def main():
# Get user input.
args = parse_user_input()
_exec("rm -f ts-analyze.tar.bz2 irc_transition.xyz irc_transition.vib",
print_command=False)
# Standardize base name to "irc_transition".
shutil.copy2(args.ts, 'irc_transition.xyz')
# Run Q-Chem calculations..
QCT = QChem("irc_transition.xyz",
charge=args.charge,
mult=args.mult,
method=args.method,
basis=args.basis)
# Ensure stability.
QCT.make_stable()
# Single point calculation for bond order matrix.
QCT.jobtype = 'sp'
QCT.remextra = OrderedDict([('scf_final_print', '1')])
QCT.calculate()
np.savetxt("irc_transition.bnd",
QCT.load_qcout().qm_bondorder,
fmt="%8.3f")
# Frequency calculation.
QCT.jobtype = 'freq'
QCT.calculate()
QCT.write_vdata('irc_transition.vib')
tarexit()
def main():
# Get user input.
args = parse_user_input()
M = Molecule(args.initial)
# Write growing string input files.
# Note that cycles are "throttled" to 100, because larger numbers will hit queue time limits and we lose all the work :(
# with open("qcoptions.in",'w') as f: print >> f, qcoptions.format(method=args.method, basis=args.basis)
prepare_template(qcrem_default,
"qcoptions.in",
args.charge,
args.mult,
args.method,
args.basis,
epsilon=args.epsilon,
molecule=M)
with open("inpfile", 'w') as f:
print(inpfile.format(xyz=args.initial,
path=os.getcwd() + '/',
chg=args.charge,
mult=args.mult,
cyc=min(100, args.cycles),
npts=len(M),
images=args.images),
file=f)
# Bootleg file-based interface for triggering stability analysis.
if args.stab: _exec("touch Do_Stability_Analysis", print_command=False)
# Execute the growing string calculation.
try:
_exec("gstring.exe", print_command=True, print_to_screen=True)
_exec("cp $(ls str[0-9]*.xyz -v | tail -1) final-string.xyz",
print_command=True,
persist=True)
Images = None
for qcout in os.popen("ls gs[0-9][0-9].out -v").readlines():
if Images == None:
Images = Molecule(qcout.strip(),
build_topology=False).without('qcrems')
else:
Images += Molecule(qcout.strip(),
build_topology=False).without('qcrems')
Images.get_populations().write('final-string.pop', ftype="xyz")
except:
tarexit.include = ['*']
tarexit()
# Archive files and exit.
tarexit()
def QCOptIC(*args, **kwargs):
"""
Try to run a Q-Chem geometry optimization; if it fails for some
reason, then try Cartesian coordinates.
"""
OptOut = QCOpt(*args, cart=False, **kwargs)
if OptOut.qcerr == 'OPTIMIZE fatal error':
print("Internal cartesian coordinates failed - trying Cartesian")
OptOut = QCOpt(*args, cart=True, **kwargs)
# Return success on maximum cycles reached.
if len(OptOut.qcerr) == 0 or OptOut.qcerr == 'Maximum optimization cycles reached':
return OptOut
else:
print(("Geometry optimization failed! (%s)" % OptOut.qcerr))
tarexit()
def main():
# Get user input.
args = parse_user_input()
# Start timer.
click()
# Run Q-Chem geometry optimization.
M = QCOptIC(args.initial, args.charge, args.mult, args.method, args.basis, cycles=args.cycles)
# Select frames where the energy is monotonically decreasing.
M = M[monotonic_decreasing(M.qm_energies)]
# Write optimization results to file.
M.write('optimize.xyz')
# Write Mulliken charge and spin populations to file.
QS = M.get_populations()
QS.write('optimize.pop', ftype='xyz')
# Archive and exit.
tarexit()
def main():
# Get user input.
args = parse_user_input()
# Start timer.
click()
# Run single point calculation to determine bond order matrix.
QCSP = QChem(args.initial,
charge=args.charge,
mult=args.mult,
method=args.method,
basis=args.basis)
QCSP.make_stable()
QCSP.jobtype = 'sp'
QCSP.remextra = OrderedDict([('scf_final_print', '1')])
QCSP.calculate()
# Rebuild bond list using the bond order matrix.
M = QCSP.load_qcout()
InitE = M.qm_energies[0]
M.bonds = []
