def __init__(self, system, model, fn_traj=None):
'''
**Arguments**
system
An instance of the System class and contains all the
system information
model
An instance of the Model class and contains all the info
to define the total PES and its electrostatic contribution.
**Optional Arguments**
fn_traj
A file name to store the perturbation trajectories to or to
read the trajectories from if the file exists. The trajectories
are stored/read after Pickling.
'''
self.system = system
self.model = model
self.pert_theory = RelaxedGeoPertTheory(system, model)
self.cost = HessianFCCost(system, model)
self.fn_traj = fn_traj
#SHLL 1508
#-- new attributes for storing potential types
self.stretch_pot_kind = system.stretch_pot_kind
self.bend_pot_kind = system.bend_pot_kind
class Program(object):
'''
The central class to manage the entire program.
'''
def __init__(self, system, model, fn_traj=None):
'''
**Arguments**
system
An instance of the System class and contains all the
system information
model
An instance of the Model class and contains all the info
to define the total PES and its electrostatic contribution.
**Optional Arguments**
fn_traj
A file name to store the perturbation trajectories to or to
read the trajectories from if the file exists. The trajectories
are stored/read after Pickling.
'''
self.system = system
self.model = model
self.pert_theory = RelaxedGeoPertTheory(system, model)
self.cost = HessianFCCost(system, model)
self.fn_traj = fn_traj
#SHLL 1508
#-- new attributes for storing potential types
self.stretch_pot_kind = system.stretch_pot_kind
self.bend_pot_kind = system.bend_pot_kind
#SHLL end
def generate_trajectories(self, skip_dihedrals=True, verbose=True):
'''
Generate a perturbation trajectory for all ics (dihedrals can be
excluded and store the coordinates in a dictionary.
**Optional Arguments**
skip_dihedrals
If set to True, the dihedral ff parameters will not
be calculated.
'''
maxlength = max([len(icname) for icname in self.model.val.pot.terms.keys()]) + 2
#Check if a filename with trajectories is given. If the file exists,
#read it and return the trajectories
if self.fn_traj is not None:
if os.path.isfile(self.fn_traj):
with open(self.fn_traj,'r') as f:
trajectories = cPickle.load(f)
return trajectories
#Generate trajectories from scratch
trajectories = {}
all_ics = []
for icname in sorted(self.model.val.pot.terms.keys()):
if skip_dihedrals and icname.startswith('dihed'):
continue
ics = self.system.ics[icname]
for ic in ics:
all_ics.append(ic)
if verbose:
print ' %s will generate %i trajectories' %(
icname+' '*(maxlength-len(icname)), len(ics)
)
results = paracontext.map(self.pert_theory.generate, all_ics)
for i in xrange(len(all_ics)):
trajectories[all_ics[i].name] = results[i]
#Check if we need to write the generated trajectories to a file
if self.fn_traj is not None:
with open(self.fn_traj,'w') as f:
cPickle.dump(trajectories,f)
return trajectories
#SHLL 1508
#-- extra parameters not needed anymore
# def estimate_from_pt(self, trajectories, skip_dihedrals=True, verbose=True, stretch_pot_kind='harmonic', bend_pot_kind='harmonic'):
#original
def estimate_from_pt(self, trajectories, skip_dihedrals=True, verbose=True):
#SHLL end
'''
Second Step of force field development: calculate harmonic force field
parameters for every internal coordinate separately from perturbation
trajectories.
**Arguments**
trajectories
A dictionairy containing numpy arrays representing perturbation
trajectories for each icname.
**Optional Arguments**
skip_dihedrals
If set to True, the dihedral ff parameters will not
be calculated.
