2006
DOI: 10.1119/1.2198880
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An intuitive approach to inertial forces and the centrifugal force paradox in general relativity

Abstract: As the velocity of a rocket in a circular orbit near a black hole increases, the outwardly directed rocket thrust must increase to keep the rocket in its orbit. This feature might appear paradoxical from a Newtonian viewpoint, but we show that it follows naturally from the equivalence principle together with special relativity and a few general features of black holes. We also derive a general relativistic formalism of inertial forces for reference frames with acceleration and rotation. The resulting equation … Show more

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Cited by 12 publications
(27 citation statements)
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“…For such an orbit, a greater outward thrust is required to maintain its orbit as the orbital speed increases. (See [8] and the references therein for further discussion, and [7,9] for the generalization to stationary axisymmetric case. )…”
Section: Black Holes and Their Photon Orbitsmentioning
confidence: 99%
“…For such an orbit, a greater outward thrust is required to maintain its orbit as the orbital speed increases. (See [8] and the references therein for further discussion, and [7,9] for the generalization to stationary axisymmetric case. )…”
Section: Black Holes and Their Photon Orbitsmentioning
confidence: 99%
“…For such considerations we refer to a companion paper [16]. There we rely on simple principles such as time dilation and the equivalence principle and derive the relativistic three-dimensional form of the inertial force equation (68) using no four-covariant formalism at all.…”
Section: Discussionmentioning
confidence: 99%
“…which at first sight appears to be identical to (8), derived in flat space-time. It must be kept in mind, however, that the gradient operator in general coordinates assumes the form [19]…”
Section: Entropy In General Coordinatesmentioning
confidence: 99%
“…where the rightmost term is the entropy due to the stress-energy-momentum of all the particles, and the factor of 1/2 is included in the first term to account for duplicate pairs of particles in the sum. Equation (19) can be simplified upon noticing that the sum over λ j in the first term is just the total field potential λ (P i ) at the position P i of U i . Using this observation puts (19) in the form…”
Section: Wwwann-physorg 4 Entropy Of a Weakly-gravitating Matter DImentioning
confidence: 99%