예제 #1
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    def test_transform_gradient(self):
        tai, atom_indices = self.make_atom_indices_python_topology()
        tnorm = self.make_normal_python_topology()
        
        coords = self.get_random_rbcoords()

        aai = tai.to_atomistic(coords.copy())
        anorm = tnorm.to_atomistic(coords.copy())

        
        lj = LJ()
#        atomistic_coords = np.random.uniform(-1, 1, 3*len(atom_indices))
#        e, atomistic_grad = lj.getEnergyGradient(atomistic_coords)
        
        e1, gai = lj.getEnergyGradient(aai.ravel())
        e2, gnorm = lj.getEnergyGradient(anorm.ravel())
        self.assertAlmostEqual(e1, e2)
        assert_arrays_almost_equal(self, gai.reshape(-1,3)[atom_indices], gnorm.reshape(-1,3))

        
        
        rb_gai = tai.transform_gradient(coords.copy(), gai)
        rb_gnorm = tnorm.transform_gradient(coords.copy(), gnorm)
        
        assert_arrays_almost_equal(self, rb_gai, rb_gnorm)
예제 #2
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파일: frozen_atoms.py 프로젝트: js850/pele
def test2():
    import numpy as np
    from pele.potentials import LJ
    from pele.utils.frozen_atoms import FrozenPotWrapper
    from pele.optimize import mylbfgs

    natoms = 4
    pot = LJ()

    reference_coords = np.random.uniform(-1, 1, [3 * natoms])
    print reference_coords

    # freeze the first two atoms (6 degrees of freedom)
    frozen_dof = range(6)

    fpot = FrozenPotWrapper(pot, reference_coords, frozen_dof)

    reduced_coords = fpot.coords_converter.get_reduced_coords(reference_coords)

    print "the energy in the full representation:"
    print pot.getEnergy(reference_coords)
    print "is the same as the energy in the reduced representation:"
    print fpot.getEnergy(reduced_coords)

    ret = mylbfgs(reduced_coords, fpot)
    print "after a minimization the energy is ", ret.energy, "and the rms gradient is", ret.rms
    print "the coordinates of the frozen degrees of freedom are unchanged"
    print "starting coords:", reference_coords
    print "minimized coords:", fpot.coords_converter.get_full_coords(ret.coords)
예제 #3
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파일: ATLJ.py 프로젝트: Mahdisadjadi/pele
class ATLJ(BasePotential):
    """
    Lennard Jones + three body Axilrod-Teller term
    
    V = sum_ij VLJ_ij   +  sum_ijk  Z * (1 + 3*cos(t1)*cos(t2)*cos(t3)) / (rij * rjk * rik)**3 )
    
    where t1, t2, t3 are the internal angles of the triangle ijk
    
    Z > 0 stabilizes linear vs. triangular geometries 
    """

    def __init__(self, eps=1.0, sig=1.0, Z=1.):
        """ simple lennard jones potential"""
        self.sig = sig
        self.eps = eps
        self.Z = Z
        self.lj = LJ(self.sig, self.eps)

    def getEnergySlow(self, coords):
        Elj = self.lj.getEnergy(coords)

        natoms = coords.size / 3
        X = np.reshape(coords, [natoms, 3])
        Z = self.Z
        energy = 0.
        for i in range(natoms):
            for j in range(i):
                for k in range(j):
                    drij = X[i, :] - X[j, :]
                    drik = X[i, :] - X[k, :]
                    drjk = X[j, :] - X[k, :]
                    rij = np.linalg.norm(drij)
                    rik = np.linalg.norm(drik)
                    rjk = np.linalg.norm(drjk)
                    energy += (Z * (1. + 3. *
                                    np.dot(drij, -drjk) *
                                    np.dot(-drij, -drik) *
                                    np.dot(drik, drjk) / (rij * rik * rjk) ** 2)
                               / (rij * rik * rjk) ** 3 )
        energy += Elj
        return energy

    def getEnergyFortran(self, coords):
        garbage, e = ATfort.axt(coords, False, self.Z)
        Elj = self.lj.getEnergy(coords)
        return e + Elj

    def getEnergyGradientFortran(self, coords):
        grad, e = ATfort.axt(coords, True, self.Z)

