def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print('usage:\npython condition.py model_name [N0, N1, R/dr]')
sys.exit(1)
model_name, keys, model_dir, graph_dir, time_gaps_str, N0, N1, Nfrm, E, P, Tmp, Tmp_av, t, stabTind, params = my.std_start(args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
if(len(args) < 4):
path = os.path.join(my.RAW_DATA_PATH, model_name)
all_filenames = [name_of_smth for name_of_smth in os.listdir(path) if os.path.isfile(os.path.join(path, name_of_smth))]
Nslice = max([int(_x) for _x in re.findall(r'condition_(\d+).dat', ' '.join(all_filenames))])
else:
Nslice = int(args[3])
input_filename = 'condition_' + str(Nslice) + '.dat'
data = my.load_file(model_name, input_filename)
x_dr = data[0];
if(len(x_dr) != Nslice):
print('wrong condition file\n' + input_filename + '\n' + 'Nslice = ' + str(Nslice) + '; len(x_dr) = ' + str(len(x_dr)))
exit(1)
data = data[1:]
if(N1 > len(data)):
print('wrong condition file\n' + input_filename + '\n' + 'max_frame_n = ' + str(len(data)-1))
exit(1)
draw_on_screen = my.find_key(keys, 'keep')
if(not draw_on_screen):
plt.switch_backend('Agg')
y_gFnc = data[0];
for i in range(N0,N1):
for j in range(Nslice):
y_gFnc[j] += data[i,j]
if(draw_on_screen):
print('condition progress: ' + str((i+1-N0)/Nfrm*100) + '% \r', end='')
y_gFnc = [_x/(N1-N0) for _x in y_gFnc]
fig_c = -1
fig = []
time_gaps_str += ('_Nslice_' + str(Nslice))
y0 = [math.exp(-my.phi_r(_x)) for _x in x_dr]
path = os.path.join(graph_dir, 'g(t)_' + time_gaps_str + '.png')
fig_c, fig = my.plot_error(fig_c, fig, x_dr, y_gFnc, y0=1, y_th=y0, x_lbl='r', y_lbl='n/n0', pic_path=path, filter_rng=round(params['R']/Nslice/0.05 + 0.5), draw_linfit='n', show_key=draw_on_screen)
if(draw_on_screen):
input()
def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print(
'usage: ./full_proc.py model_name [keys, N0, N1, ...]'
)
sys.exit(1)
model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params = my.std_start(
args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
extra_args_str = ''
for i in range(1, len(args)):
extra_args_str += (args[i] + ' ')
if (my.find_key(keys, 'energy')):
my.run_it('./E.py ' + model_name + ' ' + extra_args_str)
if (my.find_key(keys, 'maxwell')):
if (extra_args_str):
command_to_run = './maxwell.py ' + model_name + ' 100 ' + extra_args_str
else:
command_to_run = './maxwell.py ' + model_name + ' 100 ' + str(
stabTind)
my.run_it(command_to_run)
if (my.find_key(keys, 'diff') or my.find_key(keys, 'diffusion')):
my.run_it('./diffusion.py ' + model_name + ' ' + extra_args_str)
if (my.find_key(keys, 'cond') or my.find_key(keys, 'condition')):
if (extra_args_str):
command_to_run = './condition.py ' + model_name + ' ' + extra_args_str
else:
command_to_run = './condition.py ' + model_name + ' ' + str(
stabTind)
my.run_it(command_to_run)
def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print('usage:\npython E.py model_name [keys N0 N1]')
sys.exit(1)
model_name, keys, model_dir, graph_dir, time_gaps_str, N0, N1, Nfrm, E, P, Tmp, Tmp_av, t, stabTind, params = my.std_start(
args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
#for i in range(N0, N1):
# for j in range(4):
# E[i,j] /= params['Ntot']
E /= params['Ntot']
fig_c = -1
fig = []
draw_on_screen = my.find_key(keys, 'keep')
if (not draw_on_screen):
plt.switch_backend('Agg')
fig_c += 1
# 0
fig.append(plt.figure(fig_c))
plt.plot(t[N0:N1], E[N0:N1, 2], '-', label='Etot')
plt.plot(t[N0:N1], E[N0:N1, 0], '-', label='Ek')
plt.plot(t[N0:N1], E[N0:N1, 1], '-', label='Ep')
plt.xlabel('time')
plt.ylabel('E')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102),
loc=3,
ncol=3,
mode="expand",
borderaxespad=0.)
if (draw_on_screen):
fig[fig_c].show()
path = os.path.join(graph_dir, 'Energy3_' + time_gaps_str + '.png')
fig[fig_c].savefig(path)
# 1
E0 = np.mean(E[N0:N1, 0]) + abs(np.mean(E[N0:N1, 1]))
path = os.path.join(graph_dir, 'dE_norm_' + time_gaps_str + '.png')
E_av = np.mean(E[N0:N1, 2])
#y = [(e_el - E[N0,2])/E0 for e_el in E[N0:N1,2]]
y = [(e_el / E_av - 1) for e_el in E[N0:N1, 2]]
fig_c, fig = my.plot_error(fig_c,
fig,
t[N0:N1],
y,
y0=0,
y_lbl='E/<E>-1',
tit='E/<E> - 1 | std = ' +
my.str_sgn_round(np.std(y), 3),
pic_path=path,
show_key=draw_on_screen)
# shadow error
E0 = np.mean(E[N0:N1, 0]) + abs(np.mean(E[N0:N1, 1]))
path = os.path.join(graph_dir, 'dH_norm_' + time_gaps_str + '.png')
H_av = np.mean(E[N0:N1, 3])
y = [(e_el / H_av - 1) for e_el in E[N0:N1, 3]]
#print(E[N0:N1, :])
fig_c, fig = my.plot_error(fig_c,
fig,
t[N0:N1],
y,
y0=0,
y_lbl='H/<H>-1',
tit='H/<H> - 1 | std = ' +
my.str_sgn_round(np.std(y), 3),
pic_path=path,
show_key=draw_on_screen)
# shadow
fig_c += 1
fig.append(plt.figure(fig_c))
plt.plot(t[N0:N1], E[N0:N1, 2], '-', label='Etot')
plt.plot(t[N0:N1], E[N0:N1, 3], '-', label='d2H')
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102),
loc=3,
ncol=2,
mode="expand",
borderaxespad=0.)
if (draw_on_screen):
fig[fig_c].show()
path = os.path.join(graph_dir, 'E_H_' + time_gaps_str + '.png')
fig[fig_c].savefig(path)
# shadow term
fig_c += 1
fig.append(plt.figure(fig_c))
plt.plot(t[N0:N1], E[N0:N1, 3] - E[N0:N1, 2], '-', label='$d^2 H$')
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102),
loc=3,
mode="expand",
borderaxespad=0.)
