[Mesa-users] other_torque question
Alexander Heger
alexander.heger at monash.edu
Wed Mar 10 06:07:10 UTC 2021
Dear Arend Jan,
whereas I don't know the internals of MESA, it seems your star is
rapidly expanding from the pattern in the last figure).
Is there convection?
You have a Kippenhahn Diagram?
After you remove j, if there is an instability, it may just be
replenished; if the outer layers are convective, j would be replenished
swiftly.
maybe useful to plot integrated total j as a function of time to see
where j goes or comes from, as in 2000 paper.
If the star expands and keeps the outer layers in co-rotation due to
convection, and you couple with layers deep enough, you get a 'rotator'
effect.
-Alexander
On Tue, 9 Mar 2021 at 05:16, AJ Poelarends <aj.poelarends at wheaton.edu
<mailto:aj.poelarends at wheaton.edu>> wrote:
Hello everyone,____
__ __
My two research students are experimenting with a very simple toy
model to see whether torques in an accretor can keep the angular
momentum of that accretor at (or below) critical rotation (such as
in an accretion disk boundary layer).____
In this simple model, we use the other_torque routine, and “shave
off” any angular momentum that is above the critical angular
momentum, by defining ____
__ __
omega_cr = sqrt(gamma_factor*cgrav*mmid/rmid**3)____
j_cr = s% i_rot(k) * omega_cr____
j_extra= max(s% j_rot(k)-j_cr,0.0d0)____
__ __
if (s% j_rot(k) > j_cr) then ____
s% extra_jdot(k) = -j_extra/s% dt ____
end if____
__ __
We’re aware that we don’t conserve angular momentum, and that you
can’t really “shave off” excess angular momentum, but it’s a first
iteration that we hope to improve in the future by redistributing
the angular momentum. However, for whatever reason, this simple
model does not work, and the accretor keeps spinning up above
critical rotation, and we’re not really sure why that is. Does
anyone have any insight in what we might be doing wrong?____
__ __
A couple of observations that I can’t explain:____
* surf_avg_omega_div_omega_crit (first figure) rises higher than
omega_div_omega_crit. I would have expected them to be close, or
omega_div_omega_crit higher than surf_avg_omega_div_omega_crit
as the latter one is averaged over several surface cells.____
* The second figure plots j_rot, j_crit and extra_jdot. extra_jdot
is calculated as j_rot-j_crit (in run_star_extras), but it does
not have the same magnitude as the gap between j_rot and j_crit,
as plotted from the profiles data.____
* The third graph shows the time evolution of
omega_div_omega_crit, and it seems that there is no effect
extra_jdot at all once the outer layers of the star become
super-critical.____
__ __
I’ve attached our inlists and run_star_extras.f files and some plots
showing the evolution of the star. We use mesa-r12778.____
Any help would be appreciated. Thanks!____
__ __
__ __
Vnqx6PzwAAAABJRU5ErkJggg==____
Evolution of surf_avg_omega_div_omega_crit.____
__ __
____
Profiles of j_rot, j_crit and extra_jdot for model number 430.____
__ __
____
Evolution of the omega_div_omega_crit profile for model numbers 300
– 433.____
__ __
__ __
*Arend J. Poelarends, PhD____*
*Associate Professor of Physics and Astronomy, Wheaton College____*
__ __
(630) 752-5894 | www.wheaton.edu <http://www.wheaton.edu>____
501 College Ave | Wheaton, IL 60187
_______________________________________________
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