Astron. Astrophys. 352, L87-L90 (1999)
2. Runaway velocities from symmetric SNe
Consider a circular pre-SN orbit consisting of a helium star with
mass (the progenitor of the black
hole) and a companion star with mass m. Assume that the helium
star explodes in a symmetric SN during which an amount of mass,
is ejected instantaneously and
decouples gravitationally from the system. If
the binary will remain bound. The
post-SN eccentricity, period and orbital separation are given by
Bhattacharya & van den Heuvel Bhattacharya and van den
Heuvel (1991)
![[EQUATION]](img15.gif)
![[EQUATION]](img16.gif)
where we define
![[EQUATION]](img17.gif)
and subscripts i denote the pre-SN system. Since the
observed black hole binaries all have short orbital periods
( days) tidal forces act to
re-circularize the post-SN orbit. The parameters of the
re-circularized orbit are given by
![[EQUATION]](img19.gif)
And similarly . Here we have
ignored the effects of the impact of the ejected shell on the
companion star and assume there is no mass loss or transfer during the
re-circularization phase. From conservation of momentum one finds an
expression for the resulting runaway velocity (recoil) of the system
![[EQUATION]](img21.gif)
where is the pre-SN orbital
velocity of the exploding helium star in a centre-of-mass reference
frame. Together with Keplers third law we find
![[EQUATION]](img23.gif)
For convenience this equation can be expressed as
![[EQUATION]](img24.gif)
If we know the masses of the stellar components and the orbital
period after the re-circularization
( ) we can calculate
from the observed runaway velocity,
. However, we observe
mass-transferring binaries which might have evolved due to loss of
angular momentum by gravitational radiation or magnetic braking before
the mass transfer started and/or might have transferred already a
significant amount of mass from the donor to the black hole. Before
applying Eq. (7) to the observed systems we have to correct for these
effects.
Also, one has to check whether the binary before the SN would be
detached, i.e. that both stars do not fill their Roche lobes at the
moment the SN explodes.
© European Southern Observatory (ESO) 1999
Online publication: December 2, 1999
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