if (draw_on_screen):
fig[fig_c].show()
path = os.path.join(graph_dir, 'd2H_' + time_gaps_str + '.png')
fig[fig_c].savefig(path)
# Pressure
path = os.path.join(graph_dir, 'Pressure_' + time_gaps_str + '.png')
P_th = params['n'] * params['Tmp']
y = P[N0:N1]
fig_c, fig = my.plot_error(
fig_c,
fig,
t[N0:N1],
y,
y_th=[_x * P_th for _x in np.ones(len(y))],
y0=np.mean(P[N0:N1]),
y_lbl='P',
tit='P(time) | std_rel = ' +
my.str_sgn_round(np.std(P[N0:N1]) / np.mean(P[N0:N1]), 3),
pic_path=path,
show_key=draw_on_screen)
# 2
#path = os.path.join(graph_dir, 'Etot_' + time_gaps_str + '.png')
#y = [_x*params['Ntot'] for _x in E[N0:N1, 2]]
#fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=np.mean(y), y_lbl='Etot', tit='Etot | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 3
#path = os.path.join(graph_dir, 'dE_normSQRT(N)_' + time_gaps_str + '.png')
##y = [(e_el - E[N0,2])*mth.sqrt(params['Ntot']) for e_el in E[N0:N1,2]]
#y = [(e_el - E_av)*mth.sqrt(params['Ntot']) for e_el in E[N0:N1,2]]
#fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=0, y_lbl='(E - <E>)/sqrt(N)', tit='Esqrt | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 4
#path = os.path.join(graph_dir, 'dE_' + time_gaps_str + '.png')
##y = [(e_el - E[N0,2])*params['Ntot'] for e_el in E[N0:N1,2]]
#y = [(e_el - E_av)*params['Ntot'] for e_el in E[N0:N1,2]]
#fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=0, y_lbl='E - <E>', tit='E - <E> | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 5
path = os.path.join(graph_dir, 'Tmp_' + time_gaps_str + '.png')
y = Tmp
fig_c, fig = my.plot_error(fig_c,
fig,
t[N0:N1],
Tmp,
y0=Tmp_av,
y_lbl='Tmp',
tit='Tmp | std_rel = ' +
my.str_sgn_round(np.std(Tmp) / Tmp_av, 3),
pic_path=path,
show_key=draw_on_screen)
if (draw_on_screen):
input()
def main():
args = sys.argv[1:]
argc_min = 2
if len(args) < argc_min:
print(
'usage: ./maxwell.py model_name N_V_steps [keys, N0, N1]'
)
sys.exit(1)
model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params = my.std_start(
args, 0, 2, 3, 4)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
NV = int(args[1])
draw_on_screen = my.find_key(keys, 'keep')
if (not draw_on_screen):
plt.switch_backend('Agg')
if (len(args) < 4):
if (draw_on_screen):
print("N0 isn't set, N0 = ", stabTind, ' will be used')
N0 = stabTind
Nfrm = N1 - N0
Z_sum = math.pow(params['mu'] / 2 / np.pi / Tmp_av, 1.5)
k0 = 2 * np.pi * Z_sum
v_prob = math.sqrt(2 * Tmp_av / params['mu'])
v2_prob = Tmp_av / params['mu']
total_v2 = np.zeros(NV - 1)
total_v = np.zeros(NV - 1)
for n in range(N0, N1):
x, v, m = my.read_frame(model_name, n)
v2 = my.arrDot(v, v)
v_abs = my.arrFnc(v2, math.sqrt)
if (n == N0):
#v2max = max(v2)
#v2min = min(v2)
v2max = 3 * Tmp_av / params['mu'] * 4
v2min = 3 * Tmp_av / params['mu'] / 10
k_v2 = 1 / (params['Ntot'] * (v2max - v2min) / NV * Nfrm)
k_v = 1 / (params['Ntot'] *
(math.sqrt(v2max) - math.sqrt(v2min)) / NV * Nfrm)
v2steps = np.linspace(v2min, v2max, num=NV)
vsteps = np.linspace(math.sqrt(v2min), math.sqrt(v2max), num=NV)
x_v2 = [(v2steps[i] + v2steps[i + 1]) / 2 for i in range(NV - 1)]
x_v = [(vsteps[i] + vsteps[i + 1]) / 2 for i in range(NV - 1)]
y0_v2 = [
k0 * math.sqrt(_x) * math.exp(-params['mu'] * _x / 2 / Tmp_av)
for _x in x_v2
]
y0_v = [
2 * k0 * _x * _x *
math.exp(-params['mu'] * _x * _x / 2 / Tmp_av) for _x in x_v
]
#y0_ln = [-params['mu']*_x/2/Tmp_av for _x in x_v2]
y0_ln = []
for _x in x_v2:
_a = params['mu'] * _x / 2 / Tmp_av
#y0_ln.append(math.log(1-2*_a/3/params['Ntot']) - _a)
y0_ln.append(-_a)
peaks, bin_edges = np.histogram(v2, bins=v2steps)
for i in range(NV - 1):
total_v2[i] += peaks[i]
peaks, bin_edges = np.histogram(v_abs, bins=vsteps)
for i in range(NV - 1):
total_v[i] += peaks[i]
if (draw_on_screen):
print('maxwell progress: ' + str(
(n + 1 - N0) / (N1 - N0) * 100) + '% \r',
end='')
y_v2 = [total_v2[i] * k_v2 for i in range(NV - 1)]
y_v = [total_v[i] * k_v for i in range(NV - 1)]
y_ln = []
for i in range(NV - 1):
if (y_v2[i] > 0):
y_ln.append(math.log(y_v2[i] / k0 / math.sqrt(x_v2[i])))
else:
y_ln.append(0)
dy_v = [y_v[i] / y0_v[i] - 1 for i in range(len(x_v))]
dy_v2 = [y_v2[i] / y0_v2[i] - 1 for i in range(len(x_v2))]
dy_ln = [y_ln[i] / y0_ln[i] - 1 for i in range(len(x_v2))]
p_lnp = np.poly1d(np.polyfit(x_v2, y_ln, 1))
k_exp = -p_lnp.c[0]
k_th = params['mu'] / 2 / Tmp_av
#print('k_exp = ', k_exp)
#print('k_th = ', k_th)
s = 0
for i in range(NV - 1):
s += (p_lnp(x_v2[i]) - y_ln[i])**2
s /= (NV - 2)
if (draw_on_screen):
print('S = ', s)
fig_c = -1
figs = []
time_gaps_str += ('_NV_' + str(NV))
path = os.path.join(graph_dir, 'p(v)_' + time_gaps_str + '.png')
fig_c, figs = my.plot_error(fig_c,
figs,
x_v,
y_v,
y_th=y0_v,
x0=v_prob,
x_lbl='v',
y_lbl='p',
pic_path=path,
show_key=draw_on_screen)
path = os.path.join(graph_dir, 'p(v2)_' + time_gaps_str + '.png')
fig_c, figs = my.plot_error(fig_c,
figs,
x_v2,
y_v2,
y_th=y0_v2,
x0=v2_prob,
x_lbl='v^2',
y_lbl='p',
pic_path=path,
show_key=draw_on_screen)
path = os.path.join(graph_dir, 'ln_p(v2)_' + time_gaps_str + '.png')
#fig_c, figs = my.plot_error(fig_c, figs, x_v2, y_ln, y_th=y0_ln, x_lbl='v^2', y_lbl='ln(p/v^2)', tit='(ln(p/v^2))(v^2) | k_th = ' + my.str_sgn_round(k_th,3) + ', k_exp = ' + my.str_sgn_round(k_exp,3) + ' | std = ' + my.str_sgn_round(s,3), pic_path=path, show_key=draw_on_screen)
fig_c, figs = my.plot_error(fig_c,
figs,
x_v2,
y_ln,
y_th=y0_ln,
x_lbl='v^2',
y_lbl='ln(p/v^2)',
tit='k_th = ' + my.str_sgn_round(k_th, 3) +
', k_exp = ' + my.str_sgn_round(k_exp, 3) +
' | std = ' + my.str_sgn_round(s, 3) +
', p0 = ' + my.str_sgn_round(p_lnp.c[1], 3),
pic_path=path,
show_key=draw_on_screen)
path = os.path.join(graph_dir, 'd_p(v)_' + time_gaps_str + '.png')
fig_c, figs = my.plot_error(fig_c,
figs,