        elj, gradlj = self.lj.getEnergyGradient(coords)
        return e + elj, grad + gradlj

    def getEnergy(self, coords):
        return self.getEnergyFortran(coords)

    def getEnergyGradient(self, coords):
        return self.getEnergyGradientFortran(coords)
예제 #4
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 def test_to_atomistic2(self):
     x0 = np.array(list(range(self.nrigid * 6)), dtype=float)
     x2 = x0.reshape([-1,3])
     for p in x2[self.nrigid:,:]:
         p /= np.linalg.norm(p)
     atomistic = self.topology.to_atomistic(x0).flatten()
     
     from pele.potentials import LJ
     lj = LJ()
     e, g = lj.getEnergyGradient(atomistic.reshape(-1))
     grb = self.topology.transform_gradient(x0, g)
     rbpot = RBPotentialWrapper(self.topology, lj)
     print(rbpot.getEnergy(x0))
예제 #5
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class TestLJ_CPP(unittest.TestCase):
    def setUp(self):
        self.natoms = 18
        self.pot = _lj.LJ()
        
        self.pot_comp = LJ()
        x = np.random.uniform(-1,1, 3*self.natoms)
        ret = mylbfgs(x, self.pot_comp, tol=10.)
        self.x = ret.coords
        
    
    def test(self):
        eonly = self.pot.getEnergy(self.x)
        e, g = self.pot.getEnergyGradient(self.x)
        self.assertAlmostEqual(e, eonly, delta=1e-6)
        et, gt = self.pot_comp.getEnergyGradient(self.x)
        self.assertAlmostEqual(e, et, delta=1e-6)
        self.assertLess(np.max(np.abs(g - gt)), 1e-6)

    def test_numerical_gradient(self):
        e, g = self.pot.getEnergyGradient(self.x)
        gnum = self.pot.NumericalDerivative(self.x)
        gnum_old = self.pot_comp.NumericalDerivative(self.x)
        self.assertLess(np.max(np.abs(gnum_old - gnum)), 1e-6)        
        self.assertLess(np.max(np.abs(g - gnum)), 1e-6)

    def test_numerical_hessian(self):
#        e, g = self.pot.getEnergyGradient(self.x)
        h = self.pot.NumericalHessian(self.x)
        h_old = self.pot_comp.NumericalHessian(self.x)
        self.assertLess(np.max(np.abs(h_old - h)), 1e-6)        
예제 #6
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 def setUp(self):
     self.natoms = 18
     self.pot = _lj.LJ()
     
     self.pot_comp = LJ()
     x = np.random.uniform(-1,1, 3*self.natoms)
     ret = mylbfgs(x, self.pot_comp, tol=10.)
     self.x = ret.coords
    def setUp(self):
        self.natoms = 18
        self.ilist = np.array([(i,j) for i in xrange(self.natoms) for j in xrange(i+1,self.natoms)]).reshape(-1)
        assert self.ilist.size == self.natoms*(self.natoms-1)
#        print self.ilist
        self.pot = _lj.LJInteractionList(self.ilist) 
        
        self.pot_comp = LJ()
        x = np.random.uniform(-1,1, 3*self.natoms)
        ret = mylbfgs(x, self.pot_comp, tol=10.)
        self.x = ret.coords
예제 #8
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def main():
    natoms = 4
    pot = LJ()

    reference_coords = np.random.uniform(-1, 1, [3 * natoms])
    print reference_coords

    # freeze the first two atoms (6 degrees of freedom)
    frozen_dof = range(6)

    fpot = FrozenPotentialWrapper(pot, reference_coords, frozen_dof)

    reduced_coords = fpot.get_reduced_coords(reference_coords)

    print "the energy in the full representation:"
    print pot.getEnergy(reference_coords)
    print "is the same as the energy in the reduced representation:"
    print fpot.getEnergy(reduced_coords)

