def test_qmmm_acn():
import numpy as np
import ase.units as units
from ase import Atoms
from ase.calculators.acn import (ACN, m_me, r_cn, r_mec,
sigma_me, sigma_c, sigma_n,
epsilon_me, epsilon_c, epsilon_n)
from ase.calculators.qmmm import SimpleQMMM, LJInteractionsGeneral, EIQMMM
from ase.constraints import FixLinearTriatomic
from ase.optimize import BFGS
# From https://www.sciencedirect.com/science/article/pii/S0166128099002079
eref = 4.9 * units.kcal / units.mol
dref = 3.368
aref = 79.1
sigma = np.array([sigma_me, sigma_c, sigma_n])
epsilon = np.array([epsilon_me, epsilon_c, epsilon_n])
inter = LJInteractionsGeneral(sigma, epsilon, sigma, epsilon, 3)
for calc in [ACN(),
SimpleQMMM([0, 1, 2], ACN(), ACN(), ACN()),
SimpleQMMM([0, 1, 2], ACN(), ACN(), ACN(), vacuum=3.0),
EIQMMM([0, 1, 2], ACN(), ACN(), inter),
EIQMMM([0, 1, 2], ACN(), ACN(), inter, vacuum=3.0),
EIQMMM([3, 4, 5], ACN(), ACN(), inter, vacuum=3.0)]:
dimer = Atoms('CCNCCN',
[(-r_mec, 0, 0),
(0, 0, 0),
(r_cn, 0, 0),
(r_mec, 3.7, 0),
(0, 3.7, 0),
(-r_cn, 3.7, 0)])
masses = dimer.get_masses()
masses[::3] = m_me
dimer.set_masses(masses)
dimer.calc = calc
fixd = FixLinearTriatomic(triples=[(0, 1, 2), (3, 4, 5)])
dimer.set_constraint(fixd)
opt = BFGS(dimer, maxstep=0.04,
trajectory=calc.name + '.traj', logfile=calc.name + 'd.log')
opt.run(0.001, steps=1000)
e0 = dimer.get_potential_energy()
d0 = dimer.get_distance(1, 4)
a0 = dimer.get_angle(2, 1, 4)
fmt = '{0:>25}: {1:.3f} {2:.3f} {3:.1f}'
print(fmt.format(calc.name, -e0, d0, a0))
assert abs(e0 + eref) < 0.013
assert abs(d0 - dref) < 0.224
assert abs(a0 - aref) < 2.9
print(fmt.format('reference', eref, dref, aref))
def test_rattle_linear():
"""Test RATTLE and QM/MM for rigid linear acetonitrile."""
import numpy as np
from ase import Atoms
from ase.calculators.acn import (ACN, m_me, r_cn, r_mec, sigma_me, sigma_c,
sigma_n, epsilon_me, epsilon_c, epsilon_n)
from ase.calculators.qmmm import SimpleQMMM, EIQMMM, LJInteractionsGeneral
from ase.md.verlet import VelocityVerlet
from ase.constraints import FixLinearTriatomic
import ase.units as units
sigma = np.array([sigma_me, sigma_c, sigma_n])
epsilon = np.array([epsilon_me, epsilon_c, epsilon_n])
i = LJInteractionsGeneral(sigma, epsilon, sigma, epsilon, 3)
for calc in [
ACN(),
SimpleQMMM([0, 1, 2], ACN(), ACN(), ACN()),
EIQMMM([0, 1, 2], ACN(), ACN(), i)
]:
dimer = Atoms('CCNCCN', [(-r_mec, 0, 0), (0, 0, 0), (r_cn, 0, 0),
(r_mec, 3.7, 0), (0, 3.7, 0),
(-r_cn, 3.7, 0)])
masses = dimer.get_masses()
masses[::3] = m_me
dimer.set_masses(masses)
fixd = FixLinearTriatomic(triples=[(0, 1, 2), (3, 4, 5)])
dimer.set_constraint(fixd)
dimer.calc = calc
d1 = dimer[:3].get_all_distances()
d2 = dimer[3:].get_all_distances()
e = dimer.get_potential_energy()
md = VelocityVerlet(dimer,
2.0 * units.fs,
trajectory=calc.name + '.traj',
logfile=calc.name + '.log',
loginterval=20)
md.run(100)
de = dimer.get_potential_energy() - e
assert np.all(abs(dimer[:3].get_all_distances() - d1) < 1e-10)
assert np.all(abs(dimer[3:].get_all_distances() - d2) < 1e-10)
assert abs(de - -0.005) < 0.001
sig2,
eps2, # arrays for TIP4P from earlier
rc=7.5)
mmatoms.calc = calc
mmatoms.calc.initialize(mmatoms)
# LJ arrays for the 'QM' subsystem
sig_qm = np.array([sigNa, sigNa])
