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B Stationary frames of reference

  1. Jan 25, 2017 #51

    Nugatory

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    Staff: Mentor

    Yes. Google for "Foucault's pendulum".
    The orbiting earth is changing its direction in space, but not spacetime - it's following a straight line through spacetime.
     
  2. Jan 25, 2017 #52

    PeterDonis

    Staff: Mentor

    There isn't any "proportion" in the reading on the accelerometer; it's just one reading.

    As Dale said, it would not.

    Yes, but this doesn't mean what you appear to think it means.

    Consider an accelerating rocket in flat spacetime (no gravity) with 1 g proper acceleration. You can stand on the floor of this rocket just as you would stand on the surface of the Earth, and if the only information you have is what you can measure inside the rocket, you have no way of telling whether it is in fact at rest on the Earth's surface or accelerating through free space at 1 g. That is the equivalence that Einstein was talking about.

    But if we now consider what this tells us about a "gravitational field", it tells us that the acceleration you feel standing on the surface of the Earth is not due to "gravity"; it's due to the surface of the Earth pushing up on you, just as the acceleration you feel in the rocket in free space is due to the rocket pushing up on you. In other words, what the equivalence told Einstein was that "gravity", at least in the sense of "acceleration due to gravity", is not a force at all. It's just an artifact of the way you choose your reference frame.
     
  3. Jan 25, 2017 #53
    But if you had an accelerometer in the rocket, could you not just take a reading, because were you not all saying that accelerometers do not measure gravity? I was assuming that the 1g was supposed to be equivalent to the gravity on Earth, rather than a measurement of its spin. Was that assumption wrong?
     
  4. Jan 25, 2017 #54

    Dale

    Staff: Mentor

    Yes, you can take an accelerometer reading in a rocket. It will measure the proper acceleration, as always.

    Accelerometers do not measure the acceleration due to gravity nor to inertial forces. They only measure proper acceleration, which is never due to gravity or inertial forces.

    What? I don't understand this question.
     
  5. Jan 25, 2017 #55

    PeterDonis

    Staff: Mentor

    1 g is a proper acceleration; it is the acceleration you feel standing on the surface of the Earth. But just from that measurement alone, you can't tell whether you are feeling 1 g proper acceleration because you are standing on the surface of the Earth, or because you are accelerating in flat spacetime. You need other information to distinguish those two cases.

    The 1 g proper acceleration by itself tells you nothing about spin. Other measurements (such as the gyroscopes Dale mentioned) are needed if you want to know about spin.
     
  6. Jan 25, 2017 #56
    What would be causing the 1g proper acceleration if you were standing on the surface of the Earth? We might just be going around in circles here, and you meaning that if there was no Earth but you were in free fall due to gravity that there would be no acceleration, and therefore claiming that gravity does not cause proper acceleration. Whereas I have been discussing taking measurements with an accelerometer while standing on Earth, and talking about the acceleration due to gravity. The reason I was considering a proportion of the reading, in the situation, to be due to gravity, was because if the Earth had been mainly hollow for example, it would have curved spacetime less, and therefore there would be less gravity, and therefore the measured acceleration standing on the surface of the Earth would have been less. The greater reading being due to greater gravity. Do you think that perhaps that is the issue. For example would there be less measured acceleration using an accelerometer when standing on the surface of a large sphere if the sphere had less mass?


    But part of the accelerometer reading would be due to the Earth spinning though would it not?

    Also regarding the Earth orbiting the Sun, Nugatory mentioned:

    "The orbiting earth is changing its direction in space, but not spacetime - it's following a straight line through spacetime."

    Can I assume that straight lines in spacetime depend on velocity?
     
  7. Jan 25, 2017 #57

    Dale

    Staff: Mentor

    The normal force of the ground pushing up on the bottom of your feet

    I understood that and I am pretty sure that @PeterDonis did also. None of the proper acceleration is due to gravity, it is all due to the normal force. Note that the proper acceleration is upwards, which is the direction of the normal force, not the gravitational force.
     
  8. Jan 25, 2017 #58
    But would that not be linked to gravity. For example if you were standing on a sphere with less mass you'd experience less acceleration because there would be less gravitational force.
     
