def do_dynamics(mdlogf, atoms, dyn, rend_b, rend_t, v, dt, deltaY_old, theta, dtheta, \
L, thres_Z, interval, traj, M, twist, save = True):
write_line_own(mdlogf, '# Hysteresis simul begins \n', 'w')
#kink_vanis = False
y0 = atoms.positions[rend_b, 1]
i,m = 0, 0
time = 0.
while 0 < theta:
theta -= dtheta
twist.set_angle(theta)
dyn.run(1)
if i % interval == 0:
epot, ekin = saveAndPrint(atoms, traj, False)[:2]
deltaY = deltaY_old + atoms.positions[rend_b, 1] - y0
R = get_R(L, deltaY)
hmax = np.max(atoms.positions[:,2]) - 3.4 #subsract the height of the plane
data = [time, deltaY, R, theta, hmax, epot, ekin, epot + ekin]
#data = [i * dt, deltaY, R, theta, epot, ekin, epot + ekin]
if save:
stringi = ''
for k,d in enumerate(data):
if k == 0:
stringi += '%.2f ' %d
elif k == 1 or k == 2:
stringi += '%.4f ' %d
else:
stringi += '%.12f ' %d
write_line_own(mdlogf, stringi + '\n', 'a')
print i/interval, theta / (2*np.pi) * 360, R
if np.max(atoms.positions[:,2]) < thres_Z and m == 0:
write_line_own(mdlogf, '# Kink vanish! ' + '\n', 'a')
print ' kink vanished! '
m += 1
#kink_vanis = True
if i % int(M/100) == 0: theta / (2 * np.pi) *360
#if kink_vanis: m += 1
i += 1
time += dt
def do_dynamics(mdlogf, atoms, dyn, rend_b, rend_t, v, dt, deltaY_old, theta, dtheta, \
L, thres_Z, interval, traj, M, twist, save = True):
write_line_own(mdlogf, '# Hysteresis simul begins \n', 'w')
#kink_vanis = False
y0 = atoms.positions[rend_b, 1]
i, m = 0, 0
time = 0.
while 0 < theta:
theta -= dtheta
twist.set_angle(theta)
dyn.run(1)
if i % interval == 0:
epot, ekin = saveAndPrint(atoms, traj, False)[:2]
deltaY = deltaY_old + atoms.positions[rend_b, 1] - y0
R = get_R(L, deltaY)
hmax = np.max(
atoms.positions[:, 2]) - 3.4 #subsract the height of the plane
data = [time, deltaY, R, theta, hmax, epot, ekin, epot + ekin]
#data = [i * dt, deltaY, R, theta, epot, ekin, epot + ekin]
if save:
stringi = ''
for k, d in enumerate(data):
if k == 0:
stringi += '%.2f ' % d
elif k == 1 or k == 2:
stringi += '%.4f ' % d
else:
stringi += '%.12f ' % d
write_line_own(mdlogf, stringi + '\n', 'a')
print i / interval, theta / (2 * np.pi) * 360, R
if np.max(atoms.positions[:, 2]) < thres_Z and m == 0:
write_line_own(mdlogf, '# Kink vanish! ' + '\n', 'a')
print ' kink vanished! '
m += 1
#kink_vanis = True
if i % int(M / 100) == 0: theta / (2 * np.pi) * 360
#if kink_vanis: m += 1
i += 1
time += dt
def shearDyn(width, ratio, edge, save=False, force_dir_update=True):
atoms, L, W, length_int, b_idxs = create_stucture(ratio,
width,
edge,
key='rib+base')
view(atoms)
# FIXES
constraints, add_LJ, rend_b, rend_t = get_constraints(
atoms, edge, bond, b_idxs)
# END FIXES
# CALCULATOR LAMMPS
calc = LAMMPS(parameters=get_lammps_params())
atoms.set_calculator(calc)
# END CALCULATOR
# TRAJECTORY
add = ''
if force_dir_update: add = '_ff'
mdfile, mdlogfile, mdrelax, simulfile = get_fileName('LJ', edge + add, width, \
length_int, int(T), taito)
if save: traj = PickleTrajectory(mdfile, 'w', atoms)
else: traj = None
#data = np.zeros((M/interval, 5))
# RELAX
atoms.set_constraint(add_LJ)
dyn = BFGS(atoms, trajectory=mdrelax)
dyn.run(fmax=0.05)
# FIX AFTER RELAXATION
atoms.set_constraint(constraints)
# DYNAMICS
dyn = Langevin(atoms, dt * units.fs, T * units.kB, fric)
n = 0
header = '#t [fs], shift y [Angstrom], Rad, epot_tot [eV], ekin_tot [eV], etot_tot [eV] \n'
write_line_own(mdlogfile, header, 'w')
if T != 0:
# put initial MaxwellBoltzmann velocity distribution
mbd(atoms, T * units.kB)
deltaY = 0.
