Gravitational Radiation Power of Object in Forced Circular Motion

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SUMMARY

The discussion focuses on the formula for gravitational radiation power from a single object in forced circular motion, specifically addressing volumetric invariant mass densities in both low density Newtonian and high density general relativistic limits. The challenge lies in the lack of conserved momentum in a single body scenario, contrasting with the established formulas for pairs of rotating bodies where the dipole moment vanishes. The conversation highlights the potential for solutions in linearized approximations and emphasizes the significance of the quadrupole moment in gravitational radiation. Relevant resources include Wikipedia's gravitational wave page and a detailed site from Caltech.

PREREQUISITES
  • Understanding of gravitational radiation concepts
  • Familiarity with Newtonian and general relativistic physics
  • Knowledge of quadrupole moments in gravitational theory
  • Basic principles of forced circular motion
NEXT STEPS
  • Research gravitational radiation power formulas for single objects in forced circular motion
  • Explore linearized approximations in general relativity
  • Study the role of quadrupole moments in gravitational wave emission
  • Examine case studies of gravitational radiation from binary systems
USEFUL FOR

Physicists, astrophysicists, and researchers interested in gravitational radiation and the dynamics of objects in forced circular motion.

James Essig
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I am curious as to the formula for radiative power due to a single object in forced circular motion.

In particular, I am interested in the power of gravitational radiation for volumetric invariant mass densities for both the low density Newtonian limit and the high density general relativistic limit for the above scenario.

Additionally, I am interested in the power formulas for the above scenarios for which the object would undergo forced circular motion with a tangential velocity near the speed of light.
 
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I've seen some discussion and formulas for a pair of objects rotating around a common center. The problem with a single body in forced circular motion is that the motion doesn't describe a physical situation with a conserved momentum. This is a definite problem in the general non-linear theory, it might be solvable in the linearized approximation. Regardless, the information I have is for a pair of bodies, in which the dipole moment vanishes due to the conservation of momentum, and the only gravitational radiation is due to fairly high order derivative of the quadrupole moment.

See for instance https://en.wikipedia.org/wiki/Gravitational_wave, and perhaps http://www.tapir.caltech.edu/~teviet/Waves/gwave_details.html (I haven't read the later site closely).
 
Thanks for the info pervect. I am going to check out those two sites today.
 

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