  9. Jan 25, 2017 #59

    Dale

    Staff: Mentor

    The reduced proper acceleration is due to the reduced normal force. In this scenario both the normal and the gravitational forces changed together. Consider instead situations where the normal force is different but the gravitational force is the same, or vice versa.
     
  10. Jan 25, 2017 #60
    In the scenario I gave, with large spheres of differing mass, the reduction in normal force is due to the reduction in gravitational force is it not? So if the gravitational force was increased the normal force would be also would it not (given the context where there would be a normal force)? Making the gravitational force an indirect cause if not a direct cause (in that scenario).
     
    Last edited: Jan 25, 2017
  11. Jan 25, 2017 #61

    Dale

    Staff: Mentor

    If you have two possible sources of an effect and you wish to determine which one causes it then you must vary them independently. Think of scenarios where the gravity is constant, but the normal force is different. Like a man standing on a glass floor which breaks. Gravity is the same before and after, but the normal force changes to zero after. What does the accelerometer record?
     
  12. Jan 25, 2017 #62

    Boing3000

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    Gold Member

    If you want to think into GR framework you have to realize that gravity is not a force. "Gravitating" if what things do when no force apply to them (<= inertial), when they are in "free-fall", like (falling)apple, satellite, the earth (the whole system you included). It is also said those inertial things follow straight line following (curved)spacetime.

    On the ground your free-fall is stopped by the ground exerting a force on you and your accelerometer.
     
  13. Jan 25, 2017 #63
    So if you were in the jury at a court case where a person had attached a rope to a winch and placed it through a hole in a wall, and wrapped it around a person and then turned the winch on such that the person was killed, that you would accept the argument that the person turning on the winch was not the cause of the death? The defence argument being that the basis to determine whether the forces generated by the winch (which the defendant was responsible for) contributed to the death, you would have to consider whether there had been a paper wall, and their conclusion that the forces generated by the winch being unrelated to the effect (the death). Their argument that the source (the wall) of the effect (of the person dying) was one that the defendant had no causal connection to.

    Could the gravitational force not influence the calculated normal force in a situation?

    Why did the glass floor break, was there a force that prior to its breaking it was resisting?
     
    Last edited: Jan 25, 2017
  14. Jan 25, 2017 #64
    I am using language pretty loosely here. I could change the term gravity for mass if you like, but one term seems to be useful in highlighting the point you are getting to. As in the influence of mass on "Gravitating".

    Why does the ground differentiate on the force it exerts. To explain what I mean, imagine
    Scenario 1) I touch a wall with my finger (the wall does not break)
    Scenario 2) A car drives into a wall (the wall does not break)

    With architecture is there no consideration of the force being placed on the wall? And a concept of the amount of resistance that the wall can give?
     
  15. Jan 25, 2017 #65

    PeterDonis

    Staff: Mentor

    The Earth's surface pushing up on you. Just as in the accelerating rocket in flat spacetime, the 1g proper acceleration you feel is due to the rocket's floor pushing up on you.

    This is true, but it still doesn't mean the acceleration you feel standing on the Earth's surface is "due to gravity". It just means that, if the Earth's mass were smaller so it curved spacetime less (more precisely, curved spacetime less at the same radius from the center), the Earth's surface wouldn't push up on you as hard. "Gravity" here is the curvature of spacetime, but it isn't curvature of spacetime that's pushing up on you, it's the Earth's surface.

    No. Once more: in GR, gravity is not a force. It's spacetime curvature. Spacetime curvature doesn't push on anything.

    Of course not. The person is killed because the rope exerts a force on their neck and breaks it. But that doesn't contradict the fact that in GR, gravity is not a force. It isn't gravity that breaks the person's neck. Or spacetime curvature either.

    Yes, and you need to stop doing that. We are talking about physics, and you need to use language precisely in physics or you will not understand things properly.

    You keep on giving examples of things that aren't gravity exerting force on something, and then trying to argue that somehow that means gravity is a force. Can you see the problem?
     
  16. Jan 25, 2017 #66
    I am thinking of Gravity as the measured influence of "mass" on gravitation. What is the theory behind why the Earth's surface, or a wall, or a table, pushes up more in some places than others? With a spring bed for example I would expect it to be that there was more force on some areas than others (but as I understand the respondents there is no difference in force on areas). I was assuming that the curvature created a force on a body which lead to motion of that body, which on contact with another could be resisted or not (if the resistance was not enough) by that body.