eta = 1.1 # ratio between the lengths of the streched and compressed side of the ribbon.
r = L / W # length to width ratio.
deltaYMax = W / 2. * (eta + 1) / (eta - 1) * (1 - np.cos(2 * r *
(eta - 1) /
(eta + 1)))
# Estimate for the required shift
dy = v * dt
M = deltaYMax / dy
interval = int(M / 1000)
kink_formed = False
dir_vec = np.array([0., 1., 0.])
i, m = 0, 0
print 'width = %i, length = %i' % (width, length_int)
while m <= int(M / 30):
if tau < i * dt:
deltaY += dy * dir_vec[1]
for ind in rend_b:
atoms[ind].position[:] += dy * dir_vec
dyn.run(1)
if i % interval == 0:
epot, ekin = saveAndPrint(atoms, traj, False)[:2]
R = get_R(L, deltaY)
if force_dir_update: dir_vec = get_dir(atoms, rend_b, rend_t)
data = [i * dt, deltaY, R, epot, ekin, epot + ekin]
if save:
stringi = ''
for k, d in enumerate(data):
if k == 0:
stringi += '%.2f ' % d
elif k == 1 or k == 2:
stringi += '%.4f ' % d
else:
stringi += '%.12f ' % d
write_line_own(mdlogfile, stringi + '\n', 'a')
n += 1
if thres_Z < np.max(atoms.positions[:, 2]) and m == 0:
idxs = np.where(thres_Z < atoms.positions[:, 2])
write_line_own(mdlogfile,
'# Kink! at idxs %s' % str(idxs) + '\n', 'a')
print ' kink formed! '
kink_formed = True
if save and T != 0 and i * dt == tau:
write_line_own(mdlogfile, '# Thermalization complete. ' + '\n',
'a')
if i % int(M / 100) == 0: print str(i / int(M / 100)) + ' ~ % done'
if kink_formed: m += 1
i += 1
make_simul_param_file(simulfile, W, L, width, length_int, v, dy, T, \
dt, fric, thres_Z, interval, deltaY, M, edge)
def shearDyn(params_set, pot_key, save = False):
bond = params_set['bond']
T = params_set['T']
taito = params_set['taito']
dt, fric= params_set['dt'], params_set['fric']
tau = params_set['tau']
vmax = params_set['vmax']
vMAX = params_set['vMAX']
thres_Z = params_set['thresZ']
width = params_set['width']
ratio = params_set['ratio']
edge = params_set['edge']
atoms, L, W, length_int, b_idxs = \
create_stucture(ratio, width, edge, key = 'top', a = bond)
mdfile, mdlogfile, mdrelax, simulfile, folder, relaxed \
= get_fileName(pot_key, edge + '_twistRod', width, \
length_int, vmax * 1000, int(T), taito)
#view(atoms)
# FIXES
constraints, add_pot, twist, rend_b, rend_t = \
get_constraints(atoms, edge, bond, b_idxs, \
key = 'twist_p', pot = pot_key)
# END FIXES
if relaxed:
atoms = PickleTrajectory(mdrelax, 'r')[-1]
else:
trans = trans_atomsKC(atoms.positions[rend_b], edge, bond)
atoms.translate(trans)
#plot_posits(atoms, edge, bond)
