Orbital decay timescale 2026-10-25
An instantaneous orbital decay timescale is positive even when the orbital period decreases. For a constant-mass circular binary with and , . Integrating to formal zero separation instead gives . A local logarithmic decay time is not generally the remaining lifetime.
For two black holes of equal mass, and . The prescribed instantaneous orbital decay timescale gives
The integrated ten-billion-year criterion gives h. These large initial periods compared with a neutron-star pair reflect the stronger radiation reaction of the more massive system.
For the mixed pair, and . The prescribed instantaneous orbital decay timescale gives
The integrated ten-billion-year merger criterion instead gives h. Both are pre-disruption circular-orbit estimates; the final contact/capture process differs from that for two neutron stars.
The binary of neutron stars has and . Inserting these into the circular orbital decay timescale gives
Using the integrated ten-billion-year merger criterion instead would give h.
Use constant component masses and a circular Keplerian orbit. Then gives , while gives . Dividing the supplied loss law by therefore yields
The positive instantaneous orbital decay timescale is , since . For yr, the requested prescription gives
It is important to distinguish this prescription from the integrated gravitational-wave inspiral time. Integrating gives
Finite contact radii supply a small lower-limit correction when the initial separation is much larger than the compact objects. Thus the periods below satisfy the printed instantaneous-timescale criterion and have a formal merger time Gyr. If instead the requirement is literally Gyr, every period limit is larger by . Eccentric systems require a different decay calculation.