    While I am grateful for your help, I had assumed that it was the burden of the more educated in physics (that were trying to help the less educated) to try to empathise with what the less educated were getting at and explain (as there could be loads of less educated that were thinking the same way). As opposed to them being pedantic until the less educated phrased the question in a way that gave the more educated no option to misunderstand what was being asked.
     
    Last edited: Jan 25, 2017
  17. Jan 25, 2017 #67
    So change in motion requires no force? Does not curvature perpetuate at the speed of light and does it not have an effect?

    But if you have two possible sources of an effect (the wall or the winch) and you wish to determine which one causes it then should you not (as Dale suggested) vary them independently. Think of scenarios where the winch is constant, but the normal force of the wall is different. Like a man being pulled through a paper wall which breaks. The winch force is the same before and after, but the normal force (of the paper wall) changes to zero after.
     
    Last edited: Jan 25, 2017
  18. Jan 25, 2017 #68

    PeterDonis

    Staff: Mentor

    In other words, you are thinking of gravity as the measured influence of mass on gravity? That doesn't even make sense.

    In GR, the best way to think of "gravity" is as spacetime curvature. That is the "gravity" that does not depend on your choice of coordinates, and that appears in the laws of physics.

    General relativity, whose laws--the Einstein Field Equation--are based on spacetime curvature and stress-energy (which is how what you ordinarily think of as "mass", i.e., the source of "gravity", appears). You solve the EFE under particular conditions that you are interested in, and that tells you the geometry of spacetime. Then you look at different possible worldlines in that spacetime geometry, and the laws tell you what proper acceleration (how much "pushing up") will be experienced by an object following that worldline.

    "Change in motion" depends on your choice of coordinates. So it can't appear in the laws of physics.

    Changes in curvature propagate at the speed of light. But for a gravitating body like the Earth, the spacetime curvature is, to a very good approximation, static, i.e., unchanging, so there's nothing to propagate.

    Yes, spacetime curvature has an effect. See above.

    I don't understand. How is the person in your scenario killed? I thought it was the rope attached to the winch breaking their neck. Is it the winch pulling them through the wall and killing them by contact with the wall?

    Assuming the latter is the case, I still don't see the point. The person wouldn't have been pulled through the wall if the winch hadn't been turned on. So whoever turned the winch on is responsible for their death. The fact that a wall made of something less sturdy wouldn't have killed them is irrelevant. And this whole scenario seems to me like a quibble; we're not talking about legalistic reasoning, we're talking about physics.

    If the winch isn't turned on, the force of the wall on the person is zero regardless of what the wall is made of. So the causal factor that varies the force is the winch. But this whole argument is still, as I said above, a quibble.
     
  19. Jan 25, 2017 #69

    PeterDonis

    Staff: Mentor

    We can try, but if you are unable or unwilling to learn the correct language in which to describe what you are getting at, this is often not possible. Basically what we have been telling you is that you are using the wrong concepts, and your language reflects that. We are trying to get you to change the concepts you use, from ones that don't work to ones that work. It won't do any good for you to continue to insist on us answering your questions using your concepts, because they don't work.

    In conclusion: this is a "B" level thread, and I think we have answered your questions as well as they can be answered in a "B" level thread. To briefly summarize:

    (1) In GR, gravity is not a force. It's spacetime curvature. Only things that are actually felt as proper acceleration are forces in GR.

    (2) The laws of physics don't include things that depend on your choice of coordinates. That includes "rest", velocity, and coordinate acceleration.

    To go into more detail about these things would require a thread at a level higher than "B", which would require you to have the background for a discussion at that level. I would suggest working through a GR textbook: Sean Carroll's online lecture notes are a good choice to start with:

    https://arxiv.org/abs/gr-qc/9712019

    This thread is closed.
     
  20. Jan 25, 2017 #70

    Dale

    Staff: Mentor

    You seem to be trolling now rather than looking for help learning GR. If you want to learn these concepts then you are going to have to pay attention with an open mind. And if you want us to help you then you will have to respond helpfully rather than sarcastically.

    This thread is closed temporarily. PM me with a sincere analysis of the normal force, gravitational force, and accelerometer reading, and I will reopen it.
     
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