# Determined from an incredibly small # of data points.
# In example_1.xyz, an O-H distance of 1.89 Angstrom had a BO of 0.094 (so it should be > 0.1)
# In example_1.xyz, a C-H distance of 1.39 Angstrom had a BO of 0.305 (so it should be < 0.3)
bo_thresh = 0.2
numbonds = 0
bondfactor = 0.0
print("Atoms QM-BO Distance")
for i in range(M.na):
for j in range(i + 1, M.na):
# Print out the ones that are "almost" bonds.
if M.qm_bondorder[i, j] > 0.1:
print("%s%i%s%s%i % .3f % .3f" %
(M.elem[i], i, '-' if M.qm_bondorder[i, j] > bo_thresh
else ' ', M.elem[j], j, M.qm_bondorder[i, j],
np.linalg.norm(M.xyzs[-1][i] - M.xyzs[-1][j])))
if M.qm_bondorder[i, j] > bo_thresh:
M.bonds.append((i, j))
numbonds += 1
if M.qm_bondorder[i, j] <= 1:
bondfactor += M.qm_bondorder[i, j]
else:
# Count double bonds as 1
bondfactor += 1
bondfactor /= numbonds
M.build_topology()
subxyz = []
subef = []
subna = []
subchg = []
submult = []
subvalid = []
SumFrags = []
# Divide calculation into subsystems.
for subg in M.molecules:
matoms = subg.nodes()
frag = M.atom_select(matoms)
# Determine output file name.
fout = os.path.splitext(
args.initial)[0] + '.sub_%i' % len(subxyz) + '.xyz'
# Assume we are getting the Mulliken charges from the last frame, it's safer.
# Write the output .xyz file.
Chg = sum(M.qm_mulliken_charges[-1][matoms])
SpnZ = sum(M.qm_mulliken_spins[-1][matoms])
Spn2 = sum([i**2 for i in M.qm_mulliken_spins[-1][matoms]])
frag.comms = [
"Molecular formula %s atoms %s from %s charge %+.3f sz %+.3f sz^2 %.3f"
%
(subg.ef(), commadash(subg.nodes()), args.initial, Chg, SpnZ, Spn2)
]
frag.write(fout)
subxyz.append(fout)
subef.append(subg.ef())
subna.append(frag.na)
# Determine integer charge and multiplicity.
ichg, chgpass = extract_int(np.array([Chg]), 0.5, 1.0, label="charge")
ispn, spnpass = extract_int(np.array([abs(SpnZ)]),
0.5,
1.0,
label="spin-z")
nproton = sum([Elements.index(i) for i in frag.elem])
nelectron = nproton + ichg
# If calculation is valid, append to the list of xyz/chg/mult to be calculated.
if (not chgpass or not spnpass):
print("Cannot determine charge and spin for fragment %s\n" %
subg.ef())
subchg.append(None)
submult.append(None)
subvalid.append(False)
elif ((nelectron - ispn) / 2) * 2 != (nelectron - ispn):
print("Inconsistent charge and spin-z for fragment %s\n" %
subg.ef())
subchg.append(None)
submult.append(None)
subvalid.append(False)
else:
subchg.append(ichg)
submult.append(ispn + 1)
subvalid.append(True)
print("%i/%i subcalculations are valid" % (len(subvalid), sum(subvalid)))
for i in range(len(subxyz)):
print("%s formula %-12s charge %i mult %i %s" %
(subxyz[i], subef[i], subchg[i], submult[i],
"valid" if subvalid[i] else "invalid"))
fragid = open('fragmentid.txt', 'w')
for formula in subef:
fragid.write(formula + " ")
fragid.write("\nBondfactor: " + str(bondfactor))
if not all(subvalid): fragid.write("\ninvalid")
fragid.close()
# Archive and exit
tarexit()
def main():
# Get user input.
args = parse_user_input()
if len(args.methods) > 2:
logger.error("Unsure what to do with >2 electronic structure methods")
raise RuntimeError
# Delete the result from previous jobs
_exec("rm -rf ts_result.tar.bz2", print_command=False)