eps_qm = np.array([epsNa, epsNa])
# For the MM subsystem, tuple of arrays (counterion, water)
sig_mm = (np.array([sigNa]), sig2)
eps_mm = (np.array([epsNa]), eps2)
lj = LJInteractionsGeneral(sig_qm, eps_qm, sig_mm, eps_mm, 2)
ecomb, fcomb1, fcomb2 = lj.calculate(faux_qm, mmatoms, np.array([0, 0, 0]))
# This should give the same result as if not using CombineMM, on a sum
# of these systems:
# A: All the Na atoms in the 'QM' region
# B: LJInteractions between the 'QM' Na and the 'MM' Na
# C: -LJinteractions between the 'MM' Na and the 'MM' Water
# A:
mmatoms = dimer
mmatoms.calc = []
sig_qm = np.concatenate((sig_qm, sig_qm))
eps_qm = np.concatenate((eps_qm, eps_qm))
sig_mm = sig_mm[1]
def test_qmmm_tip4p():
from math import cos, sin, pi
import numpy as np
#import matplotlib.pyplot as plt
import ase.units as units
from ase import Atoms
from ase.calculators.tip4p import TIP4P, epsilon0, sigma0, rOH, angleHOH
from ase.calculators.qmmm import (SimpleQMMM, EIQMMM, LJInteractions,
LJInteractionsGeneral)
from ase.constraints import FixInternals
from ase.optimize import BFGS
r = rOH
a = angleHOH * pi / 180
# From https://doi.org/10.1063/1.445869
eexp = 6.24 * units.kcal / units.mol
dexp = 2.75
aexp = 46
D = np.linspace(2.5, 3.5, 30)
i = LJInteractions({('O', 'O'): (epsilon0, sigma0)})
# General LJ interaction object
sigma_mm = np.array([sigma0, 0, 0])
epsilon_mm = np.array([epsilon0, 0, 0])
sigma_qm = np.array([sigma0, 0, 0])
epsilon_qm = np.array([epsilon0, 0, 0])
ig = LJInteractionsGeneral(sigma_qm, epsilon_qm, sigma_mm, epsilon_mm, 3)
for calc in [
TIP4P(),
SimpleQMMM([0, 1, 2], TIP4P(), TIP4P(), TIP4P()),
SimpleQMMM([0, 1, 2], TIP4P(), TIP4P(), TIP4P(), vacuum=3.0),
EIQMMM([0, 1, 2], TIP4P(), TIP4P(), i),
EIQMMM([3, 4, 5], TIP4P(), TIP4P(), i, vacuum=3.0),
EIQMMM([0, 1, 2], TIP4P(), TIP4P(), i, vacuum=3.0),
EIQMMM([0, 1, 2], TIP4P(), TIP4P(), ig),
EIQMMM([3, 4, 5], TIP4P(), TIP4P(), ig, vacuum=3.0),
EIQMMM([0, 1, 2], TIP4P(), TIP4P(), ig, vacuum=3.0)
]:
dimer = Atoms('OH2OH2', [(0, 0, 0), (r * cos(a), 0, r * sin(a)),
(r, 0, 0), (0, 0, 0),
(r * cos(a / 2), r * sin(a / 2), 0),
(r * cos(a / 2), -r * sin(a / 2), 0)])
dimer.calc = calc
E = []
F = []
for d in D:
dimer.positions[3:, 0] += d - dimer.positions[3, 0]
E.append(dimer.get_potential_energy())
F.append(dimer.get_forces())
F = np.array(F)
#plt.plot(D, E)
F1 = np.polyval(np.polyder(np.polyfit(D, E, 7)), D)
F2 = F[:, :3, 0].sum(1)
error = abs(F1 - F2).max()
assert error < 0.01
dimer.constraints = FixInternals(bonds=[(r, (0, 1)), (r, (0, 2)),
(r, (3, 4)), (r, (3, 5))],
angles=[(a, (2, 0, 1)),
(a, (5, 3, 4))])
opt = BFGS(dimer,
maxstep=0.04,
trajectory=calc.name + '.traj',
logfile=calc.name + 'd.log')
opt.run(0.01)
e0 = dimer.get_potential_energy()
d0 = dimer.get_distance(0, 3)
R = dimer.positions
v1 = R[2] - R[3]
v2 = R[3] - (R[5] + R[4]) / 2
a0 = np.arccos(
np.dot(v1, v2) /
(np.dot(v1, v1) * np.dot(v2, v2))**0.5) / np.pi * 180
fmt = '{0:>23}: {1:.3f} {2:.3f} {3:.3f} {4:.1f}'
print(fmt.format(calc.name, -min(E), -e0, d0, a0))
assert abs(e0 + eexp) < 0.002
assert abs(d0 - dexp) < 0.006
assert abs(a0 - aexp) < 2.5
print(fmt.format('reference', 9.999, eexp, dexp, aexp))
"""Test RATTLE and QM/MM for rigid linear acetonitrile."""
