# What happens to the angular momentum of two merging black holes?

Let's suppose that two black holes of roughly equal mass in a binary system forming from say a large mass stellar binary system are in orbits around their center of mass. Further suppose that we are looking at their equations of motion well in advance of their merger. As a very crude approximation, I am using the Schwartzchild metric even though I know that this not a spherically symmetric system. The effective potential in this metric would be of the form:

$$V_{eff}=\frac{\mu c^2}{2}[-\frac{r_s}{r}+\frac{a^2}{r^2}-\frac{r_s a^2}{r^3}]$$

Where $a=\frac{L}{mc}$, $r_s$ is the Schwartzchild radius, and $\mu$ is the reduced mass.

So as this system loses energy via gravitational waves, they would eventually reach a circular orbit with a radius $$r_{min}=\frac{a^2}{r_s}(1+\sqrt{1-\frac{3r_s^2}{a^2}})$$ which is a local minimum in this effective potential.

However, to lose more energy and merge, there is a centripetal barrier to overcome. The only way I see around this is for the system to lose orbital angular momentum to a point where $a=\sqrt{3}r_s$ when this barrier disappears.

I know this fairly crude and in reality this requires computer simulations using Einstein's field equations, but it seems to me that for black holes to merge they would need to lose orbital angular momentum as well as energy.

1. Does the system transfer orbital angular momentum to the spin angular momentum of the black holes basically spinning them up as they approach one another? I am assuming that overall angular momentum still has to be conserved in the center of mass frame. What would be the mechanism for this transfer? Would this involve an ergosphere around each black hole?

2. Can one infer the spins of the merging black holes from the gravitational wave signal detected here on Earth?