Skip to content

Very simple integrator for geodesics in Schwarzschild spacetime

Notifications You must be signed in to change notification settings

stefanoschmidt1995/BH_geodesics

Folders and files

NameName
Last commit message
Last commit date

Latest commit

 

History

4 Commits
 
 
 
 
 
 
 
 

Repository files navigation

BH motion

This simple script computes the motion of a satellite (test particle) around a BH. The computation can be performed both in GR or within the Netwonian limit.

How it works

The geodesics around a non-spinning BH (Schwarzschild) are a simple matter: it's just about writing down the conservation of energy and integrating the trajectories. The wikipedia page will tell you a lot on this.

How to use it

The code works in python. You will need to be able to run python (better from a terminal) with numpy, scipy and matplotlib installed.

To compute the orbit, you need to write some options in a config_file.ini. Then you just type:

    python BH_geodesics.py config_file.ini

A standard ini file looks like:


[BBH]
L= 5.02
phi_0= 0.
r_0 = 50.9
r_dot_0 = 0.
GR = 1
t_max= 9e4

max_step = 1e3
relative_units = 1
compare = 0
show = 1
save_trajectories = 0

Everything is in units of mass (where G = c = 1) In the ini file, you need to set:

  • L : angular momentum (in units of M**2)
  • r_0 : initial distance (in units of M)
  • phi_0 : initial angle (dimension less)
  • r_dot_0 : initial radial velocity (dimensionless)
  • GR: a boolean variable to control whether the Newtonian potential or the GR potential shall be used
  • t_max : maximum integration time (in units of M)

There are also a bunch of optionals parameters:

  • max_step (default = 1e4): controls the maximum integration step: if the integration doesn't converge, it may be a good idea to decrase it
  • relatives_units (default = 0): if True, r_dot_0 will be in units of sqrt(2*V(r,L)). This makes the dynamics more redable:
    • if |r_dot_0|>1 there are unbound orbits (hyperbolic)
    • if |r_dot_0|<1 we have a bound system (ellyptic)
  • compare (default = 0): if set to True, both GR and newtonian solutions will be computed and plotted together
  • show(default = 1): if True, it will plot show some plots
  • save_trajectories (default = 0): if True, it will save the trajectories to a jpeg file

If you want to display a quick help message, just type python BH_geodesics.py --help.

You can also set several configurations in the same file. Make sure each sets of configurations starts with [SET_NAME].

Examples

In folder plots, you can find an ini file with some examples. Feel free to play with them and explore the different possibilities.

Setting a zero initial velocity and negative energy, you will find strongly precessing orbits: the trajectory will look very nice.

If we set a non zero outward radial velocity (still keeping negative total energy) we will obtain strongly precessing, strongly eccentric orbits.

We can also set a positive total energy to obtain an hyperbolic trajectory. Starting far away from the BH and setting a large angular momentum, the path of the object will be slightly deviated.

If we start closer to the black hole, the gravitational deviation effect will be much much higher.

Note that in every case, the effect of Newtonian physics and those of GR are very different! This is only because a 1/r**3 term in the potential: cool, isn't it?

Of course, GR is not always important. If we take the case of the earth orbiting around the sun, the Newtonian physics works just fine:

Author

This was part of the tutorial for a GR course at Utrecht Univerisity. If you want more information, please feel free to send me an email: stefanoschmidt1995@gmail.com

About

Very simple integrator for geodesics in Schwarzschild spacetime

Topics

Resources

Stars

Watchers

Forks

Languages