    ret = mylbfgs(reduced_coords, fpot)
    print "after a minimization the energy is ", ret.energy, "and the rms gradient is", ret.rms
    print "the coordinates of the frozen degrees of freedom are unchanged"
    print "starting coords:", reference_coords
    print "minimized coords:", fpot.get_full_coords(ret.coords)
예제 #9
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파일: test_otp.py 프로젝트: jdf43/pele
 def test_to_atomistic2(self):
     x0 = np.array(range(self.nrigid * 6), dtype=float);
     x2 = x0.reshape([-1,3])
     for p in x2[self.nrigid:,:]:
         p /= np.linalg.norm(p);
     print x0
     print "range to atomistic"
     print x0
     atomistic = self.topology.to_atomistic(x0).flatten()
     print atomistic
     print atomistic.size
     print atomistic[14]
     print atomistic[23]
     
     from pele.potentials import LJ
     lj = LJ()
     e, g = lj.getEnergyGradient(atomistic.reshape(-1))
     grb = self.topology.transform_gradient(x0, g);
     print "transformed gradient"
     print grb
     
     print "rbpotential"
     rbpot = RBPotentialWrapper(self.topology, lj);
     print rbpot.getEnergy(x0);
예제 #10
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class TestLJ_CPP_Ilist(unittest.TestCase):
    def setUp(self):
        self.natoms = 18
        self.ilist = np.array([(i,j) for i in xrange(self.natoms) for j in xrange(i+1,self.natoms)]).reshape(-1)
        assert self.ilist.size == self.natoms*(self.natoms-1)
#        print self.ilist
        self.pot = _lj.LJInteractionList(self.ilist) 
        
        self.pot_comp = LJ()
        x = np.random.uniform(-1,1, 3*self.natoms)
        ret = mylbfgs(x, self.pot_comp, tol=10.)
        self.x = ret.coords
        
    
    def test(self):
        eonly = self.pot.getEnergy(self.x)
        e, g = self.pot.getEnergyGradient(self.x)
        self.assertAlmostEqual(e, eonly, delta=1e-6)
        et, gt = self.pot_comp.getEnergyGradient(self.x)
        self.assertAlmostEqual(e, et, delta=1e-6)
        self.assertLess(np.max(np.abs(g - gt)), 1e-6)
예제 #11
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파일: ATLJ.py 프로젝트: Mahdisadjadi/pele
 def __init__(self, eps=1.0, sig=1.0, Z=1.):
     """ simple lennard jones potential"""
     self.sig = sig
     self.eps = eps
     self.Z = Z
     self.lj = LJ(self.sig, self.eps)
예제 #12
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 def get_potential(self):
     return LJ(self.natoms)
예제 #13
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파일: otp.py 프로젝트: js850/pele
 def getEnergyGradient(self, coords):
     atom_coords = self.aatopology.to_atomistic(coords)
     e, atom_grad = LJ.getEnergyGradient(self, atom_coords.flatten())
     grad = self.aatopology.transform_gradient(coords, atom_grad)
     return e, grad
예제 #14
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In the above we used three imports.  We used the `numpy` library to construct a random
one dimensional array.  We used the Lennard-Jones potential :class:`.LJ`, and we used the minimization
routine :func:`.lbfgs_py` which is just a wrapper for the class :class:`.LBFGS`.

The return value is an optimization result, which is just a container (:class:`.Result`) that stores
the final energy, final coordinates, the number of function calls, etc.

If we want to then save the minimized coordinates in an xyz file we can use the function :func:`.write_xyz`
::
    from pele.utils.xyz import write_xyz
    with open("out.xyz", "w") as fout:
        title = "energy = " + str(result.energy)
        write_xyz(fout, result.coords, title=title)

"""
import numpy as np
from pele.potentials import LJ
from pele.optimize import lbfgs_py

natoms = 5
x = np.random.uniform(-2, 2, natoms * 3)
pot = LJ()
result = lbfgs_py(x, pot)
print result

from pele.utils.xyz import write_xyz
with open("out.xyz", "w") as fout:
    title = "energy = " + str(result.energy)
    write_xyz(fout, result.coords, title=title)
예제 #15
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파일: ATLJ.py 프로젝트: borislavujo/pele
class ATLJ(BasePotential):
    """
    Lennard Jones + three body Axilrod-Teller term
    
    V = sum_ij VLJ_ij   +  sum_ijk  Z * (1 + 3*cos(t1)*cos(t2)*cos(t3)) / (rij * rjk * rik)**3 )
    
    where t1, t2, t3 are the internal angles of the triangle ijk
    
    Z > 0 stabilizes linear vs. triangular geometries 
    """
    def __init__(self, eps=1.0, sig=1.0, Z=1.):
        """ simple lennard jones potential"""
        self.sig = sig
        self.eps = eps
        self.Z = Z
        self.lj = LJ(self.sig, self.eps)