# CALCULATOR LAMMPS
calc = LAMMPS(parameters=get_lammps_params())
atoms.set_calculator(calc)
# END CALCULATOR
# TRAJECTORY
if save: traj = PickleTrajectory(mdfile, 'w', atoms)
else: traj = None
#data = np.zeros((M/interval, 5))
# RELAX
atoms.set_constraint(add_pot)
dyn = BFGS(atoms, trajectory = mdrelax)
dyn.run(fmax=0.05)
dist = np.linalg.norm(atoms.positions[rend_b] - atoms.positions[rend_t])
twist.set_dist(dist)
# FIX AFTER RELAXATION
atoms.set_constraint(constraints)
# DYNAMICS
dyn = Langevin(atoms, dt*units.fs, T*units.kB, fric)
header = '#t [fs], shift y [Angstrom], Rad, theta [rad], hmax [A], epot_tot [eV], ekin_tot [eV], etot_tot [eV], F [eV/angst] \n'
write_line_own(mdlogfile, header, 'w')
if T != 0:
# put initial MaxwellBoltzmann velocity distribution
mbd(atoms, T*units.kB)
y0 = atoms.positions[rend_b, 1]
kink_formed = False
kink_vanished = False
i = 0
print 'width = %i, length = %i, v=%.6f' %(width, length_int, vmax)
M_therm = int(tau / dt)
dyn.run(M_therm)
M = int(2 * L / (np.pi * dt * vmax))
M_min = int(2 * L / (np.pi * dt * vMAX))
dtheta = np.pi / 2 / M
dtheta_max = np.pi / 2 / M_min
interval = int( M / 1000 )
theta, time, m = 0., 0., 0
i_kink = 0
while 0. <= theta:
if not kink_formed:
if theta < np.pi/4:
theta += dtheta_max
else:
theta += dtheta
twist.set_angle(theta)
else:
if i_kink / 10 < m:
theta -= dtheta
twist.set_angle(theta)
dyn.run(1)
if i % interval == 0:
epot, ekin = saveAndPrint(atoms, traj, False)[:2]
deltaY = atoms.positions[rend_b, 1] - y0
hmax = np.max(atoms.positions[:,2]) #substract the height of the plane?
R = get_R(L, deltaY)
data = [time, deltaY, R, theta, hmax, epot, ekin, epot + ekin]
if save:
stringi = ''
for k,d in enumerate(data):
if k == 0:
stringi += '%.2f ' %d
elif k == 1 or k == 2:
stringi += '%.4f ' %d
else:
stringi += '%.12f ' %d
write_line_own(mdlogfile, stringi + '\n', 'a')
if thres_Z < hmax and not kink_formed:
idxs = np.where(thres_Z < atoms.positions[:,2])
write_line_own(mdlogfile, '# Kink! at idxs %s' %str(idxs) + '\n', 'a')
print ' kink formed! ' + str(i / interval)
kink_formed = True
i_kink = i
if hmax < 3.6 and kink_formed and not kink_vanished:
write_line_own(mdlogfile, '# Kink vanished! \n', 'a')
print ' kink vanished '
kink_vanished = True
print i/interval, theta / (2*np.pi) * 360, R
if kink_formed: m += 1
i += 1
time += dt
make_simul_param_file(simulfile, W, L, width, length_int, dtheta/dt, dtheta, T, \
dt, fric, thres_Z, interval, deltaY, theta, i, edge)
return folder
def shearDyn(params_set, pot_key, save=False):