# Perform transition state search.
# First run the TS-calculation with the smaller basis set
QCTS1 = QChemTS(args.tsest,
charge=args.charge,
mult=args.mult,
method=args.methods[0],
basis=args.bases[0],
finalize=(len(args.methods) == 1),
qcin='qcts1.in',
vout='irc_transition.vib')
QCTS1.write('ts1.xyz')
if len(args.methods) == 2:
print(' --== \x1b[1;92mUpgrading\x1b[0m ==--')
QCTS2 = QChemTS("ts1.xyz",
charge=args.charge,
mult=args.mult,
method=args.methods[1],
basis=args.bases[1],
finalize=True,
qcin='qcts2.in',
vout='irc_transition.vib')
QCTS2.write('ts2.xyz')
qcdir = QCTS2.qcdir
shutil.copy2('ts2.xyz', 'ts.xyz')
else:
qcdir = QCTS1.qcdir
shutil.copy2('ts1.xyz', 'ts.xyz')
# Intrinsic reaction coordinate calculation.
print("Intrinsic reaction coordinate..")
# Process and save IRC results.
M_IRC, E_IRC = QChemIRC("ts.xyz",
charge=args.charge,
mult=args.mult,
method=args.methods[-1],
basis=args.bases[-1],
qcdir=qcdir,
xyz0=args.initpath)
M_IRC.write("irc.xyz")
M_IRC.get_populations().write('irc.pop', ftype='xyz')
# Save the IRC energy as a function of arc length.
ArcMol = arc(M_IRC, RMSD=True)
ArcMolCumul = np.insert(np.cumsum(ArcMol), 0, 0.0)
np.savetxt("irc.nrg",
np.hstack((ArcMolCumul.reshape(-1, 1), E_IRC.reshape(-1, 1))),
fmt="% 14.6f",
header="Arclength(Ang) Energy(kcal/mol)")
# Create IRC with equally spaced structures.
M_IRC_EV = SpaceIRC(M_IRC, E_IRC, RMSD=True)
M_IRC_EV.write("irc_spaced.xyz")
# Run two final single point calculations with SCF_FINAL_PRINT set to 1
M_IRC[0].write("irc_reactant.xyz")
M_IRC[-1].write("irc_product.xyz")
QCR = QChem("irc_reactant.xyz",
charge=args.charge,
mult=args.mult,
method=args.methods[-1],
basis=args.bases[-1])
QCP = QChem("irc_product.xyz",
charge=args.charge,
mult=args.mult,
method=args.methods[-1],
basis=args.bases[-1])
shutil.copy2("ts.xyz", "irc_transition.xyz")
QCT = QChem("irc_transition.xyz",
charge=args.charge,
mult=args.mult,
method=args.methods[-1],
basis=args.bases[-1])
def FinalSCF(SP):
SP.make_stable()
SP.jobtype = 'sp'
SP.remextra = OrderedDict([('scf_final_print', '1')])
SP.calculate()
FinalSCF(QCR)
FinalSCF(QCP)
FinalSCF(QCT)
np.savetxt("irc_reactant.bnd", QCR.load_qcout().qm_bondorder, fmt="%8.3f")
np.savetxt("irc_product.bnd", QCP.load_qcout().qm_bondorder, fmt="%8.3f")
np.savetxt("irc_transition.bnd",
QCT.load_qcout().qm_bondorder,
fmt="%8.3f")