x_v,
dy_v,
x0=v_prob,
y0=0,
x_lbl='v',
y_lbl='p/p0-1',
pic_path=path,
show_key=draw_on_screen)
path = os.path.join(graph_dir, 'd_p(v2)_' + time_gaps_str + '.png')
fig_c, figs = my.plot_error(fig_c,
figs,
x_v2,
dy_v2,
x0=v2_prob,
y0=0,
x_lbl='v^2',
y_lbl='p/p0-1',
pic_path=path,
show_key=draw_on_screen)
path = os.path.join(graph_dir, 'd_ln_p(v2)_' + time_gaps_str + '.png')
fig_c, figs = my.plot_error(fig_c,
figs,
x_v2,
dy_ln,
y0=0,
x_lbl='v^2',
y_lbl='dln(p)',
pic_path=path,
show_key=draw_on_screen)
if (draw_on_screen):
input()
def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print('usage:\npython diffusion.py model_name [keys, N0, N1, Nprt]')
sys.exit(1)
# --------------------------------- std start ------------------------------------------
model_name, keys, model_dir, graph_dir, time_gaps_str, N0, N1, Nfrm, E, P, Tmp, Tmp_av, t, stabTind, params = my.std_start(args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
# --------------------------------- input handle ------------------------------------------
if(Nfrm < 10):
print('Too few grames (Nfrm < 10)')
return
if(len(args) < 5):
Nprt = params['Ntot']
else:
Nprt = int(args[4])
draw_on_screen = my.find_key(keys, 'keep')
pnrt_progress = (my.find_key(keys, 'percent') or my.find_key(keys, 'prcnt'))
if(not draw_on_screen):
plt.switch_backend('Agg')
make_pics = (my.find_key(keys, 'pics') or draw_on_screen)
# --------------------------------- theory prediction ------------------------------------------
n0 = params['n']
r_th0 = 1
lmd_th0 = 1/(n0 * math.pi * r_th0**2 * math.sqrt(2))
r_th1 = r_th0 * my.r_th1(Tmp_av, n0)
lmd_th1 = lmd_th0 * (r_th0/r_th1)**2
#r_th2 = pow(2, 1/6) * math.sqrt(1 + 2/(3*Tmp_av))
r_th2 = r_th0 * my.r_th2(Tmp_av)
lmd_th2 = lmd_th0 * (r_th0/r_th2)**2
k_th = 4*lmd_th1 * math.sqrt(2*Tmp_av / math.pi)
c_th = 1 / (6*Tmp_av)
# --------------------------------- experimant data ------------------------------------------
diff_file_path = os.path.join(model_dir, my.diff_filename)
if(os.path.isfile(diff_file_path) and (not my.find_key(keys, 'recomp'))):
data = np.loadtxt(diff_file_path)
#data = np.delete(data, (0), axis=0)
#data = np.delete(data, (0), axis=1)
r2 = cp.deepcopy(data[0])
l = len(r2);
x_cm = np.zeros((l, 3))
v_cm = np.zeros((l, 3))
for i in range(l):
for j in range(3):
x_cm[i][j] = data[j+1][i]
v_cm[i][j] = data[j+4][i]
data = None;
else:
r2 = []
dr = [0,0,0]
cubeSize = 2*params['R']
cubeSzEff = params['R']
x_cm = []
#r_cm = []
v_cm = []
for n in range(N0,N1):
x,v = my.read_frame(model_name, n)
m = np.ones(params['Ntot'])
if(n == N0):
# set start conditions
x0 = cp.deepcopy(x)
x_real = cp.deepcopy(x)
r2.append(0)
v_start_av = np.mean([my.length(_x) for _x in v])
else:
r2_sum = 0
for i in range(Nprt): # find <r^2> considering coords's shifts
for j in range(3):
dr[j] = x[i][j]-x0[i][j]
r2_sum += my.dot(dr,dr)
r2.append(r2_sum/Nprt)
x_cm.append(my.find_cm(x, m))
v_cm.append(my.find_cm(v,m))
if(pnrt_progress):
print('diffusion progress: ' + str((n + 1 - N0) / Nfrm * 100) + '% \r', end='')
xx = [_x[0] for _x in x_cm]
xy = [_x[1] for _x in x_cm]
xz = [_x[2] for _x in x_cm]
vx = [_x[0] for _x in v_cm]
vy = [_x[1] for _x in v_cm]
vz = [_x[2] for _x in v_cm]
np.savetxt(diff_file_path, (r2, xx, xy, xz, vx, vy, vz))
# --------------------------------- experimant analisys ------------------------------------------
# find proper tg
r1 = my.arrFnc(r2, math.sqrt)
big_time = 3
small_time = 0.5
approx_r2 = np.poly1d(np.polyfit(t[N0:N1], r2, 1))
k_exp = approx_r2.c[0]
tau = c_th*k_exp
c2 = int(tau*params['dumpDT'] * big_time)
if(c2 > Nfrm-10):
c2 = Nfrm-10
if(c2 < 10):
c2 = int(Nfrm/2)
approx_r2 = np.poly1d(np.polyfit(t[(N0+c2):N1], r2[c2:], 1))
k_exp = abs(approx_r2.c[0])
tau = c_th * k_exp
c2 = int(tau*params['dumpDT'] * big_time)
if(c2 > Nfrm - 5):
c2 = Nfrm - 5
if(c2 < 10):
c2 = int(Nfrm/2)
c1 = int(tau*params['dumpDT'] * small_time)
if(c1 < 3):
c1 = 3
# in case of strange emergencies
bad_k_exp = (k_exp < my.myeps)
if(bad_k_exp):
if(k_exp < 0):
k_exp = -k_exp
if(k_exp < my.myeps):
k_exp = my.myeps
xa0 = abs(approx_r2(0))
tau = xa0/k_exp
c_exp = xa0 / k_exp**2
B = (1 - r2[-2] / (k_exp * t[N1-1])) * math.sqrt(t[N1-1])
subdiff_c = int(round(B*B*params['dumpDT'] + 1.01))
x = my.arrFnc(t[(N0+c2):N1], math.log)
y = my.arrFnc(r2[c2:], math.log)
logEnd_approx = np.poly1d(np.polyfit(x, y, 1))
x = my.arrFnc(t[N0:c1], math.log)
y = my.arrFnc(r2[1:c1], math.log)
logBeg_approx = np.poly1d(np.polyfit(x, y, 1))
x = t[N0:c1]
y = my.arrFnc(r2[1:c1], math.sqrt)
approx_r1 = np.poly1d(np.polyfit(x, y, 1))
#lmd_1 = math.sqrt(3*math.pi*xa0)/4
lmd_1 = my.lmd_1(xa0)
#lmd_2 = k_exp/4 * math.sqrt(math.pi / (Tmp_av*2))
lmd_2 = my.lmd_2(k_exp, 1, Tmp_av)
D_Einst = lmd_2 * math.sqrt(8 * Tmp_av / math.pi) / 3
selfconsist = my.rel_err(lmd_1, lmd_2)
lmd_3 = my.lmd_3(logBeg_approx.c[0], logBeg_approx.c[1], logEnd_approx.c[0], logEnd_approx.c[1], 1, Tmp_av) # tau -> lmd
lmd_4 = my.lmd_4(logBeg_approx.c[0], logBeg_approx.c[1], logEnd_approx.c[0], logEnd_approx.c[1]) # straight lmd
if(make_pics):
fig_c = -1
figs = []
if(my.find_key(keys, 'r_cm')):
# -------------------------------- r_cm(t) -----------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
cm = []
std_cm = []
x = t[N0:N1]
t**s = ['x', 'y', 'z']
for _j in range(3):
cm.append([x_cm[_i][_j]-x_cm[0][_j] for _i in range(Nfrm)])
std_cm.append(np.std(cm[_j]))
plt.plot(x, cm[_j], '-', label = t**s[_j] + '; std = ' + str(my.str_sgn_round(std_cm[_j],3))) # experiment data
x = [t[N0], t[N1-1]]
plt.plot(x, [0,0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0,0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0,0))
plt.xlabel('t')
plt.ylabel('xyz_cm')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102), loc=3,