bond = params_set['bond']
T = params_set['T']
taito = params_set['taito']
dt, fric = params_set['dt'], params_set['fric']
tau = params_set['tau']
vmax = params_set['vmax']
vMAX = params_set['vMAX']
thres_Z = params_set['thresZ']
width = params_set['width']
ratio = params_set['ratio']
edge = params_set['edge']
atoms, L, W, length_int, b_idxs = \
create_stucture(ratio, width, edge, key = 'top', a = bond)
mdfile, mdlogfile, mdrelax, simulfile, folder, relaxed \
= get_fileName(pot_key, edge + '_twistRod', width, \
length_int, vmax * 1000, int(T), taito)
#view(atoms)
# FIXES
constraints, add_pot, twist, rend_b, rend_t = \
get_constraints(atoms, edge, bond, b_idxs, \
key = 'twist_p', pot = pot_key)
# END FIXES
if relaxed:
atoms = PickleTrajectory(mdrelax, 'r')[-1]
else:
trans = trans_atomsKC(atoms.positions[rend_b], edge, bond)
atoms.translate(trans)
#plot_posits(atoms, edge, bond)
# CALCULATOR LAMMPS
calc = LAMMPS(parameters=get_lammps_params())
atoms.set_calculator(calc)
# END CALCULATOR
# TRAJECTORY
if save: traj = PickleTrajectory(mdfile, 'w', atoms)
else: traj = None
#data = np.zeros((M/interval, 5))
# RELAX
atoms.set_constraint(add_pot)
dyn = BFGS(atoms, trajectory=mdrelax)
dyn.run(fmax=0.05)
dist = np.linalg.norm(atoms.positions[rend_b] - atoms.positions[rend_t])
twist.set_dist(dist)
# FIX AFTER RELAXATION
atoms.set_constraint(constraints)
# DYNAMICS
dyn = Langevin(atoms, dt * units.fs, T * units.kB, fric)
header = '#t [fs], shift y [Angstrom], Rad, theta [rad], hmax [A], epot_tot [eV], ekin_tot [eV], etot_tot [eV], F [eV/angst] \n'
write_line_own(mdlogfile, header, 'w')
if T != 0:
# put initial MaxwellBoltzmann velocity distribution
mbd(atoms, T * units.kB)
y0 = atoms.positions[rend_b, 1]
kink_formed = False
kink_vanished = False
i = 0
print 'width = %i, length = %i, v=%.6f' % (width, length_int, vmax)
M_therm = int(tau / dt)
dyn.run(M_therm)
M = int(2 * L / (np.pi * dt * vmax))
M_min = int(2 * L / (np.pi * dt * vMAX))
dtheta = np.pi / 2 / M
dtheta_max = np.pi / 2 / M_min
interval = int(M / 1000)
theta, time, m = 0., 0., 0
i_kink = 0
while 0. <= theta:
if not kink_formed:
if theta < np.pi / 4:
theta += dtheta_max
else:
theta += dtheta
twist.set_angle(theta)
else:
if i_kink / 10 < m:
theta -= dtheta
twist.set_angle(theta)
dyn.run(1)
if i % interval == 0:
epot, ekin = saveAndPrint(atoms, traj, False)[:2]
deltaY = atoms.positions[rend_b, 1] - y0
hmax = np.max(
atoms.positions[:, 2]) #substract the height of the plane?
