What is Linear Frame Dragging in General Relativity?

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SUMMARY

Linear frame dragging is a phenomenon in general relativity where a test mass near an accelerating massive object experiences a slight acceleration in the same direction, creating the illusion that the universe is accelerating oppositely. This effect, while theoretically valid, is less discussed and harder to verify experimentally compared to rotational frame dragging. The terminology may also be referred to as "inertia induction," as noted by Dennis Sciama. The relationship between linear frame dragging and the geodetic effect remains unclear, despite references in literature such as Wikipedia and Brian Greene's "Fabric of The Cosmos."

PREREQUISITES
  • Understanding of general relativity principles
  • Familiarity with frame dragging concepts
  • Knowledge of the Kerr metric in physics
  • Awareness of Mach's principle and its implications
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  • Research the Kerr metric and its role in frame dragging
  • Study the geodetic effect and its relationship to frame dragging
  • Explore Dennis Sciama's paper "On the Origin of Inertia"
  • Investigate experimental methods for measuring linear frame dragging
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Physicists, students of general relativity, and anyone interested in advanced concepts of spacetime and gravitational effects.

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"Linear frame dragging"?

wikipedia at http://en.wikipedia.org/wiki/Frame_Dragging#Frame_dragging_effects says:
Linear frame dragging is the similarly inevitable result of the general principle of relativity, applied to linear momentum. Although it arguably has equal theoretical legitimacy to the "rotational" effect, the difficulty of obtaining an experimental verification of the effect means that it receives much less discussion and is often omitted from articles on frame-dragging (but see Einstein, 1921)

(Naty1 has drawn attention to this to this in a Library comment.)

What is this referring to?

Is it a generally accepted terminology, or is it just wikipedia's wishful thinking? :confused:
 
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Linear frame-dragging is the effect that if a test mass is near to an accelerating massive object, its frame of reference is slightly accelerated in the same direction, giving the impression that the rest of the universe is accelerating slightly in the opposite direction. This is consistent with the Mach's principle idea that if the whole universe were accelerating uniformly in the same direction, local reference frames would also accelerate with it, making the acceleration unobservable.

This linear frame-dragging effect is of course tiny in comparison with the ordinary gravitational acceleration and is even more difficult to measure than rotational frame-dragging.

I don't know where the terminology came from; I've heard it before, but I've also heard this effect being referred to as "inertia induction" (by Dennis Sciama, in his fascinating paper "On the Origin of Inertia").
 


If anyone knows a physical explanation for frame dragging, I'd sure be interested. Wiki derives the ffect from the Kerr metric: does the interaction arise from a specific piece of the Einstein stress energy tensor??

Also, how is frame dragging related to the geodetic effect; Wikipedia has a cross reference with frame dragging, but the relationship isn't clear..

http://en.wikipedia.org/wiki/Geodetic_effect
 


When I read a few pages about rotational frame dragging in Fabric of The Cosmos by Brian Greene, I see I wrote myself a note:

"seems to follow the equivalence principle of acceleration and "g", but here via
v = w(r)" ...not too far fetched...

Brian Greene says :
...just as a massive objects warps space and time so a rotating object drags space and time around it...(it) implies, for example, an asteroid freely falling toward a rapdily rotating neutron star or black hole will get caught up in a whirlpool of spinning space and be whipped around as it journeys downward."
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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