How negative feedback and the ambient environment limit the influence of recombination in common envelope evolution

Author:

Chamandy Luke12ORCID,Carroll-Nellenback Jonathan23,Blackman Eric G2ORCID,Frank Adam2,Tu Yisheng24,Liu Baowei23,Zou Yangyuxin2ORCID,Nordhaus Jason56

Affiliation:

1. National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute , Bhubaneswar 752050, Odisha , India

2. Department of Physics and Astronomy, University of Rochester , Rochester NY 14627 , USA

3. Center for Integrated Research Computing, University of Rochester , Rochester NY 14627 , USA

4. Department of Astronomy, University of Virginia , Charlottesville, VA 22904 , USA

5. Center for Computational Relativity and Gravitation, Rochester Institute of Technology , Rochester, NY 14623 , USA

6. National Technical Institute for the Deaf, Rochester Institute of Technology , Rochester, NY 14623 , USA

Abstract

ABSTRACT We perform 3D hydrodynamical simulations to study recombination and ionization during the common envelope (CE) phase of binary evolution, and develop techniques to track the ionic transitions in time and space. We simulate the interaction of a $2\, \mathrm{M_\odot }$ red giant branch primary and a $1\, \mathrm{M_\odot }$ companion modelled as a particle. We compare a run employing a tabulated equation of state (EOS) that accounts for ionization and recombination, with a run employing an ideal gas EOS. During the first half of the simulations, ∼15 per cent more mass is unbound in the tabulated EOS run due to the release of recombination energy, but by simulation end the difference has become negligible. We explain this as being a consequence of (i) the tabulated EOS run experiences a shallower inspiral and hence smaller orbital energy release at late times because recombination energy release expands the envelope and reduces drag, and (ii) collision and mixing between expanding envelope gas, ejecta and circumstellar ambient gas assists in unbinding the envelope, but does so less efficiently in the tabulated EOS run where some of the energy transferred to bound envelope gas is used for ionization. The rate of mass unbinding is approximately constant in the last half of the simulations and the orbital separation steadily decreases at late times. A simple linear extrapolation predicts a CE phase duration of ${\sim}2\, {\rm yr}$, after which the envelope would be unbound.

Funder

National Science Foundation

Department of Energy

National Aeronautics and Space Administration

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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