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@Nick3523
Created May 29, 2023 06:30
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N - Body
# coding: utf8
import os
import shutil
import random
import moviepy.video.io.ImageSequenceClip
from PIL import Image, ImageFile
import numpy as np
import matplotlib.pyplot as plt
ImageFile.LOAD_TRUNCATED_IMAGES = True
"""
Code original pris sur https://github.com/pmocz/nbody-python (Philip Mocz (2020) Princeton Univeristy)
J'ai repris et modifié ce dernier pour :
- Utiliser une version non véctorisé sur le calcul des accélérations : pour mettre mieux en évidence la seconde loi de Newton
- Retirer l'évolution de la force dans le système dans le temps (pas utile dans ma démarche)
- Créer des scénarios prédéfinies et aléatoires avec : la constante gravitationnelle G n'est plus fixée à 1, mais varie entre 1 et 5, de même pour la masse des corps et de leur nombre : ils sont générés aléatoirement
- Et enfn, sauvegarder les images de la simulation pour enfaire ensuite des vidéos qui composent les scénarios.
"""
def getAcc( pos, mass, G, softening ):
"""
Calculate the acceleration on each particle due to Newton's Law
pos is an N x 3 matrix of positions
mass is an N x 1 vector of masses
G is Newton's Gravitational constant
softening is the softening length
a is N x 3 matrix of accelerations
"""
# positions r = [x,y,z] for all particles
x = pos[:,0:1]
y = pos[:,1:2]
z = pos[:,2:3]
# matrix that stores all pairwise particle separations: r_j - r_i
dx = x.T - x
dy = y.T - y
dz = z.T - z
# matrix that stores 1/r^3 for all particle pairwise particle separations
inv_r3 = (dx**2 + dy**2 + dz**2 + softening**2)
inv_r3[inv_r3>0] = inv_r3[inv_r3>0]**(-1.5)
ax = G * (dx * inv_r3) @ mass
ay = G * (dy * inv_r3) @ mass
az = G * (dz * inv_r3) @ mass
# pack together the acceleration components
a = np.hstack((ax,ay,az))
return a
def main(repeat=1):
""" N-body simulation """
for simuNumber in range(repeat):
# Simulation parameters
N = random.randint(2, 20) # Number of particles
t = 0 # current time of the simulation
tEnd = 10.0 # time at which simulation ends
dt = 0.01 # timestep
softening = 0.1 # softening length
G = random.randint(1, 5) # Newton's Gravitational Constant
plotRealTime = True
# Generate Initial Conditions
np.random.seed(42)
#mass = 20.0*np.ones((N,1))/N #static and uniform mass
mass = np.random.randint(1, 20, size=(N,1)) #random and unequal mass
pos = np.random.randn(N,3)
vel = np.random.randn(N,3)
# calculate initial gravitational accelerations
acc = getAcc( pos, mass, G, softening )
Nt = 300 # number of steps
#Nt = int(np.ceil(tEnd/dt)) # number of timesteps
# particle orbits for plotting trails
pos_save = np.zeros((N,3,Nt+1))
pos_save[:,:,0] = pos
# prep figure
fig = plt.figure(figsize=(4,5), dpi=80)
grid = plt.GridSpec(3, 1, wspace=0.0, hspace=0.3)
ax1 = plt.subplot(grid[0:3,0])
image_files = []
os.makedirs('temp')
print("nbiter : ", Nt)
# Simulation Main Loop
for i in range(Nt):
print(i)
# (1/2) kick
vel += acc * dt/2.0
# drift
pos += vel * dt
# update accelerations
acc = getAcc( pos, mass, G, softening )
# (1/2) kick
vel += acc * dt/2.0
# update time
t += dt
# save energies, positions for plotting trail
pos_save[:,:,i+1] = pos
# plot in real time
if plotRealTime or (i == Nt-1):
plt.sca(ax1)
plt.cla()
xx = pos_save[:,0,max(i-50,0):i+1]
yy = pos_save[:,1,max(i-50,0):i+1]
plt.scatter(xx,yy,s=1,color=[.7,.7,1])
plt.scatter(pos[:,0],pos[:,1],s=10,color='blue')
ax1.set(xlim=(-2, 2), ylim=(-2, 2))
ax1.set_aspect('equal', 'box')
imgpath = 'temp/nbody' + str(i) + '.png'
plt.savefig(imgpath, dpi=240)
image_files.append(imgpath)
plt.xlabel('time')
plt.ylabel('energy')
clip = moviepy.video.io.ImageSequenceClip.ImageSequenceClip(image_files, fps=30)
clip.write_videofile('videos/simulation_' + str(N) + '_gravity_' + str(G) + 'particles_' + str(simuNumber) + '.mp4')
shutil.rmtree('temp/') #delet all previous images, run again simulation
return 0
if __name__== "__main__":
main(100)
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