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