R = get_R(L, deltaY)
data = [time, deltaY, R, theta, hmax, epot, ekin, epot + ekin]
if save:
stringi = ''
for k, d in enumerate(data):
if k == 0:
stringi += '%.2f ' % d
elif k == 1 or k == 2:
stringi += '%.4f ' % d
else:
stringi += '%.12f ' % d
write_line_own(mdlogfile, stringi + '\n', 'a')
if thres_Z < hmax and not kink_formed:
idxs = np.where(thres_Z < atoms.positions[:, 2])
write_line_own(mdlogfile,
'# Kink! at idxs %s' % str(idxs) + '\n', 'a')
print ' kink formed! ' + str(i / interval)
kink_formed = True
i_kink = i
if hmax < 3.6 and kink_formed and not kink_vanished:
write_line_own(mdlogfile, '# Kink vanished! \n', 'a')
print ' kink vanished '
kink_vanished = True
print i / interval, theta / (2 * np.pi) * 360, R
if kink_formed: m += 1
i += 1
time += dt
make_simul_param_file(simulfile, W, L, width, length_int, dtheta/dt, dtheta, T, \
dt, fric, thres_Z, interval, deltaY, theta, i, edge)
return folder
def shearDyn(width, ratio, edge, save=False):
atoms, L, W, length_int, b_idxs = create_stucture(ratio,
width,
edge,
key='top')
view(atoms)
# FIXES
constraints, add_LJ, twist, rend_b, rend_t = get_constraints(atoms,
edge,
bond,
b_idxs,
key='twist')
# END FIXES
# CALCULATOR LAMMPS
calc = LAMMPS(parameters=get_lammps_params())
atoms.set_calculator(calc)
# END CALCULATOR
# TRAJECTORY
mdfile, mdlogfile, mdrelax, simulfile = get_fileName('LJ', edge + '_twist', width, \
length_int, int(T), taito)
if save: traj = PickleTrajectory(mdfile, 'w', atoms)
else: traj = None
#data = np.zeros((M/interval, 5))
# RELAX
atoms.set_constraint(add_LJ)
dyn = BFGS(atoms, trajectory=mdrelax)
dyn.run(fmax=0.05)
# FIX AFTER RELAXATION
atoms.set_constraint(constraints)
# DYNAMICS
dyn = Langevin(atoms, dt * units.fs, T * units.kB, fric)
header = '#t [fs], shift y [Angstrom], Rad, epot_tot [eV], \
ekin_tot [eV], etot_tot [eV], F [eV/angst] \n'
write_line_own(mdlogfile, header, 'w')
if T != 0:
# put initial MaxwellBoltzmann velocity distribution
mbd(atoms, T * units.kB)
y0 = atoms.positions[rend_b, 1][0]
kink_formed = False
dir_vec = np.array([0., 1., 0.])
i, m = 0, 0
interval = 20
print 'width = %i, length = %i' % (width, length_int)
M_therm = int(tau / dt)
dyn.run(M_therm)
F = 0.
while not kink_formed:
pos_0 = atoms.positions[rend_b][0]
F_vec = F * np.array([dir_vec[1], -dir_vec[0], 0.])
twist.set_F(F_vec)
dyn.run(interval)
i += interval
epot, ekin = saveAndPrint(atoms, traj, False)[:2]
pos_1 = atoms.positions[rend_b][0]
deltaY = pos_1[1] - y0
v = np.sign(pos_1[1] - pos_0[1]) * np.linalg.norm(
(pos_1 - pos_0) / (interval * dt))
R = get_R(L, deltaY)
dir_vec = get_dir(atoms, rend_b, rend_t)
data = [
i * dt, deltaY, R, epot, ekin, epot + ekin, F_vec[0], F_vec[1],
F_vec[2]
]
#if vmax/5 < v: F -= .01
if v < vmax / 5 and not kink_formed: F += .01
print deltaY, v, F
if save:
stringi = ''
for k, d in enumerate(data):
if k == 0:
stringi += '%.2f ' % d
elif k == 1 or k == 2:
stringi += '%.4f ' % d
else:
stringi += '%.12f ' % d
write_line_own(mdlogfile, stringi + '\n', 'a')
if thres_Z < np.max(atoms.positions[:, 2]) and m == 0:
idxs = np.where(thres_Z < atoms.positions[:, 2])
write_line_own(mdlogfile, '# Kink! at idxs %s' % str(idxs) + '\n',
'a')
print ' kink formed! '
kink_formed = True
F = 0
if save and T != 0 and i * dt == tau:
write_line_own(mdlogfile, '# Thermalization complete. ' + '\n',
'a')
if i % 100 == 0: print i
if kink_formed: m += 1
make_simul_param_file(simulfile, W, L, width, length_int, v, deltaY/i, T, \
dt, fric, thres_Z, interval, deltaY, i, edge)