# Calculate ZPEs, entropy, enthalpy for Delta-G calcs
# Should be able to take out freq calcs of R and P once we get can confidently get rid of this section.
QCR.remextra = OrderedDict()
QCP.remextra = OrderedDict()
QCT.remextra = OrderedDict()
QCR.freq()
R = QCR.load_qcout()
QCP.freq()
P = QCP.load_qcout()
QCT.freq()
T = QCT.load_qcout()
nrgfile = open('deltaG.nrg', 'w')
deltaH = P.qm_energies[0] * Ha_to_kcalmol + P.qm_zpe[
0] - R.qm_energies[0] * Ha_to_kcalmol - R.qm_zpe[0]
deltaG = deltaH - P.qm_entropy[0] * 0.29815 + P.qm_enthalpy[
0] + R.qm_entropy[0] * 0.29815 - R.qm_enthalpy[0]
Ha = T.qm_energies[0] * Ha_to_kcalmol + T.qm_zpe[
0] - R.qm_energies[0] * Ha_to_kcalmol - R.qm_zpe[0]
Ga = Ha - T.qm_entropy[0] * 0.29815 + T.qm_enthalpy[
0] + R.qm_entropy[0] * 0.29815 - R.qm_enthalpy[0]
nrgfile.write(
"=> ** The following data is referenced to reactant and product complexes **\n"
)
nrgfile.write(
"=> ** WARNING! Data may not be accurate in cases with >1 molecule **\n"
)
nrgfile.write(
"=> ** Activation enthalpy H_a (0K) = %.4f kcal/mol **\n"
% Ha)
nrgfile.write(
"=> ** Activation Gibbs energy G_a (STP) = %.4f kcal/mol **\n"
% Ga)
nrgfile.write(
"=> ** Delta-H(0K) = %.4f kcal/mol **\n"
% deltaH)
nrgfile.write(
"=> ** Delta-G(STP) = %.4f kcal/mol **\n"
% deltaG)
# Calculate Delta-G's based on fragment information from reactant and product
# Get data from fragment nrg files
if args.fragpath == None:
fragpath = os.path.abspath('../../../../../fragments')
else:
fragpath = args.fragpath
formulas = []
nrg = []
zpe = []
entr = []
enth = []
validity = []
for frm in os.listdir(fragpath):
optdir = os.path.join(fragpath, frm, "opt")
if os.path.exists(os.path.join(optdir, 'fragmentopt.nrg')):
fragnrgfile = open(os.path.join(optdir, 'fragmentopt.nrg'))
formulas.append(fragnrgfile.readline().strip())
nrg.append(float(fragnrgfile.readline().split()[3]))
zpe.append(float(fragnrgfile.readline().split()[2]))
entr.append(float(fragnrgfile.readline().split()[3]))
enth.append(float(fragnrgfile.readline().split()[3]))
validity.append(fragnrgfile.readline().strip())
fragnrgfile.close()
# Compare list of molecules to choose right energy
formulasR = []
formulasP = []
nrgR = 0.0
nrgP = 0.0
R.build_topology()
for subg in R.molecules:
formulasR.append(subg.ef())
formulasR = sorted(formulasR)
P.build_topology()
for subg in P.molecules:
formulasP.append(subg.ef())
formulasP = sorted(formulasP)
for i in range(len(formulas)):
formlist = sorted(formulas[i].split())
if formlist == formulasR and validity[i] != "invalid":
nrgR = nrg[i]
zpeR = zpe[i]
entrR = entr[i]
enthR = enth[i]
if formlist == formulasP and validity[i] != "invalid":
nrgP = nrg[i]
zpeP = zpe[i]
entrP = entr[i]
enthP = enth[i]
# Calculate energetics
if nrgR != 0.0:
Ha = T.qm_energies[0] * Ha_to_kcalmol + T.qm_zpe[
0] - nrgR * Ha_to_kcalmol - zpeR
Ga = Ha - T.qm_entropy[0] * 0.29815 + T.qm_enthalpy[
0] + entrR * 0.29815 - enthR
nrgfile.write(
"=> ## The following data is calculated referenced to isolated reactant and product molecules:\n"
)
nrgfile.write(
"=> ## Activation enthalpy H_a (0K) = %.4f kcal/mol ##\n"
% Ha)
nrgfile.write(
"=> ## Activation Gibbs energy G_a (STP) = %.4f kcal/mol ##\n"
% Ga)
else:
nrgfile.write(
"=> Reactant state could not be identified among fragment calculations\n"
)
nrgfile.write(
"=> No energetics referenced to isolated molecules will be calculated for this pathway\n"
)
if nrgR != 0.0 and nrgP != 0.0:
deltaH = nrgP * Ha_to_kcalmol + zpeP - nrgR * Ha_to_kcalmol - zpeR
deltaG = deltaH - entrP * 0.29815 + enthP + entrR * 0.29815 - enthR
nrgfile.write(
"=> ## Delta-H(0K) = %.4f kcal/mol **\n"
% deltaH)
nrgfile.write(
"=> ## Delta-G(STP) = %.4f kcal/mol **\n"
% deltaG)
elif nrgP == 0.0:
nrgfile.write(
"=> Product state could not be identified among fragment calculations\n"
)
nrgfile.write(
"=> No reaction energies referenced to isolated molecules will be calculated for this pathway\n"
)
nrgfile.close()
print("\x1b[1;92mIRC Success!\x1b[0m")
tarexit()
def main():
# Get user input.
args = parse_user_input()
# Start timer.
click()
subxyz = []
subna = []
subchg = []
submult = []
subvalid = []
subefstart = []
subeffinal = []
SumFrags = []
fragfiles = []
# Pick out the files in the tarfile that have the structure "example*.sub_*.xyz"
idhome = os.path.abspath('..')