ncol=3, mode="expand", borderaxespad=0.)
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'xyz_cm(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
if(my.find_key(keys, 'r2')):
# -------------------------------- r2(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
#tau = 1
x = t[N0:N1]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, r2, '-', label="exp") # experiment data
x = t[N0:N1]
r2_th = [k_exp*tau*(_x/tau - 1 + math.exp(- _x/tau)) for _x in x]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, r2_th, '--', label="my_th") # my approximation
if(my.find_key(keys, 'subdiff')):
x = t[(N0 + subdiff_c):N1]
subdiff_app = [k_exp*_x*(1 - B/math.sqrt(_x)) for _x in x]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, subdiff_app, '-.', label="subdiff") # subdiff approximation
x = [t[N0], t[N1-1]]
y = [approx_r2(_x) for _x in x]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, y, '--', label="line asimp") # line approximation
plt.ticklabel_format(style='sci', axis='y', scilimits=(0,0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0,0))
plt.xlabel('t/tau')
plt.ylabel('<r^2>')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('r^2(t) | tau = ' + my.str_sgn_round(tau,3) + ' | B = ' + my.str_sgn_round(B,3))
plt.legend()
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r2(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- log(r2)(log(t)) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
x = t[N0:N1]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, r2, '-', label="exp") # experiment data
x = [_x/tau for _x in t[N0:N1]]
plt.plot(x, r2_th, '--', label="my_th") # my approximation
if(my.find_key(keys, 'subdiff')):
x = t[(N0 + subdiff_c):N1]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, subdiff_app, '--', label="subdiff") # subdiff approximation
x = [t[N0], t[N0+c2]]
y = [math.exp(logBeg_approx(math.log(_x))) for _x in x]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, y, '--', label="ballistic") # beginning approximation
x = [t[N0+c1], t[N1-1]]
y = [math.exp(logEnd_approx(math.log(_x))) for _x in x]
x_draw = [_x/tau for _x in x]
plt.plot(x_draw, y, '--', label="linear") # ending approximation
plt.xlabel('t/tau')
plt.ylabel('<r^2>')
plt.grid(True)
plt.xscale('log')
plt.yscale('log')
plt.title('log(r2) | k_begin = ' + str(my.str_sgn_round(logBeg_approx.c[0],3)) + '; k_end = ' + str(my.str_sgn_round(logEnd_approx.c[0],3)))
plt.legend()
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r2(t)_loglog_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r1, '-', label="exp") # experiment data
x = t[N0:N1]
y = my.arrFnc(r2_th, math.sqrt)
plt.plot(x, y, '--', label="my_th") # my approximation
if(my.find_key(keys, 'subdiff')):
x = t[(N0 + subdiff_c):N1]
y = my.arrFnc(subdiff_app, math.sqrt)
plt.plot(x, y, '--', label="subdiff") # sudiff approximation
x = [t[N0], t[c2]]
y = [approx_r1(_x) for _x in x]
plt.plot(x, y, '--', label="ballistic") # beginning approximation
plt.xlabel('t')
plt.ylabel('sqrt(<r^2>)')
plt.grid(True)
#plt.title('sqrt(r2) | l_th = ' + str(my.str_sgn_round(lmd_th1,3)) + '; l_3 = ' + str(my.str_sgn_round(lmd_3,3)) + '; l_2 = ' + str(my.str_sgn_round(lmd_2,3)))
plt.title('sqrt(<r^2>)')
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r1(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
if(my.find_key(keys, 'r2_err')):
# -------------------------------- r2_err(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
x = t[N0:N1]
y = [r2[_i] - r2_th[_i] for _i in range(len(r2_th))]
plt.plot(x, y, '-') # my approximation
if(my.find_key(keys, 'subdiff')):
x = t[(N0 + subdiff_c):N1]
y = [r2[_i + subdiff_c] - subdiff_app[_i] for _i in range(0, N1 - N0 - subdiff_c)]
plt.plot(x, y, '--') # subdiff approximation
plt.plot([t[N0+1], t[N1-1]], [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0,0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0,0))
plt.xlabel('t')
plt.ylabel('<r^2> - <r^2>_th')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('<r^2> error')
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r2_err(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r2_err_rel(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
tmp = int(round(tau*5*params['dumpDT']))
x = t[(N0 + subdiff_c + tmp):N1]
y = [my.rel_err(r2[_i], r2_th[_i]) for _i in range(tmp, N1 - N0 - subdiff_c)]
plt.plot(x, y, '-') # my approximation
if(my.find_key(keys, 'subdiff')):
x = t[(N0 + subdiff_c + tmp):N1]
y = [my.rel_err(r2[_i + subdiff_c],subdiff_app[_i]) for _i in range(tmp, N1 - N0 - subdiff_c)]
plt.plot(x, y, '-.') # subdiff approximation
plt.plot([t[N0+1], t[N1-1]], [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0,0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0,0))
plt.xlabel('t')
plt.ylabel('err')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('|<r^2> / <r^2>_th - 1|')
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r2_err_rel(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
if(my.find_key(keys, 'v_cm')):
# -------------------------------- v_cm(t) -----------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
x = t[N0:N1]
dv_cm = []
std_dvcm = []
t**s = ['vx', 'vy', 'vz']
for _j in range(3):
v_av = np.mean(v_cm[:][_j])
dv_cm.append([v_cm[_i][_j] - v_av for _i in range(Nfrm)])
std_dvcm.append(np.std(dv_cm[_j]))
plt.plot(x, dv_cm[_j], '-', label = t**s[_j] + '; std = ' + str(my.str_sgn_round(std_dvcm[_j],3))) # experiment data
x = [t[N0], t[N1-1]]
plt.plot(x, [0,0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0,0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0,0))
plt.xlabel('t')
plt.ylabel('v_cm')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102), loc=3,
ncol=3, mode="expand", borderaxespad=0.)
