Frame drag to accelerate spaceships?

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Discussion Overview

The discussion revolves around the concept of frame dragging near rotating black holes and its potential to accelerate spaceships. Participants explore theoretical implications, comparisons to gravity assists, and specific proposals like Robert Forward's ideas on using frame dragging for propulsion.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that a spaceship orbiting a rotating black hole could gain additional acceleration due to frame dragging, questioning whether there is a maximum speed gain similar to gravity assists or if infinite acceleration is possible.
  • Robert Forward's proposal involving a toroidal structure for acceleration via frame dragging is mentioned, though details are not fully recalled by all participants.
  • One participant notes that geodesics in the Kerr metric maintain constants of motion, suggesting that a particle falling into a black hole would not gain energy upon re-emergence.
  • There is a discussion about whether the constraints of energy and angular momentum apply to both the spaceship and the black hole, with a specific inquiry into whether a falling body can "borrow" energy from the black hole.
  • Another participant highlights the ergosphere's role, indicating that benefits from frame dragging require non-geodesic actions, such as firing rockets or utilizing the Penrose Process, to achieve acceleration.
  • Concerns are raised about the effectiveness of Forward's toroidal concept, with assertions that a freely falling object would not experience a change in energy after passing through the torus.

Areas of Agreement / Disagreement

Participants express differing views on the effectiveness of frame dragging for acceleration, with some supporting the idea of potential gains and others challenging the feasibility based on principles of general relativity. The discussion remains unresolved regarding the practical implications of these theories.

Contextual Notes

Limitations include the dependence on specific definitions of energy and angular momentum, as well as the unresolved nature of how frame dragging interacts with geodesics and non-geodesic actions.

makc
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As far as I understand, a spaceship going around rotating black hole should gain additional acceleration due to frame drag. Right? So, would there be max speed gain, like in gravity assist, or could you accelerate infinitely? Thanks.
 
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Robert Forward had some proposal to accelerate objects via frame dragging, but I don't recall the details. A large torus of some sort, I believe.
 
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As far as I understand, a spaceship going around rotating black hole should gain additional acceleration due to frame drag. Right? So, would there be max speed gain, like in gravity assist, or could you accelerate infinitely? Thanks.
Geodesics in the Kerr metric have the usual constants of the motion: energy and angular momentum. A particle falling in from infinity would re-emerge with the same energy it went in with.
 
is it not the same as with gravity assist, these constraints should apply to spaceship and black hole together?

200px-Gravitational_slingshot.svg.png


I guess I'm asking if falling body can borrow some of black hole energy.
 
More on Forward's scheme -- which I never quite followed. (The original was in "Indistinguishable from Magic", a collection of non-fiction essays.).

The General Relativistic Antigravity Machine consists of a torus of dense mass which is turning inside-out like a smoke ring. A mass with this motion, according to Einstein’s theory, "drags the metric" through the center of the torus. Unidirectional general relativistic forces arise which are equivalent to gravity, and may be used to neutralize planetary surface gravity or as a space propulsion system.

17.5B.gif
 
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Ok, I guess I really do need some education here. I've seen Forward's device before - in fact I remember a rather long Am J Phys article he wrote - but I never realized before how much I just don't get the point of it. It all comes back to my earlier comment:
Geodesics in the Kerr metric have the usual constants of the motion: energy and angular momentum. A particle falling in from infinity would re-emerge with the same energy it went in with.
This continues to be true in Forward's torus, does it not? It's stationary and axially symmetric. Hence by general principles, a particle traveling along a geodesic will have constant energy and angular momentum. So you can't simply drop a particle through the hole and expect it to be accelerated!

The ergosphere in the Kerr metric only works a benefit if you do something nongeodesic while inside it: either (a) fire your rockets or (b) split in two, as in the Penrose Process. I'd have to say the torus is similar - on a freely falling object the frame dragging has only a temporary effect, and when you emerge from the other side and move away you'll find to your disappointment that nothing has changed. :frown:
 

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