves around the concept of inertial reference frames in the context of Newtonian mechanics and general relativity. Participants explore how to determine whether a force is acting on an object, the implications of acceleration, and the definitions of inertial frames in different frameworks.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants question how one can know a force is applied without observing acceleration, suggesting that the conclusion of a force acting on an object typically arises from its acceleration.
  • One participant defines an inertial reference frame as one where an accelerometer at rest reads zero, while others challenge this definition in the context of Newtonian mechanics.
  • There is a discussion about the role of gravity in defining inertial frames, with some arguing that a frame influenced by gravity can still be considered inertial in general relativity but not in Newtonian mechanics.
  • Participants express confusion over distinguishing between fictitious forces and real forces, particularly when acceleration is observed.
  • Some argue that the definitions of inertial frames differ between Newtonian mechanics and general relativity, with implications for how gravity is treated in each framework.
  • A suggestion is made for an alternative definition of inertial reference frames that could apply to both Newtonian and Einsteinian contexts, focusing on the absence of fictitious forces.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the definitions and implications of inertial frames, with multiple competing views remaining on how to interpret the concepts within Newtonian mechanics versus general relativity.

Contextual Notes

There is a lack of clarity regarding the assumptions underlying the definitions of inertial frames, particularly in relation to gravity and fictitious forces. The discussion highlights the complexity of these concepts and the potential for confusion among participants with varying levels of understanding.

  • #31
kev said:
If you fell straight down from space towards the surface of the Earth a passing satellite will appear to be moving a straight line relative to you. This is because when you are falling you are a true inertial observer.
Really?
 
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  • #32
MeJennifer said:
Really?

I think it is true in a small enough region such as within a small falling elevator. It is not true if the elevator is large as the curvature of spacetime that is present around a sperical gravitational body becomes noticeable. This is where the equivalence principle breaks down, because a free falling elevator should be the same as a elevator far away from any gravitational sources and you would not expect to see any curved trajectories with no gravity present.

To be honest, it bothers me a lot that it seems impossible to find a situation where the equivalence principle holds exactly. If we define the principle as not being able to perform any experiments in an accelerating elevator/rocket that would detect whether the acceleration was due to a rocket or gravity, then I have not been able to find a single example where that is exactly true and it is only justified by making the elevator very small. Basically, the tidal effects always give the game away.
 
Last edited:
  • #33
kev said:
If you fell straight down from space towards the surface of the Earth a passing satellite will appear to be moving a straight line relative to you. This is because when you are falling you are a true inertial observer.
MeJennifer said:
Really?

Hi Jennifer,

I have found an example where my statement is exactly true, even over quite a large area and the apparent straight line motion of the orbiting particle to a free falling observer is shown in the attached gif. The box represents a falling elevator that is dropped from just above the Earth's surface and falls through a tunnel drilled right through the Earth. Such an elavator would fall to the other side of the Earth and then come back again following simple harmonic oscillation and would continue bobbing up and down indefinitely if there was no atmsosphere present creating friction. The period of the oscillating elevator in free fall would be the same as the period of a satellite in very low Earth orbit (again assuming no atmosphere). In the animated gif the apogee of the elavator is designed to coincide with the satellite passing the elevator. You can see from the gif that in this particular example it would not matter how wide the elevator is or even if the observer in the elevator looks out the windows, the satellite always seems to follow a stright path from his point of view. In a more realistic example of a satellite in high orbit and with a large elevator, some slight curvature of the satellites path would probably be noticed by the free falling observer in the elavator.
 
  • #34
kev said:
Hi Jennifer,

I have found an example where my statement is exactly true, even over quite a large area and the apparent straight line motion of the orbiting particle to a free falling observer is shown in the attached gif. The box represents a falling elevator that is dropped from just above the Earth's surface and falls through a tunnel drilled right through the Earth. Such an elavator would fall to the other side of the Earth and then come back again following simple harmonic oscillation and would continue bobbing up and down indefinitely if there was no atmsosphere present creating friction. The period of the oscillating elevator in free fall would be the same as the period of a satellite in very low Earth orbit (again assuming no atmosphere). In the animated gif the apogee of the elavator is designed to coincide with the satellite passing the elevator. You can see from the gif that in this particular example it would not matter how wide the elevator is or even if the observer in the elevator looks out the windows, the satellite always seems to follow a stright path from his point of view. In a more realistic example of a satellite in high orbit and with a large elevator, some slight curvature of the satellites path would probably be noticed by the free falling observer in the elavator.

Ummm..here is the gif that should have been attached to my last post..not sure how it came unattached...it was there in there in the preview.. :confused:

In case it is not obvious, the left part of the animated gif is the point of view of a non inertial observer watching the satellite follow a circular path while the right side of the gif is the point of view of the inertial observer in the free falling elevator who considers the elevator to be stationary. m
 

Attachments

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    lineorbit.gif
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  • #35
calculus_jy said:
i think i understand, so they define a frame which is far away from all body as inertial frame, and an accelerometer will determine where is accelerate relative to the defined inertial frame, then you can tell whether the forces on a body is fictiticious or not, generally you cannot conclude whether you are accelerating or a body is accelerating if you do not define a first inertial frame!? correct, if correct then i completely get the fundamental idea of relativity
How about a homemade accelerometer? If you hold a bowling ball three feet in front of you and release it, measure its (coordinate) acceleration. If you're at rest in an inertial frame, the bowling ball will float in front of your face. If the bowling ball accelerates (coordinate) relative to you, then you're in an accelerated frame.

Seriously, Wikipedia has info: http://en.wikipedia.org/wiki/Inertial_frame_of_reference.
They also have articles on acceleration (proper and coordinate), fictional forces, and almost anything else you can think of.

Al
 

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