import numpy as np
from ase import Atoms
from ase.calculators.acn import (ACN, m_me, r_cn, r_mec, sigma_me, sigma_c,
sigma_n, epsilon_me, epsilon_c, epsilon_n)
from ase.calculators.qmmm import SimpleQMMM, EIQMMM, LJInteractionsGeneral
from ase.md.verlet import VelocityVerlet
from ase.constraints import FixLinearTriatomic
import ase.units as units
sigma = np.array([sigma_me, sigma_c, sigma_n])
epsilon = np.array([epsilon_me, epsilon_c, epsilon_n])
i = LJInteractionsGeneral(sigma, epsilon, sigma, epsilon, 3)
for calc in [
ACN(),
SimpleQMMM([0, 1, 2], ACN(), ACN(), ACN()),
EIQMMM([0, 1, 2], ACN(), ACN(), i)
]:
dimer = Atoms('CCNCCN', [(-r_mec, 0, 0), (0, 0, 0), (r_cn, 0, 0),
(r_mec, 3.7, 0), (0, 3.7, 0), (-r_cn, 3.7, 0)])
masses = dimer.get_masses()
masses[::3] = m_me
dimer.set_masses(masses)
fixd = FixLinearTriatomic(triples=[(0, 1, 2), (3, 4, 5)])
# From http://dx.doi.org/10.1063/1.445869
eexp = 6.50 * units.kcal / units.mol
dexp = 2.74
aexp = 27
D = np.linspace(2.5, 3.5, 30)
i = LJInteractions({('O', 'O'): (epsilon0, sigma0)})
# General LJ interaction object
sigma_mm = np.array([0, 0, sigma0])
epsilon_mm = np.array([0, 0, epsilon0])
sigma_qm = np.array([0, 0, sigma0])
epsilon_qm = np.array([0, 0, epsilon0])
ig = LJInteractionsGeneral(sigma_qm, epsilon_qm, sigma_mm, epsilon_mm, 3)
for calc in [TIP3P(),
SimpleQMMM([0, 1, 2], TIP3P(), TIP3P(), TIP3P()),
SimpleQMMM([0, 1, 2], TIP3P(), TIP3P(), TIP3P(), vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), i),
EIQMMM([3, 4, 5], TIP3P(), TIP3P(), i, vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), i, vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), ig),
EIQMMM([3, 4, 5], TIP3P(), TIP3P(), ig, vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), ig, vacuum=3.0)]:
dimer = Atoms('H2OH2O',
[(r * cos(a), 0, r * sin(a)),
(r, 0, 0),
(0, 0, 0),
(r * cos(a / 2), r * sin(a / 2), 0),
def test_qmmm(testdir):
r = rOH
a = angleHOH * pi / 180
# From https://doi.org/10.1063/1.445869
eexp = 6.50 * units.kcal / units.mol
dexp = 2.74
aexp = 27
D = np.linspace(2.5, 3.5, 30)
i = LJInteractions({('O', 'O'): (epsilon0, sigma0)})
# General LJ interaction object
sigma_mm = np.array([0, 0, sigma0])
epsilon_mm = np.array([0, 0, epsilon0])
sigma_qm = np.array([0, 0, sigma0])
epsilon_qm = np.array([0, 0, epsilon0])
ig = LJInteractionsGeneral(sigma_qm, epsilon_qm, sigma_mm, epsilon_mm, 3)
for calc in [
TIP3P(),
SimpleQMMM([0, 1, 2], TIP3P(), TIP3P(), TIP3P()),
SimpleQMMM([0, 1, 2], TIP3P(), TIP3P(), TIP3P(), vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), i),
EIQMMM([3, 4, 5], TIP3P(), TIP3P(), i, vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), i, vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), ig),
EIQMMM([3, 4, 5], TIP3P(), TIP3P(), ig, vacuum=3.0),
EIQMMM([0, 1, 2], TIP3P(), TIP3P(), ig, vacuum=3.0)
]:
dimer = Atoms('H2OH2O',
[(r * cos(a), 0, r * sin(a)), (r, 0, 0), (0, 0, 0),
(r * cos(a / 2), r * sin(a / 2), 0),
(r * cos(a / 2), -r * sin(a / 2), 0), (0, 0, 0)])
dimer.calc = calc
