About man falling into grate paradox

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    Falling Paradox
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Discussion Overview

The discussion revolves around the "man falling into grate paradox," exploring the implications of relativity on the behavior of a rod under uniform acceleration and the resulting stresses and bending. Participants examine the physical significance of bending in different reference frames, the nature of rigidity, and the effects of simultaneity in relativistic contexts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question the general acceptance of the idea that bending occurs in the rod's rest frame and whether this bending has physical significance, suggesting that no stress should occur if all parts of the rod are pushed simultaneously.
  • Others reference Bell's spaceship paradox to argue that even if the rod appears unbent in one frame, it could still break due to relativistic effects.
  • A participant proposes that rigid rods do not exist and suggests modeling the rod as a "wet noodle," which would sag and potentially catch on the grate.
  • There is a discussion about the nature of bending, with some arguing that if different parts of the rod are pushed at different times, this could lead to actual bending rather than just apparent bending.
  • Some participants explore the implications of removing the floor under a moving rod and how this relates to the relativity of simultaneity, questioning whether the rod would fall normally.
  • One participant suggests that the non-simultaneous pushes in the rod's frame would make the rod more vertical, allowing it to fit into the grate.
  • Another participant emphasizes that if there is no force on one end of the rod while there is on the other, the transmission of forces is limited, complicating the notion of rigidity.

Areas of Agreement / Disagreement

The discussion contains multiple competing views regarding the physical behavior of the rod under acceleration and the implications of relativity. Participants do not reach a consensus on whether the bending is actual or apparent, or on the nature of rigidity in relativistic contexts.

Contextual Notes

Participants express uncertainty about the physical significance of bending and stress in different frames, and the discussion highlights the limitations of classical models of rigidity in relativistic scenarios.

  • #31
jartsa said:
Well I had a problem with the energy of the supposed stress, where does it come from, particularly in the still standing observers frame.

In all frames, there will be some period of time when the rod is sticking out over the edge, so that one end is supported by the ground underneath and the other end is not. This is just an ordinary cantilever, no different in principle from a balcony on the side of a building. The rod doesn't even have to moving relative to the hole for there to be stress in the rod: gravity is pulling the projecting end of the rod down into the hole, and is being resisted by stress forces within the rod.
 
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  • #32
jartsa said:
Well I had a problem with the energy of the supposed stress, where does it come from, particularly in the still standing observers frame.
I don't know what you mean by the still standing observer's frame.

The energy for the stress comes from work done on the rod - a great force (10^15 Newtons) does work on it, moving it distance (1 millimiter). The energy (work) applied to the rod, stressing it, is on the order of a terajoule (about 1% of the energy released by the Nagasiki atomic bomb). In rod frame (the only relevant frame for analyzing stress), this forice is not applied simultaneously, but from right to left (assuming the rod is moving left to right).

Following earlier suggestions, I proposed a piston pushing the rod down the hole. This has many advantages over gravity. Dealing with gravity (from a source that would have to specified) on an object moving near c relative to it, with gravity needing to be extremely strong field, would be a complex problem in GR. Also, the piston ensures that the rod is seen to remain horizontal in the grate frame.
jartsa said:
But maybe that problem can be solved.

Let's see ... two rapidly spinning discs are pushed so that they slam together and fuse together, the result is a slowly spinning object. The spinning energy of the two disc system turned into stress energy of the discs, which stress energy turned into heat when the discs collided.

Is the above correct?

The discs are identical, they have identical angular momentum, and they collide with the flat parts first. And all velocities are relativistic.

The above is correct, but not very relevant the rod pushed through a grate hole.
 
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  • #33
Nugatory said:
In all frames, there will be some period of time when the rod is sticking out over the edge, so that one end is supported by the ground underneath and the other end is not. This is just an ordinary cantilever, no different in principle from a balcony on the side of a building. The rod doesn't even have to moving relative to the hole for there to be stress in the rod: gravity is pulling the projecting end of the rod down into the hole, and is being resisted by stress forces within the rod.
No the ground never pushes the rod. In the man falling into grate paradox "It is assumed that the rod is entirely over the grate in the grate frame of reference before the downward acceleration begins simultaneously and equally applied to each point in the rod"

Quoted part is from the wikipedia.
 
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  • #34
jartsa said:
No the ground never pushes the rod. In the man falling into grate paradox "It is assumed that the rod is entirely over the grate in the grate frame of reference before the downward acceleration begins simultaneously and equally applied to each point in the rod"

Quoted part is from the wikipedia.

Of course, the key point being simultaneously in the grate frame = not simultaneously in the rod frame. Thus, for a given element of the rod, the element to its right (for example) accelerates down and to the left before any force or acceleration is applied to the given element.
 
  • #35
jartsa said:
No the ground never pushes the rod. In the man falling into grate paradox "It is assumed that the rod is entirely over the grate in the grate frame of reference before the downward acceleration begins simultaneously and equally applied to each point in the rod"

Quoted part is from the wikipedia.

Ah - right - yes, as I've seen the paradox described in other sources that part isn't always specified.

It's still something of a red herring though, because if you choose to use the grate frame you're just choosing to use a frame in which the problem is harder to analyze, hence leading to the apparent paradox. If you're going to insist on starting with the grate frame, you might try drawing the world lines of three points (each end and the middle of the rod) in such a way that the acceleration will be simultaneous in the grate frame. You'll see that these are also the world lines of those three points if the rod is being bent by the progressive application of force from one end to the other it its rest frame.
 

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