if(draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'v_cm(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
if(my.find_key(keys, 'human')):
print('n = ', n0, '; T = ', Tmp_av)
print('lmd_0 = ', lmd_th0, '; lmd_T<1 = ', lmd_th1, '; lmd_T>1 = ', lmd_th2)
print('lmd_a = ', lmd_1, '; lmd_tg = ', lmd_2, '; lmd_exp_intercept = ', lmd_3, '; lmd_tau_intercept = ', lmd_4)
print('inconsistency = ', selfconsist)
else:
print(n0, Tmp_av, lmd_th0, lmd_th1, lmd_th2, lmd_1, lmd_2, lmd_3, lmd_4)
#print('D_Einst = ' + str(D_Einst))
if(draw_on_screen):
#print(c_th, c_exp, my.rel_err(c_th, c_exp))
input()
def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print('usage: ./diffusion.py model_name [keys, N0, N1, Nprt]')
sys.exit(1)
# --------------------------------- std start ------------------------------------------
model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params = my.std_start(
args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
# --------------------------------- input handle ------------------------------------------
if (Nfrm < 10):
print('Too few grames (Nfrm < 10)')
return
if (len(args) < 4):
Nprt = params['Ntot']
else:
Nprt = int(args[3])
draw_on_screen = my.find_key(keys, 'keep')
pnrt_progress = (my.find_key(keys, 'percent')
or my.find_key(keys, 'prcnt'))
if (not draw_on_screen):
plt.switch_backend('Agg')
make_pics = (my.find_key(keys, 'pics') or draw_on_screen)
# --------------------------------- theory prediction ------------------------------------------
n0 = params['Ntot'] / math.pow(2 * params['R'], 3)
r_th0 = 1
lmd_th0 = 1 / (n0 * math.pi * r_th0**2 * math.sqrt(2))
r_th1 = r_th0 * my.r_th1(Tmp_av, n0)
lmd_th1 = lmd_th0 * (r_th0 / r_th1)**2
#r_th2 = pow(2, 1/6) * math.sqrt(1 + 2/(3*Tmp_av))
r_th2 = r_th0 * my.r_th2(Tmp_av)
lmd_th2 = lmd_th0 * (r_th0 / r_th2)**2
k_th = 4 * lmd_th1 * math.sqrt(2 * Tmp_av / (math.pi * params['mu']))
c_th = params['mu'] / (6 * Tmp_av)
# --------------------------------- experimant data ------------------------------------------
r2 = []
dr = [0, 0, 0]
cubeSize = 2 * params['R']
cubeSzEff = params['R']
x_cm = []
r_cm = []
v_cm = []
for n in range(N0, N1):
x, v, m = my.read_frame(model_name, n)
if (my.find_key(keys, 'vcm')):
v_cm.append(my.find_cm(v, m))
else:
if (n == N0):
# set start conditions
x0 = cp.deepcopy(x)
x_real = cp.deepcopy(x)
x_prev = cp.deepcopy(x)
r2.append(0)
v_start_av = np.mean([my.length(_x) for _x in v])
else:
r2_sum = 0
for i in range(Nprt): # find <r^2> considering coords's shifts
for j in range(3):
dx = x[i][j] - x_prev[i][j]
if (dx > cubeSzEff): # re-shift coords
dx -= cubeSize
elif (dx < -cubeSzEff):
dx += cubeSize
x_real[i][j] += dx
# find real displacement
dr[j] = x_real[i][j] - x0[i][j]
r2_sum += my.dot(dr, dr)
r2.append(r2_sum / Nprt)
x_prev = cp.deepcopy(x)
x_cm.append(my.find_cm(x_real, m))
r_cm.append(my.length(x_cm[-1]))
if (pnrt_progress):
print('diffusion progress: ' + str(
(n + 1 - N0) / Nfrm * 100) + '% \r',
end='')
if (not my.find_key(keys, 'vcm')):
# --------------------------------- experimant analisys ------------------------------------------
# find proper tg
r1 = my.arrFnc(r2, math.sqrt)
big_time = 3
small_time = 0.5
approx_r2 = np.poly1d(np.polyfit(t[N0:N1], r2, 1))
k_exp = approx_r2.c[0]
tau = c_th * k_exp
c2 = int(tau * params['dumpDT'] * big_time)
if (c2 > Nfrm - 10):
c2 = Nfrm - 10
if (c2 < 10):
c2 = int(Nfrm / 2)
approx_r2 = np.poly1d(np.polyfit(t[(N0 + c2):N1], r2[c2:], 1))
k_exp = abs(approx_r2.c[0])
tau = c_th * k_exp
c2 = int(tau * params['dumpDT'] * big_time)
if (c2 > Nfrm - 5):
c2 = Nfrm - 5
if (c2 < 10):
c2 = int(Nfrm / 2)
c1 = int(tau * params['dumpDT'] * small_time)
if (c1 < 3):
c1 = 3
# in case of strange emergencies
bad_k_exp = (k_exp < my.myeps)
if (bad_k_exp):
if (k_exp < 0):
k_exp = -k_exp
if (k_exp < my.myeps):
k_exp = my.myeps
xa0 = abs(approx_r2(0))
#tau = xa0/k_exp
c_exp = xa0 / k_exp**2
x = my.arrFnc(t[(N0 + c2):N1], math.log)
y = my.arrFnc(r2[c2:], math.log)
logEnd_approx = np.poly1d(np.polyfit(x, y, 1))
x = my.arrFnc(t[N0 + 1:c1], math.log)
y = my.arrFnc(r2[1:c1], math.log)
logBeg_approx = np.poly1d(np.polyfit(x, y, 1))
x = t[N0 + 1:c1]
y = my.arrFnc(r2[1:c1], math.sqrt)
approx_r1 = np.poly1d(np.polyfit(x, y, 1))
#lmd_1 = math.sqrt(3*math.pi*xa0)/4
lmd_1 = my.lmd_1(xa0)
#lmd_2 = k_exp/4 * math.sqrt(math.pi*params['mu'] / (Tmp_av*2))
lmd_2 = my.lmd_2(k_exp, params['mu'], Tmp_av)
lmd_3 = my.lmd_3(logBeg_approx.c[0], logBeg_approx.c[1],
logEnd_approx.c[0], logEnd_approx.c[1], params['mu'],
Tmp_av) # tau -> lmd
lmd_4 = my.lmd_4(logBeg_approx.c[0], logBeg_approx.c[1],
logEnd_approx.c[0],
logEnd_approx.c[1]) # straight lmd
if (make_pics):
fig_c = -1
figs = []
if (not my.find_key(keys, 'vcm')):
# -------------------------------- r_cm(t) -----------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
cm = []
std_cm = []
x = t[N0:N1]
t**s = ['x', 'y', 'z']
for _j in range(3):
cm.append([x_cm[_i][_j] - x_cm[0][_j] for _i in range(Nfrm)])
std_cm.append(np.std(cm[_j]))