E = []
F = []
for d in D:
dimer.positions[3:, 0] += d - dimer.positions[5, 0]
E.append(dimer.get_potential_energy())
F.append(dimer.get_forces())
F = np.array(F)
F1 = np.polyval(np.polyder(np.polyfit(D, E, 7)), D)
F2 = F[:, :3, 0].sum(1)
error = abs(F1 - F2).max()
assert error < 0.01
dimer.constraints = FixInternals(bonds=[(r, (0, 2)), (r, (1, 2)),
(r, (3, 5)), (r, (4, 5))],
angles_deg=[
(np.degrees(a), (0, 2, 1)),
(np.degrees(a), (3, 5, 4))
])
opt = GPMin(dimer,
trajectory=calc.name + '.traj',
logfile=calc.name + 'd.log')
opt.run(0.01)
e0 = dimer.get_potential_energy()
d0 = dimer.get_distance(2, 5)
R = dimer.positions
v1 = R[1] - R[5]
v2 = R[5] - (R[3] + R[4]) / 2
a0 = np.arccos(
np.dot(v1, v2) /
(np.dot(v1, v1) * np.dot(v2, v2))**0.5) / np.pi * 180
fmt = '{0:>20}: {1:.3f} {2:.3f} {3:.3f} {4:.1f}'
print(fmt.format(calc.name, -min(E), -e0, d0, a0))
assert abs(e0 + eexp) < 0.002
assert abs(d0 - dexp) < 0.01
assert abs(a0 - aexp) < 4
print(fmt.format('reference', 9.999, eexp, dexp, aexp))
def test_combine_mm():
"""Test CombineMM forces by combining tip3p and tip4p with them selves, and
by combining tip3p with tip4p and testing against numerical forces.
Also test LJInterationsGeneral with CombineMM """
from math import cos, sin, pi
import numpy as np
from ase import Atoms
from ase import units
from ase.calculators.counterions import AtomicCounterIon as ACI
from ase.calculators.combine_mm import CombineMM
from ase.calculators.qmmm import LJInteractionsGeneral
from ase.calculators.tip3p import TIP3P, rOH, angleHOH
from ase.calculators.tip4p import TIP4P
from ase.calculators.tip3p import epsilon0 as eps3
from ase.calculators.tip3p import sigma0 as sig3
from ase.calculators.tip4p import epsilon0 as eps4
from ase.calculators.tip4p import sigma0 as sig4
def make_atoms():
r = rOH
a = angleHOH * pi / 180
dimer = Atoms('H2OH2O',
[(r * cos(a), 0, r * sin(a)), (r, 0, 0), (0, 0, 0),
(r * cos(a / 2), r * sin(a / 2), 0),
(r * cos(a / 2), -r * sin(a / 2), 0), (0, 0, 0)])
dimer = dimer[[2, 0, 1, 5, 3, 4]]
# put O-O distance in the cutoff range
dimer.positions[3:, 0] += 2.8
return dimer
dimer = make_atoms()
rc = 3.0
for (TIPnP, (eps, sig), nm) in zip([TIP3P, TIP4P],
((eps3, sig3), (eps4, sig4)), [3, 3]):
dimer.calc = TIPnP(rc=rc, width=1.0)
F1 = dimer.get_forces()
sigma = np.array([sig, 0, 0])
epsilon = np.array([eps, 0, 0])
dimer.calc = CombineMM([0, 1, 2],
nm,
nm,
TIPnP(rc=rc, width=1.0),
TIPnP(rc=rc, width=1.0),
sigma,
epsilon,
sigma,
epsilon,
rc=rc,
width=1.0)
F2 = dimer.get_forces()
dF = F1 - F2
print(TIPnP)
print(dF)
assert abs(dF).max() < 1e-8
# Also check a TIP3P/TIP4P combination against numerical forces:
eps1 = np.array([eps3, 0, 0])
sig1 = np.array([sig3, 0, 0])
eps2 = np.array([eps4, 0, 0])
sig2 = np.array([sig4, 0, 0])
dimer.calc = CombineMM([0, 1, 2], 3, 3, TIP3P(rc, 1.0), TIP4P(rc, 1.0),
sig1, eps1, sig2, eps2, rc, 1.0)
F2 = dimer.get_forces()
Fn = dimer.calc.calculate_numerical_forces(dimer, 1e-7)
dF = F2 - Fn
print('TIP3P/TIP4P')
print(dF)
