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Emergence of alignment in a system of active rod-shaped particles
We consider a system of rod-shaped particles defined by their positions \(x_i\) and active directions of motion \(n_i\). Each \(n_i\) is defined at each time step as the maximal eigenvector associated to the PCA of the Laguerre cell (with the correct sign to avoid flipping). The collisions between particles thus lead to a local re-orientation process and eventually to the emergence of a globally aligned state.
# sphinx_gallery_thumbnail_path = '_static/RodShape_t3000.png'
import os
import sys
sys.path.append("..")
import pickle
import math
import torch
import numpy as np
from matplotlib import colors
from matplotlib.colors import ListedColormap
from iceshot import cells
from iceshot import costs
from iceshot import OT
from iceshot.OT import OT_solver
from iceshot import plot_cells
from iceshot import sample
from iceshot import utils
use_cuda = torch.cuda.is_available()
if use_cuda:
torch.set_default_tensor_type("torch.cuda.FloatTensor")
device = "cuda"
# ot_algo = OT.sinkhorn_zerolast
ot_algo = OT.LBFGSB
simu_name = "simu_RodShape"
os.mkdir(simu_name)
os.mkdir(simu_name+"/frames")
os.mkdir(simu_name+"/data")
N = 300
M = 512
seeds = torch.rand((N,2))
source = sample.sample_grid(M)
vol_x = 0.65*torch.ones(N)/N
ar = 3.0
simu = cells.Cells(
seeds=seeds,source=source,
vol_x=vol_x,extra_space="void",
ar=ar,bc="periodic"
)
p = 3.5
cost_params = {
"p" : p,
"scaling" : "volume",
"b" : math.sqrt(simu.volumes[0].item()/(math.pi + 4*(ar-1))),
"C" : 1.0
}
solver = OT_solver(
n_sinkhorn=300,n_sinkhorn_last=3000,n_lloyds=20,s0=2.0,
cost_function=costs.spherocylinders_2_cost,cost_params=cost_params
)
T = 30.0
dt = 0.002
plot_every = 4
t = 0.0
t_iter = 0
t_plot = 0
v0 = 0.3
tau = torch.ones(N)/simu.R_mean
tau *= 0.14
# tau = torch.ones(N)
# tau *= 10.0
cap = None
cmap = utils.cmap_from_list(N,0,0,color_names=["tab:blue","tab:blue","tab:blue"])
#======================= INITIALISE ========================#
solver.solve(simu,
sinkhorn_algo=ot_algo,cap=cap,
tau=1.0,
to_bary=True,
show_progress=False,weight=1.0)
simu_plot = plot_cells.CellPlot(simu,figsize=8,cmap=cmap,
plot_pixels=True,plot_scat=True,plot_quiv=False,plot_boundary=True,
scat_size=15,scat_color='k',
r=None,K=5,boundary_color='k',
plot_type="imshow",void_color='w')
simu_plot.fig.savefig(simu_name + "/frames/" + f"t_{t_plot}.png")
with open(simu_name + "/data/" + f"data_{t_plot}.pkl",'wb') as file:
pickle.dump(simu,file)
t += dt
t_iter += 1
t_plot += 1
solver.n_lloyds = 1
solver.cost_params["p"] = p
with open(simu_name + f"/params.pkl",'wb') as file:
pickle.dump(solver,file)
#=========================== RUN ===========================#
while t<T:
print("--------------------------",flush=True)
print(f"t={t}",flush=True)
print("--------------------------",flush=True)
plotting_time = t_iter%plot_every==0
if plotting_time:
print("I plot.",flush=True)
solver.n_sinkhorn_last = 3000
solver.n_sinkhorn = 3000
solver.s0 = 1.0
else:
print("I do not plot.",flush=True)
solver.n_sinkhorn_last = 300
solver.n_sinkhorn = 300
solver.s0 = simu.R_mean
F_inc = solver.lloyd_step(simu,
sinkhorn_algo=ot_algo,cap=cap,
tau=tau,
to_bary=False,
show_progress=False,
default_init=False)
simu.x += v0*simu.axis*dt + F_inc*dt
cov = simu.covariance_matrix()
cov /= torch.sqrt(torch.det(cov).reshape((simu.N_cells,1,1)))
L,Q = torch.linalg.eigh(cov)
axis = Q[:,:,-1]
axis = (axis * simu.axis).sum(1).sign().reshape((simu.N_cells,1)) * axis
simu.axis = axis
simu.orientation = simu.orientation_from_axis()
simu.x = torch.remainder(simu.x,1)
print(torch.max(torch.norm(F_inc,dim=1)))
if plotting_time:
simu_plot.update_plot(simu)
simu_plot.fig.savefig(simu_name + "/frames/" + f"t_{t_plot}.png")
with open(simu_name + "/data/" + f"data_{t_plot}.pkl",'wb') as file:
pickle.dump(simu,file)
t_plot += 1
t += dt
t_iter += 1
utils.make_video(simu_name=simu_name,video_name=simu_name)