plt.plot(
x,
cm[_j],
'-',
label=t**s[_j] + '; std = ' +
str(my.str_sgn_round(std_cm[_j], 3))) # experiment data
x = [t[N0], t[N1 - 1]]
plt.plot(x, [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('xyz_cm')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102),
loc=3,
ncol=3,
mode="expand",
borderaxespad=0.)
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir,
'xyz_cm(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r2(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r2, '-') # experiment data
x = [t[N0 + 1], t[N1 - 1]]
y = [approx_r2(_x) for _x in x]
plt.plot(x, y, '--') # line approximation
x = t[N0:N1]
#y = [xa0*(_x/tau - 1 + math.exp(- _x/tau)) for _x in x]
r2_th = [
k_exp * (_x - tau * (1 - math.exp(-_x / tau))) for _x in x
]
plt.plot(x, r2_th, '--') # my approximation
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('<r^2>')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('r^2(t)')
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r2(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r2_err(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
x = t[N0:N1]
y = [r2[_i] - r2_th[_i] for _i in range(len(x))]
plt.plot(x, y, '-') # experiment data
plt.plot([t[N0 + 1], t[N1 - 1]], [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('<r^2> - <r^2>_th')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('<r^2> error')
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir,
'r2_err(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r2_err_rel(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
x = t[N0:N1]
y = [my.rel_err(r2[_i], r2_th[_i]) for _i in range(len(x))]
plt.plot(x, y, '-') # experiment data
plt.plot([t[N0 + 1], t[N1 - 1]], [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('err')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('|<r^2> / <r^2>_th - 1|')
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir,
'r2_err_rel(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- log(r2)(log(t)) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r2, '-') # experiment data
x = [t[N0 + 1], t[N0 + c2]]
y = [math.exp(logBeg_approx(math.log(_x))) for _x in x]
plt.plot(x, y, '--') # beginning approximation
x = [t[N0 + c1], t[N1 - 1]]
y = [math.exp(logEnd_approx(math.log(_x))) for _x in x]
plt.plot(x, y, '--') # ending approximation
x = t[N0:N1]
plt.plot(x, r2_th, '--') # my approximation
plt.xlabel('t')
plt.ylabel('<r^2>')
plt.grid(True)
plt.xscale('log')
plt.yscale('log')
plt.title('log(r2) | k_begin = ' +
str(my.str_sgn_round(logBeg_approx.c[0], 3)) +
'; k_end = ' +
str(my.str_sgn_round(logEnd_approx.c[0], 3)))
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir,
'r2(t)_loglog_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r1, '-') # experiment data
x = [t[N0 + 1], t[c2]]
y = [approx_r1(_x) for _x in x]
plt.plot(x, y, '--') # beginning approximation
x = t[N0:N1]
y = my.arrFnc(r2_th, math.sqrt)
plt.plot(x, y, '--') # my approximation
plt.xlabel('t')
plt.ylabel('sqrt(<r^2>)')
plt.grid(True)
#plt.title('sqrt(r2) | l_th = ' + str(my.str_sgn_round(lmd_th1,3)) + '; l_3 = ' + str(my.str_sgn_round(lmd_3,3)) + '; l_2 = ' + str(my.str_sgn_round(lmd_2,3)))
plt.title('sqrt(<r^2>)')
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r1(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- v_cm(t) -----------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
x = t[N0:N1]
dv_cm = []
std_dvcm = []
t**s = ['vx', 'vy', 'vz']
for _j in range(3):
v_av = np.mean(v_cm[:][_j])
dv_cm.append([v_cm[_i][_j] - v_av for _i in range(Nfrm)])
std_dvcm.append(np.std(dv_cm[_j]))
plt.plot(x,
dv_cm[_j],
'-',
label=t**s[_j] + '; std = ' +
str(my.str_sgn_round(std_dvcm[_j], 3))) # experiment data
x = [t[N0], t[N1 - 1]]
plt.plot(x, [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('v_cm')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102),
loc=3,
ncol=3,
mode="expand",
borderaxespad=0.)
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'v_cm(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
if (not my.find_key(keys, 'vcm')):
print(n0, Tmp_av, lmd_th0, lmd_th1, lmd_th2, lmd_1, lmd_2, lmd_3,
lmd_4)
if (draw_on_screen):
#print(c_th, c_exp, my.rel_err(c_th, c_exp))
input()
def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print('usage: ./E.py model_name [keys N0 N1]')
sys.exit(1)
model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params = my.std_start(args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
for i in range(N0, N1):
for j in range(3):
E[i,j] /= params['Ntot']
fig_c = -1
fig = []
draw_on_screen = my.find_key(keys, 'keep')
if(not draw_on_screen):
plt.switch_backend('Agg')
fig_c += 1
# 0
fig.append(plt.figure(fig_c))
plt.plot(t[N0:N1], E[N0:N1,2], '-', label = 'Etot')
plt.plot(t[N0:N1], E[N0:N1,0], '-', label = 'Ek')
plt.plot(t[N0:N1], E[N0:N1,1], '-', label = 'Ep')
plt.xlabel('time')
plt.ylabel('E')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102), loc=3,
ncol=3, mode="expand", borderaxespad=0.)