'''
ff = FFTable()
#SHLL 1606
#-- transfer potential info from program to fftable
ff.stretch_pot_kind = self.stretch_pot_kind
ff.bend_pot_kind = self.bend_pot_kind
#SHLL end
maxlength = max([len(icname) for icname in self.model.val.pot.terms.keys()]) + 2
for icname in sorted(self.model.val.pot.terms.keys()):
ics = self.system.ics[icname]
if skip_dihedrals and icname.startswith('dihed'):
continue
ks = DataArray(unit=ics[0].kunit)
# print 'kunit:',ics[0].kunit #GBdebug
q0s = DataArray(unit=ics[0].qunit)
for ic in ics:
#SHLL 1508
#-- estimate spf or harmcos potential params
if icname.startswith('bond') and self.stretch_pot_kind.lower()=='spf':
k, q0 = self.pert_theory.estimate(ic,trajectories[ic.name], pot_kind=self.stretch_pot_kind)
elif icname.startswith('angle') and self.bend_pot_kind.lower()=='harmcos':
k, q0 = self.pert_theory.estimate(ic,trajectories[ic.name], pot_kind=self.bend_pot_kind)
else:
k, q0 = self.pert_theory.estimate(ic,trajectories[ic.name], pot_kind='harmonic')
#original
# k, q0 = self.pert_theory.estimate(ic,trajectories[ic.name])
#SHLL end
ks.append(k)
q0s.append(q0)
ff.add(icname, ks, q0s)
descr = icname + ' '*(maxlength-len(icname))
if verbose:
print ' %s K = %s q0 = %s' % (
descr, ks.string(), q0s.string()
)
self.model.val.update_fftable(ff)
return ff
def refine_cost(self, verbose=True):
'''
Second step of force field development: refine the force constants
using a Hessian least squares cost function.
'''
fcs = self.cost.estimate()
self.model.val.update_fcs(fcs)
fftab = self.model.val.get_fftable()
#SHLL 1606
#-- transfer potential info from program to fftable
fftab.stretch_pot_kind = self.stretch_pot_kind
fftab.bend_pot_kind = self.bend_pot_kind
#SHLL end
if verbose:
fftab.print_screen()
return fftab
def run(self):
'''
Run all steps of the QuickFF methodology to derive a covalent
force field. This method returns an instance of the class
:class:`quickff.fftable.FFTable`, which contains all force field
parameters.
'''
print header
print sysinfo()
print '~'*120+'\n'
print 'System information:\n'
self.system.print_atom_info()
print '\nModel information:\n'
self.model.print_info()
print '\nDetermine dihedral potentials\n'
self.model.val.determine_dihedral_potentials(self.system)
print '\nDetermine the coordinates of the perturbation trajectories\n'
self.trajectories = self.generate_trajectories()
print '\nEstimating all pars for bonds, bends and opdists\n'
fftab = self.estimate_from_pt(self.trajectories)
print '\nRefining force constants using a Hessian LSQ cost\n'
fftab = self.refine_cost()
print '\n'+'~'*120+'\n'
print 'Time: ' + datetime.datetime.now().isoformat().replace('T', ' ') + '\n'
print footer
return fftab
def plot_pt(self, icname, start=None, end=None, steps=51, verbose=True):
'''
Generate the perturbation trajectories and plot the energy
contributions along the trajectory for all ics with a name
compatible with icname.
**Arguments**
icname
A string describing for which ics the perturbation trajectories
should be generated.
'''
#Logging
if verbose:
print header
print sysinfo()
print '~'*120+'\n'
print 'System information:\n'
self.system.print_atom_info()
print '\nModel information:\n'
self.model.print_info()
print '\nDetermine the coordinates of the perturbation trajectories\n'
#Reading/generating trajectories
trajectories = {}
if self.fn_traj is not None:
if os.path.isfile(self.fn_traj):
with open(self.fn_traj,'r') as f:
trajectories = cPickle.load(f)
for i, ic in enumerate(self.system.ics[icname]):
if ic.name in trajectories.keys():
#already read
if verbose:
print ' %s Read %2i/%i from %s' %(
icname, i+1, len(self.system.ics[icname]), self.fn_traj
)
else:
#generating
if verbose:
sys.stdout.write(' %s Generating %2i/%i' %(
icname, i+1, len(self.system.ics[icname])
))
sys.stdout.flush()
try:
trajectories[ic.name] = self.pert_theory.generate(ic, start=start, end=end, steps=51)
print ''
except KeyboardInterrupt:
if verbose:
sys.stdout.write(' INTERRUPTED\n')
sys.stdout.flush()
#Writing trajectories
if self.fn_traj is not None:
with open(self.fn_traj,'w') as f:
cPickle.dump(trajectories, f)
#Plotting/writing output
for ic in self.system.ics[icname]:
if ic.name in trajectories.keys():
name = ic.name.replace('/', '-')
self.pert_theory.plot(ic, trajectories[ic.name], 'energies-'+name+'.pdf')
self.pert_theory.write(trajectories[ic.name], 'trajectory-'+name+'.xyz')
#Logging
if verbose:
print ''
print '\n'+'~'*120+'\n'
print 'Time: ' + datetime.datetime.now().isoformat().replace('T', ' ') + '\n'
print footer
