Space-time & Gyroscopic Effect: Arthur's First Post

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Discussion Overview

The discussion revolves around the effects of gravity on spacetime and how these effects might influence the behavior of rotating gyroscopes, particularly in relation to the Earth's axial tilt and its orientation with respect to the Sun. Participants explore theoretical implications within general relativity and consider practical observations in the solar system.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Arthur proposes that if gravity bends spacetime, a rotating gyroscope should exhibit effects related to this curvature, particularly in the context of the Earth's axial tilt and its orientation towards the Sun.
  • One participant agrees that curvature affects everything but argues that the Earth does not maintain its tilt-orientation with respect to the Sun due to the nature of spacetime curvature.
  • Another participant clarifies that while the Earth behaves somewhat like a gyroscope, the general relativistic effects necessary for maintaining tilt orientation are too weak in the solar system, citing Thomas precession and geodetic precession.
  • A different viewpoint suggests that the Earth won't maintain its tilt-orientation with respect to distant stars after one orbit, emphasizing the minimal effects in the Sun-Earth system.
  • A participant references the Gravity Probe B experiment, which aimed to measure the frame-dragging effect on a gyroscope, indicating that such experiments relate to the discussion but are not directly about the Earth's axial tilt.

Areas of Agreement / Disagreement

Participants express differing views on the implications of spacetime curvature on the Earth's axial tilt and gyroscopic behavior. While some agree that curvature affects gyroscopes, there is no consensus on the practical outcomes or the significance of these effects in the solar system.

Contextual Notes

Participants note that the general relativistic effects discussed are weak in the context of the Earth-Sun system, and there are unresolved aspects regarding the specific conditions under which these effects might be observed.

Arthur95
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My first post (and from a mobile), so please pardon any impropriety...

If gravity bends spacetime, wouldn't we expect to see that effect on a rotating gyroscope? Using the Earth's axial tilt as an example: we have seasons through the year as we orbit, but shouldn't the curved spacetime created by the sun mean the Earth would maintain its tilt-orientation with respect to the sun all year (eg: northern hemisphere always inclined toward the sun for the 'endless summer')?

I imagine there is conservation of momentum / inertia or something coming into play here, or more likely I just don't understand this spacetime stuff!

Thanks for indulgence!
Arthur
 
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Welcome to PF;
If gravity bends spacetime, wouldn't we expect to see that effect on a rotating gyroscope?
Yes - the curvature would affect everything.
Using the Earth's axial tilt as an example: we have seasons through the year as we orbit, but shouldn't the curved spacetime created by the sun mean the Earth would maintain its tilt-orientation with respect to the sun all year (eg: northern hemisphere always inclined toward the sun for the 'endless summer')?
No ... as you have seen, this does not happen.
The Earth is tilted wrt the line, drawn through curved space, from the Earth to the Sun.

Where the curvature is more extreme across the diameter of a planet, you do get one face always to the primary ... the effect is called "tidal locking". Which you probably already know ;)
 
Last edited:
Arthur95 said:
If gravity bends spacetime, wouldn't we expect to see that effect on a rotating gyroscope? Using the Earth's axial tilt as an example: we have seasons through the year as we orbit, but shouldn't the curved spacetime created by the sun mean the Earth would maintain its tilt-orientation with respect to the sun all year (eg: northern hemisphere always inclined toward the sun for the 'endless summer')?

The Earth isn't exactly a gyroscope but it is to the extent that it doesn't matter for this discussion. What you're describing is possible in principle in GR but certainly not in practice in our solar system because the necessary general relativistic effects due to the Sun, that is, Thomas precession and geodetic precession, are far too weak; in fact Thomas precession would be entirely absent since the Earth is in free fall and hence doesn't accelerate relative to local inertial frames.

However let's consider a Schwarzschild black hole of mass ##M## and a gyroscope accelerating on a circular trajectory at a special radius (##r = 3M##) at which light can orbit. If the gyroscope axis is initially aligned in the radial direction, so that it points towards the black hole, then it will remain pointing towards the black hole during its entire trajectory around the black hole.

If you want I can point to some intuitive explanations of this effect.
 
Arthur95 said:
but shouldn't the curved spacetime created by the sun mean the Earth would maintain its tilt-orientation with respect to the sun all year
No, it just means that it won't exactly maintain its tilt-orientation with respect to the distant stars after one orbit. But as others said, this effect is tiny for the Sun Earth system.
 
Something distantly related but similar have been done experimentally in Gravity probe B experiment:
http://en.wikipedia.org/wiki/Gravity_Probe_B

They had almost perfect gyroscope rotating from pole to pole around Earth. They tried to measure tiny influence of frame dragging of Earth on the gyroscope.
 

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