if(draw_on_screen):
fig[fig_c].show()
path = os.path.join(graph_dir, 'Energy3_' + time_gaps_str + '.png')
fig[fig_c].savefig(path)
# 1
E0 = np.mean(E[N0:N1,0]) + abs(np.mean(E[N0:N1,1]))
path = os.path.join(graph_dir, 'dE_norm_' + time_gaps_str + '.png')
E_av = np.mean(E[:,2])
#y = [(e_el - E[N0,2])/E0 for e_el in E[N0:N1,2]]
y = [(e_el - E_av)/E0 for e_el in E[N0:N1,2]]
fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=0, y_lbl='E/<E>-1', tit='E/<E> - 1 | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 2
path = os.path.join(graph_dir, 'Etot_' + time_gaps_str + '.png')
y = [_x*params['Ntot'] for _x in E[N0:N1, 2]]
fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=np.mean(y), y_lbl='Etot', tit='Etot | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 3
path = os.path.join(graph_dir, 'dE_normSQRT(N)_' + time_gaps_str + '.png')
#y = [(e_el - E[N0,2])*mth.sqrt(params['Ntot']) for e_el in E[N0:N1,2]]
y = [(e_el - E_av)*mth.sqrt(params['Ntot']) for e_el in E[N0:N1,2]]
fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=0, y_lbl='(E - <E>)/sqrt(N)', tit='Esqrt | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 4
path = os.path.join(graph_dir, 'dE_' + time_gaps_str + '.png')
#y = [(e_el - E[N0,2])*params['Ntot'] for e_el in E[N0:N1,2]]
y = [(e_el - E_av)*params['Ntot'] for e_el in E[N0:N1,2]]
fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], y, y0=0, y_lbl='E - <E>', tit='E - <E> | std = ' + my.str_sgn_round(np.std(y),3), pic_path=path, show_key=draw_on_screen)
# 5
path = os.path.join(graph_dir, 'Tmp_' + time_gaps_str + '.png')
fig_c, fig = my.plot_error(fig_c, fig, t[N0:N1], Tmp, y0=Tmp_av, y_lbl='Tmp', tit='Tmp | std/Tmp = ' + my.str_sgn_round(np.std(Tmp)/Tmp_av,3), pic_path=path, show_key=draw_on_screen)
if(draw_on_screen):
input()
def main():
args = sys.argv[1:]
argc_min = 1
if len(args) < argc_min:
print('usage: ./diffusion.py model_name [keys, N0, N1, Nprt]')
sys.exit(1)
model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params = my.std_start(
args, 0, 1, 2, 3)
# std_start(args, model_i, N0_i, N1_i):
# model_name, keys, graph_dir, time_gaps_str, N0, N1, Nfrm, E, Tmp, Tmp_av, t, stabTind, params
if (len(args) < 4):
Nprt = params['Ntot']
else:
Nprt = int(args[3])
if (len(args) == 1):
full_mode = 1
else:
full_mode = (my.find_key(keys, 'full_mode')
or my.find_key(keys, 'full'))
if (full_mode and (Nfrm < int(Nfrm / 2) + 5)):
print('too few frames for full_mode')
sys.exit(1)
draw_on_screen = my.find_key(keys, 'keep')
if (not draw_on_screen):
plt.switch_backend('Agg')
make_pics = (my.find_key(keys, 'pics') or draw_on_screen)
n0 = params['Ntot'] / math.pow(2 * params['R'], 3)
sgm_th0 = 1
lmd_th0 = 1 / (n0 * math.pi * math.sqrt(2))
sgm_th2 = pow(2, 1 / 6) * math.sqrt(1 + 2 / (3 * Tmp_av))
lmd_th2 = lmd_th0 / (sgm_th2 * sgm_th2)
sgm_th1 = math.pow(
(1 + math.sqrt(1 + 1.5 * Tmp_av + ((2 * n0)**2) * (n0**2 - 1))) / 2,
-1 / 6)
lmd_th1 = lmd_th0 / (sgm_th1 * sgm_th1)
k_th = 4 * lmd_th1 * math.sqrt(2 * Tmp_av / (math.pi * params['mu']))
r2 = []
dr = [0, 0, 0]
cubeSize = 2 * params['R']
cubeSzEff = params['R']
x_cm = []
r_cm = []
for n in range(N0, N1):
x, v, m = my.read_frame(model_name, n)
if (n == N0):
# set start conditions
x0 = cp.deepcopy(x)
x_real = cp.deepcopy(x)
x_prev = cp.deepcopy(x)
r2.append(0)
v_start_av = np.mean([my.length(_x) for _x in v])
else:
r2_sum = 0
for i in range(Nprt): # find <r^2> considering coords's shifts
for j in range(3):
dx = x[i][j] - x_prev[i][j]
if (dx > cubeSzEff): # re-shift coords
dx -= cubeSize
elif (dx < -cubeSzEff):
dx += cubeSize
x_real[i][j] += dx
# find real displacement
dr[j] = x_real[i][j] - x0[i][j]
r2_sum += my.dot(dr, dr)
r2.append(r2_sum / Nprt)
x_prev = cp.deepcopy(x)
x_cm.append(my.find_cm(x_real, m))
r_cm.append(my.length(x_cm[-1]))
if (draw_on_screen):
print('diffusion progress: ' + str(
(n + 1 - N0) / Nfrm * 100) + '% \r',
end='')
fig_c = -1
figs = []
# -------------------------------- r_cm(t) ------------------------------------------
if (make_pics):
fig_c += 1
figs.append(plt.figure(fig_c))
cm = []
std_cm = []
x = t[N0:N1]
t**s = ['x', 'y', 'z']
for _j in range(3):
cm.append([x_cm[_i][_j] - x_cm[0][_j] for _i in range(Nfrm)])
std_cm.append(np.std(cm[_j]))
plt.plot(x,
cm[_j],
'-',
label=t**s[_j] + '; std = ' +
str(my.str_sgn_round(std_cm[_j], 3))) # experiment data
x = [t[N0], t[N1 - 1]]
plt.plot(x, [0, 0], '--')
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('xyz_cm')
plt.grid(True)
plt.legend(bbox_to_anchor=(0., 1.02, 1., .102),
loc=3,
ncol=3,
mode="expand",
borderaxespad=0.)