tar = tarfile.open(os.path.join(idhome, 'fragmentid.tar.bz2'), 'r')
for tarinfo in tar:
splitlist = tarinfo.name.split(".")
if len(splitlist) > 2:
if splitlist[2] == "xyz":
subxyz.append(tarinfo.name)
fragfiles.append(tarinfo)
# Extract these files from the tarfile
tar.extractall(members=fragfiles)
tar.close()
# Load files as molecules
for frag in subxyz:
M = Molecule(frag)
M.read_comm_charge_mult()
subchg.append(M.charge)
submult.append(M.mult)
subna.append(M.na)
efstart = re.search('(?<=Molecular formula )\w+', M.comms[0]).group(0)
subefstart.append(efstart)
print("Running individual optimizations.")
# Run individual geometry optimizations.
FragE = 0.0
FragZPE = 0.0
FragEntr = 0.0
FragEnth = 0.0
for i in range(len(subxyz)):
if subna[i] > 1:
M = QCOptIC(subxyz[i],
subchg[i],
submult[i],
args.method,
args.basis,
cycles=args.cycles,
qcin='%s.opt.in' % os.path.splitext(subxyz[i])[0])
# Select frames where the energy is monotonically decreasing.
M = M[monotonic_decreasing(M.qm_energies)]
else:
# Special case of a single atom
QCSP = QChem(subxyz[i],
charge=subchg[i],
mult=submult[i],
method=args.method,
basis=args.basis,
qcin='%s.sp.in' % os.path.splitext(subxyz[i])[0])
QCSP.make_stable()
QCSP.jobtype = 'sp'
QCSP.calculate()
M = QCSP.load_qcout()
# Write optimization final result to file.
M = M[-1]
fragoptfile = os.path.splitext(subxyz[i])[0] + ".opt.xyz"
M.write(fragoptfile)
QCFR = QChem(fragoptfile,
charge=subchg[i],
mult=submult[i],
method=args.method,
basis=args.basis,
qcin='%s.freq.in' % os.path.splitext(fragoptfile)[0])
QCFR.freq()
M = QCFR.load_qcout()
# Print out new molecular formulas.
# This time we should be able to use covalent radii.
M.build_topology(force_bonds=True)
optformula = ' '.join([m.ef() for m in M.molecules])
subeffinal.append(optformula)
print(("%s.opt.xyz : formula %s; charge %i; mult %i; energy %f Ha;"
"ZPE %f kcal/mol; entropy %f cal/mol.K; enthalpy %f kcal/mol" %
(os.path.splitext(subxyz[i])[0], optformula, subchg[i],
submult[i], M.qm_energies[0], M.qm_zpe[0], M.qm_entropy[0],
M.qm_enthalpy[0])))
FragE += M.qm_energies[0]
FragZPE += M.qm_zpe[0]
FragEntr += M.qm_entropy[0]
FragEnth += M.qm_enthalpy[0]
SumFrags.append(M[0])
for fragment in SumFrags:
fragment.write('fragmentopt.xyz', append=True)
if subefstart != subeffinal:
print("Fragments changed during optimization, calculation invalid")
print("Final electronic energy (Ha) of optimized frags: % 18.10f" % FragE)
print("Final ZPE (kcal/mol) of optimized frags: % 18.10f" % FragZPE)
print("Final entropy (cal/mol.K) of optimized frags: % 18.10f" % FragEntr)
print("Final enthalpy (kcal/mol) of optimized frags: % 18.10f" % FragEnth)
nrg = open('fragmentopt.nrg', 'w')
for subef in subeffinal:
nrg.write(subef + " ")
nrg.write("\nTotal electronic energy: %f Ha\n" % FragE)
nrg.write("Total ZPE: %f kcal/mol\n" % FragZPE)
nrg.write("Total entropy (STP): %f cal/mol.K\n" % FragEntr)
nrg.write("Total enthalpy (STP): %f kcal/mol\n" % FragEnth)
if subefstart != subeffinal: nrg.write("invalid")
nrg.close()
# Archive and exit.
tarexit()
