Source code for swiftest.tool
"""
Copyright 2024 - The Minton Group at Purdue University
This file is part of Swiftest.
Swiftest is free software: you can redistribute it and/or modify it under the terms of the GNU General Public License
as published by the Free Software Foundation, either version 3 of the License, or (at your option) any later version.
Swiftest is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty
of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details.
You should have received a copy of the GNU General Public License along with Swiftest.
If not, see: https://www.gnu.org/licenses.
"""
import numpy as np
[docs]
def wrap_angle(angle):
"""
Converts angles to be between 0 and 360 degrees.
Parameters
----------
angle : float
Angle to be converted
Returns
-------
angle : float
Converted angle
"""
while np.any(angle >= 360.0 ):
angle[angle >= 360.0] -= 360.0
while np.any(angle < 0.0):
angle[angle < 0.0] += 360.0
return angle
[docs]
def follow_swift(ds, ifol=None, nskp=None):
"""
Emulates the Swift version of tool_follow.f
It will generate a file called follow.out containing 10 columns (angles are all in degrees)::
1 2 3 4 5 6 7 8 9 10
t,a,e,inc,capom,omega,capm,peri,apo,obar
Parameters
----------
ds : Xarray Dataset
Dataset containing orbital elements
ifol : int, optional
Particle number to follow. The default is None, in which case the user is prompted to enter a particle number.
nskp : int, optional
Print frequency. The default is None, in which case the user is prompted to enter a print frequency.
Returns
-------
fol : Xarray Dataset
Dataset containing only the followed body with angles converted to degrees
"""
fol = None
if ifol is None:
intxt = input(' Input the particle number to follow \n')
ifol = int(intxt)
print(f"Following particle {ifol}")
if ifol < 0: # Negative numbers are planets
fol = ds.where(np.invert(np.isnan(ds['Gmass'])), drop=True)
fol = fol.where(np.invert(np.isnan(fol['a'])), drop=True) # Remove times where this body doesn't exist (but this also gets rid of the central body)
fol = fol.isel(id = -ifol - 2) # Take 1 off for 0-indexed arrays in Python, and take 1 more off because the central body is gone
elif ifol > 0: # Positive numbers are test particles
fol = ds.where(np.isnan(ds['Gmass']), drop=True).drop_vars(['Gmass', 'radius'],errors="ignore")
fol = fol.where(np.invert(np.isnan(fol['a'])), drop=True)
fol = fol.isel(id = ifol - 1) # Take 1 off for 0-indexed arrays in Python
if nskp is None:
intxt = input('Input the print frequency\n')
nskp = int(intxt)
fol['obar'] = fol['capom'] + fol['omega']
fol['obar'] = fol['obar'].fillna(0)
fol['obar'] = wrap_angle(fol['obar'])
fol['peri'] = fol['a'] * (1.0 - fol['e'])
fol['apo'] = fol['a'] * (1.0 + fol['e'])
tslice = slice(None, None, nskp)
try:
with open('follow.out', 'w') as f:
print('# 1 2 3 4 5 6 7 8 9 10', file=f)
print('# t,a,e,inc,capom,omega,capm,peri,apo,obar', file=f)
for t in fol.isel(time=tslice).time:
a = fol['a'].sel(time=t).values
e = fol['e'].sel(time=t).values
inc = fol['inc'].sel(time=t).values
capom = fol['capom'].sel(time=t).values
omega = fol['omega'].sel(time=t).values
capm = fol['capm'].sel(time=t).values
peri = fol['peri'].sel(time=t).values
apo = fol['apo'].sel(time=t).values
obar = fol['obar'].sel(time=t).values
print(f"{t.values:15.7e} {a:22.16f} {e:22.16f} {inc:22.16f} {capom:22.16f} {omega:22.16f} {capm:22.16f} {peri:22.16f} {apo:22.16f} {obar:22.16f}", file=f)
except IOError:
print(f"Error writing to follow.out")
return fol