Hi Maria,

On Tuesday 2016-06-07 10:02, Hamilton, Maria wrote:

Date: Tue, 7 Jun 2016 10:02:36
From: "Hamilton, Maria" <[email protected]>
To: Peter Diener <[email protected]>, Frank Loeffler <[email protected]>
Cc: Einstein Toolkit Users <[email protected]>
Subject: Re: [Users] Resolving two BH

Hello,

Does this paper come with access to a par file that will show how to set the dynamic shift?

No it doesn't. That paper was based on the Jena groups BAM code and these features have not yet been implemented in McLachlan.

I need some help as well in setting up a run with two unequal mass black holes, for an undergraduate visualization project. My understanding is that the initial conditions are set with the parameters given in the TwoPunctures thorn. For example, if I want the first black hole to be equal with the mass of the sun, and the second, 10 times the mass of the sun, I do something like this?

TwoPunctures::par_m_plus                = 1.5
TwoPunctures::par_m_minus            = 15

The code uses units so G=c=1 so you can get mass you want. But yes, this will give you a mass ratio of 10. Note however, that if you want this to be the physical masses, you have to set

TwoPunctures::give_bare_mass = no

as well. Otherwise these will be the bare mass parameters given as input to the elliptical solve, and the actual physical masses after the solve might be a little bit different. One comment: I usually preferred to have the total mass be 1.0 in order to make grid setup as well as analysis simpler between runs with different mass ratio. So I would use

TwoPunctures::par_m_plus                = 0.09090909090909
TwoPunctures::par_m_minus            = 0.9090909090909

But That is a matter of taste of course.

The last thing I need to set is the velocity for each hole, If I want each of them to move at 1/3 c tangential velocity? I’m assuming I need to set:

TwoPunctures::par_P_plus [1] = +0.45
TwoPunctures::par_P_minus[1] = -4.5

You most likely want to do the simulation in the rest frame, where the
total momentum is 0. Otherwise your black hole system will drift away from the system. So the larger black hole will move 10 times slower than the small black hole. How big a velocity you want depends on exactly what kind of system you want to evolve. Do you want a hyperbolic flyby,
an elliptical orbit or a quasi-circular orbit?

Is this correct? And one more important thing: if I want the distance between them to be for example 150, how do I set this? I see a parameter par_b which gives the x coordinate of the m+ puncture, but I’m not clear if this is what I need to set, and how.

Yes, par_b gives the x-coordinate of the m+ puncture. By default the m- puncture will then be at -par_b (on the x-axis). So par_b is 1/2 the coordinate separation of the punctures. There is in addition a parameter center_offset that allow you to add an offset to the initial position. Again the choice of the separation and of the momenta goes hand in hand to determine what kind of orbit you'll get.

All the other parameters I am assuming are to be kept the way they are. In Rahul’s parameter file I do not see the PunctureTracker thorn activated. I do want to know the position of the back holes on the grid, and the distance between them at each step of the evolution. Do I need to activate PunctureTracker? What output do I need for this?

As far as I remember you just need to activate PunctureTracker and then
set a few parameters to activate tracking as well as setting the initial
puncture positions consistently with the TwoPuncture parameters.

And as far as I remember PunctureTracker keeps track of the punctures in Cactus grid scalars and you'd just need to request output for those.

Thank you,
Maria

Cheers,

  Peter

On 6/7/16, 10:13 AM, "[email protected] on behalf of Peter Diener" 
<[email protected] on behalf of [email protected]> wrote:

Hi,

This issue is discussed for example in

http://arxiv.org/abs/1003.4681

where a non-constant damping in the gamma driver shift is presented to
handle unequal mass binaries. As far as I remember there may also be
later papers with further improvements to the method.

Cheers,

  Peter

On Tuesday 2016-06-07 01:00, Frank Loeffler wrote:

Date: Tue, 7 Jun 2016 01:00:59
From: Frank Loeffler <[email protected]>
To: rahul kashyap <[email protected]>
Cc: Einstein Toolkit Users <[email protected]>
Subject: Re: [Users] Resolving two BH

On Mon, Jun 06, 2016 at 06:50:04PM -0400, rahul kashyap wrote:
Thanks for the reply. My apologies that I'm not completely familiar many of
the physical and numerical issues while simulating bbh. I have experience
in AMR astrophysical simulations.

No need to apologize.

When I do the bbh simulation of ratio around 1, it evolves perfectly fine.
With higher mass ratio, the smaller BH just becomes bigger and blows up.
I'm assuming this as a problem of refinement.

It is not. It looks like what I described earlier: your gauge
conditions, in particular the shift condition, isn't well suited for the
small black hole. Grid points are "falling in", making it appear growing
on the computational grid. You may try to play with the values such that
the small black hole evolves fine (you can try that with a simulation of
only a small black hole of that size), but then you might find that the
large black hole "vanishes from the grid" because grid points there are
pushed out too much. If this is the case, you might need
position-dependent values.

Frank



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