assert abs(dF).max() < 1e-8
# LJInteractionsGeneral with CombineMM.
# As it is used within EIQMMM, but avoiding long calculations for tests.
# Total system is a unit test system comprised of:
# 2 Na ions playing the role of a 'QM' subsystem
# 2 Na ions as the 'Counterions'
# 2 Water molecules
dimer.calc = []
faux_qm = Atoms('2Na', positions=np.array([[1.4, -4, 0], [1.4, 4, 0]]))
ions = Atoms('2Na', positions=np.array([[1.4, 0, -4], [1.4, 0, 4]]))
mmatoms = ions + dimer
sigNa = 1.868 * (1.0 / 2.0)**(1.0 / 6.0) * 10
epsNa = 0.00277 * units.kcal / units.mol
# ACI for atoms 0 and 1 of the MM subsystem (2 and 3 for the total system)
# 1 atom 'per molecule'. The rest is TIP4P, 3 atoms per molecule:
calc = CombineMM(
[0, 1],
1,
3,
ACI(1, epsNa, sigNa), # calc 1
TIP4P(), # calc 2
[sigNa],
[epsNa], # LJs for subsystem 1
sig2,
eps2, # arrays for TIP4P from earlier
rc=7.5)
mmatoms.calc = calc
mmatoms.calc.initialize(mmatoms)
# LJ arrays for the 'QM' subsystem
sig_qm = np.array([sigNa, sigNa])
eps_qm = np.array([epsNa, epsNa])
# For the MM subsystem, tuple of arrays (counterion, water)
sig_mm = (np.array([sigNa]), sig2)
eps_mm = (np.array([epsNa]), eps2)
lj = LJInteractionsGeneral(sig_qm, eps_qm, sig_mm, eps_mm, 2)
ecomb, fcomb1, fcomb2 = lj.calculate(faux_qm, mmatoms, np.array([0, 0, 0]))
# This should give the same result as if not using CombineMM, on a sum
# of these systems:
# A: All the Na atoms in the 'QM' region
# B: LJInteractions between the 'QM' Na and the 'MM' Na
# C: -LJinteractions between the 'MM' Na and the 'MM' Water
# A:
mmatoms = dimer
mmatoms.calc = []
sig_qm = np.concatenate((sig_qm, sig_qm))
eps_qm = np.concatenate((eps_qm, eps_qm))
sig_mm = sig_mm[1]
eps_mm = eps_mm[1]
lj = LJInteractionsGeneral(sig_qm, eps_qm, sig_mm, eps_mm, 4)
ea, fa1, fa2 = lj.calculate(faux_qm + ions, mmatoms, np.array([0, 0, 0]))
# B:
lj = LJInteractionsGeneral(sig_qm[:2], eps_qm[:2], sig_qm[:2], eps_qm[:2],
2, 2)
eb, fb1, fb2, = lj.calculate(faux_qm, ions, np.array([0, 0, 0]))
# C:
lj = LJInteractionsGeneral(sig_qm[:2], eps_qm[:2], sig_mm, eps_mm, 2, 3)
ec, fc1, fc2, = lj.calculate(ions, dimer, np.array([0, 0, 0]))
assert ecomb - (ea + eb) + ec == 0
