Encounter between an extended hyperelastic body and a Schwarzschild black hole with quadrupole-order effects
arXiv:2511.08699 · doi:10.1103/rxtx-1btd
Abstract
We model the general relativistic interaction of a small hyperelastic sphere with a Schwarzschild black hole as it follows an initially marginally-bound orbit through a close encounter. While the interaction reveals effects that are encoded by the Mathisson-Papapetrou-Dixon (MPD) multipolar equations through quadrupole order, the calculation is made using an independent general relativistic finite element scheme that we described earlier (Phys.~Rev.~D 108(8):084020, October 2023). The finite element calculation is done in Schwarzschild coordinates, following a large and scalable number of mass elements in interaction with each other through elastic forces derived from a potential energy function and with the spacetime geometry. After the fact, we analyze the dynamics using a local Fermi coordinate system, computing (1) the deviation of the center of mass of the body relative to the initial marginally-bound orbit, (2) changes in orbital and spin angular momenta, and (3) the decrease in orbital energy and accompanying deposition of energy into internal elastic dynamics. The interaction leads to the capture of the small body into a highly eccentric orbit ( in a sample calculation).
v2: Added ancillary supplementary video; updated journal reference/DOI (accepted for publication in Phys. Rev. D)
References in corpus (9)
- Tidal Love numbers of neutron stars
- Evolution of small-mass-ratio binaries with a spinning secondary
- Self-Force Calculations with a Spinning Secondary
- Spinning test-body orbiting around a Kerr black hole: circular dynamics and gravitational-wave fluxes
- Elastic stars in general relativity: IV. Axial perturbations
- Extended-body motion in black hole spacetimes: What is possible?
- Extended bodies with spin induced quadrupoles on circular equatorial orbits in Kerr spacetime
- Extended body dynamics in general relativity: hyperelastic models
- Continuous body dynamics and the Mathisson-Papapetrou-Dixon equations