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'xyz_cm(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
c2 = int(Nfrm / 2)
if (full_mode):
c1 = int(Nfrm / 4)
c3 = int(Nfrm / 100)
c4 = int(Nfrm / 8)
x = my.arrFnc(t[(N0 + c2):(N1 - c4)], math.log)
y = my.arrFnc(r2[c2:-c4], math.log)
logEnd_approx = np.poly1d(np.polyfit(x, y, 1))
x = my.arrFnc(t[N0 + 1:c3], math.log)
y = my.arrFnc(r2[1:c3], math.log)
logBeg_approx = np.poly1d(np.polyfit(x, y, 1))
x = t[N0 + 1:c3]
y = my.arrFnc(r2[1:c3], math.sqrt)
approx_r1 = np.poly1d(np.polyfit(x, y, 1))
else:
c1 = 0
approx_r2 = np.poly1d(np.polyfit(t[(N0 + c1):N1], r2[c1:], 1))
k_exp = approx_r2.c[0]
bad_k_exp = (k_exp < my.myeps)
if (bad_k_exp):
if (k_exp < 0):
k_exp = -k_exp
if (k_exp < my.myeps):
k_exp = my.myeps
# -------------------------------- r2(t) ------------------------------------------
if (make_pics):
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r2, '-') # experiment data
x = [t[N0], t[N1 - 1]]
plt.plot(x, [approx_r2(_x) for _x in x],
'--') # line experiment approximation
tau = abs(approx_r2(0)) / k_exp
x = t[N0:N1]
y = [k_exp * (_x - tau + tau * pow(math.e, -_x / tau)) for _x in x]
#plt.plot(x, [k_exp*(_x - tau + tau*math.exp(-_x/tau)) for _x in x], '--') # non-line experiment approximation
plt.plot(x, y, '--') # non-line experiment approximation
#plt.plot([t[c2], t[c2]], [min(r2), max(r2)], '--') # last part boundary
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.ticklabel_format(style='sci', axis='x', scilimits=(0, 0))
plt.xlabel('t')
plt.ylabel('<r^2>')
plt.grid(True)
#plt.title('r^2(t) | k_exp = ' + str(my.str_sgn_round(k_exp,3)) + ', k_th = ' + str(my.str_sgn_round(k_th,3)))
plt.title('r^2(t)')
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r2(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
lmd_1 = k_exp / 4 * math.sqrt(math.pi * params['mu'] / (Tmp_av * 2))
sgm_1 = 1 / math.sqrt(n0 * math.pi * lmd_1 * math.sqrt(2))
lmd_4 = math.sqrt(abs(approx_r2(0)) * math.pi * 3) / 4
if (draw_on_screen):
print('Tmp_av = ', Tmp_av)
print('sgm_th1 = ', sgm_th1)
print('lmd_th1 = ', lmd_th1)
print('sgm_1 = ', sgm_1)
print('lmd_1 = ', lmd_1)
print('lmd_4 = ', lmd_4)
if (full_mode):
i_log = 2
while (1):
tg = math.log(r2[i_log + 10] / r2[i_log]) / math.log(
t[N0 + i_log + 10] / t[N0 + i_log])
if (abs(2 - tg) > 0.2):
break
i_log += 1
if (i_log >= N1 - N0 - 10):
break
stab_time_log = t[i_log]
i_r1 = 2
r1 = my.arrFnc(r2, math.sqrt)
while (1):
tg = (r1[i_r1 + 10] - r1[i_r1]) / (t[N0 + i_r1 + 10] -
t[N0 + i_r1]) / v_start_av
if (abs(tg - 1) > 0.18):
break
i_r1 += 1
if (i_r1 >= N1 - N0 - 10):
break
stab_time_r1 = t[i_r1]
#lmd_2 = 2 * stab_time * math.sqrt(2*Tmp_av / (math.pi*params['mu']))
# it's incorrect to calculate lmd this way here, because in the beggining V doesn't have maxwell distribution
lmd_2 = stab_time_log * v_start_av
lmd_3 = stab_time_r1 * v_start_av
sgm_2 = 1 / math.sqrt(n0 * math.pi * lmd_2 * math.sqrt(2))
sgm_3 = 1 / math.sqrt(n0 * math.pi * lmd_3 * math.sqrt(2))
stab_time_th = lmd_th1 / 2 * math.sqrt(math.pi * params['mu'] /
(2 * Tmp_av))
if (draw_on_screen):
print('stab_time_th = ', stab_time_th)
print('stab_time_log = ', stab_time_log)
print('stab_time_r1 = ', stab_time_r1)
print('sgm_2 = ', sgm_2)
print('lmd_2 = ', lmd_2)
print('r2 = ', math.sqrt(r2[i_log]))
print('sgm_3 = ', sgm_3)
print('lmd_3 = ', lmd_3)
print('r1 = ', r1[i_r1])
else:
print(n0, Tmp_av, lmd_th0, lmd_th1, lmd_th2, lmd_1, lmd_2, lmd_3,
lmd_4)
if (make_pics):
# -------------------------------- log(r2)(log(t)) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r2, '-') # experiment data
x = [t[N0 + 1], t[N1 - 1]]
plt.plot(x, [math.exp(logBeg_approx(math.log(_x))) for _x in x],
'--') # beginning approximation
plt.plot(x, [math.exp(logEnd_approx(math.log(_x))) for _x in x],
'--') # ending approximation
#plt.plot(x, [lmd_th1**2, lmd_th1**2], '--')
#plt.plot(x, [lmd_1**2, lmd_1**2], '--')
#plt.plot([stab_time_th, stab_time_th], [min(r2), max(r2)], '--')
#plt.plot([t[c2], t[c2]], [min(r2), max(r2)], '--')
plt.xlabel('t')
plt.ylabel('<r^2>')
plt.grid(True)
plt.xscale('log')
plt.yscale('log')
plt.title('log(r2) | k_begin = ' +
str(my.str_sgn_round(logBeg_approx.c[0], 3)) +
'; k_end = ' +
str(my.str_sgn_round(logEnd_approx.c[0], 3)))
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir,
'r2(t)_loglog_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
# -------------------------------- r(t) ------------------------------------------
fig_c += 1
figs.append(plt.figure(fig_c))
plt.plot(t[N0:N1], r1, '-') # experiment data
x = [t[N0 + 1], t[c4]]
plt.plot(x, [approx_r1(_x) for _x in x],
'--') # beginning approximation
#plt.plot(x, [lmd_th1, lmd_th1], '--')
#plt.plot([stab_time_th, stab_time_th], [min(r1), max(r1)], '--')
#plt.plot([stab_time_r1, stab_time_r1], [min(r1), max(r1)], '--')
#plt.plot([t[c2], t[c2]], [min(r1), max(r1)], '--')
plt.xlabel('t')
plt.ylabel('sqrt(<r^2>)')
plt.grid(True)
#plt.title('sqrt(r2) | l_th = ' + str(my.str_sgn_round(lmd_th1,3)) + '; l_3 = ' + str(my.str_sgn_round(lmd_3,3)) + '; l_2 = ' + str(my.str_sgn_round(lmd_2,3)))
plt.title('sqrt(<r^2>)')
if (draw_on_screen):
figs[fig_c].show()
path = os.path.join(graph_dir, 'r1(t)_' + time_gaps_str + '.png')
figs[fig_c].savefig(path)
if (draw_on_screen):
input()