    
#    def getEnergyWeave(self, coords):
#        """
#        use weave inline
#        """
#        Elj = self.lj.getEnergy(coords)
#        
#        natoms = coords.size/3
#        coords = np.reshape(coords, [natoms,3])
#        energy=0.
#        Z = self.Z
#        #support_code
#        code = """
#        double drij[3];
#        double drik[3];
#        double drjk[3];
#        energy = 0.;
#        for (int i=0; i < natoms; ++i){
#            for (int j=0; j<i; ++j){
#                for (int k=0; k<j; ++k){
#                
#                    double rij = 0.;
#                    double rik = 0.;
#                    double rjk = 0.;
#        
#                    for (int d=0; d<3; ++d){
#                        drij[d] = coords(i,d) - coords(j,d);
#                        rij += drij[d]*drij[d];
#                    }
#                    for (int d=0; d<3; ++d){
#                        drjk[d] = coords(j,d) - coords(k,d);
#                        rjk += drjk[d]*drjk[d];
#                    }
#                    for (int d=0; d<3; ++d){
#                        drik[d] = coords(i,d) - coords(k,d);
#                        rik += drik[d]*drik[d];
#                    }
#                    
#                    rij = sqrt(rij);
#                    rjk = sqrt(rjk);
#                    rik = sqrt(rik);
#                    
#                    double ctijk = ( -(drij[0]*drjk[0] + drij[1]*drjk[1] + drij[2]*drjk[2]) / (rij * rjk) );
#                    double ctjki = (  (drjk[0]*drik[0] + drjk[1]*drik[1] + drjk[2]*drik[2]) / (rjk * rik) );
#                    double ctkij = (  (drik[0]*drij[0] + drik[1]*drij[1] + drik[2]*drij[2]) / (rik * rij) );
#
#                    double r3 = rij*rjk*rik;
#                    energy += Z*(1. + 3. * ctijk * ctjki * ctkij) / (r3*r3*r3);
#                }
#            }
#        }
#        return_val= energy;
#        """
#        energy = weave.inline(code, ["coords", "energy", "Z", "natoms"], type_converters=converters.blitz, verbose=2)
#        #print "fast energy", Elj, energy
#        energy += Elj
#        return energy



    def getEnergySlow(self, coords):
        Elj = self.lj.getEnergy(coords)
        
        natoms = coords.size/3
        X = np.reshape(coords, [natoms,3])
        Z = self.Z
        energy = 0.
        for i in range(natoms):
            for j in range(i):
                for k in range(j):
                    #print i, j, k
                    drij = X[i,:] - X[j,:]
                    drik = X[i,:] - X[k,:]
                    drjk = X[j,:] - X[k,:]
                    rij = np.linalg.norm( drij )
                    rik = np.linalg.norm( drik )
                    rjk = np.linalg.norm( drjk )
                    energy += Z * (1. + 3.*\
                            np.dot( drij, -drjk ) * \
                            np.dot(-drij, -drik ) * \
                            np.dot( drik,  drjk ) / (rij*rik*rjk)**2) \
                            / (rij*rik*rjk)**3
        #print "slow energy", Elj, energy
        energy += Elj
        return energy

    def getEnergyFortran(self, coords):
        #grad,potel = axt(x,gradt,zstar,[n])
        natoms = len(coords)/3
        garbage, e = ATfort.axt(coords, False, self.Z)
        
        Elj = self.lj.getEnergy(coords)
        return e + Elj

    def getEnergyGradientFortran(self, coords):
        #grad,potel = axt(x,gradt,zstar,[n])
        natoms = len(coords)/3
        grad, e = ATfort.axt(coords, True, self.Z)
        
        elj, gradlj = self.lj.getEnergyGradient(coords)
        return e + elj, grad + gradlj

    def getEnergy(self, coords):
        return self.getEnergyFortran(coords)
    
    def getEnergyGradient(self, coords):
        #return self.getEnergyGradientNumerical(coords)
        return self.getEnergyGradientFortran(coords)
예제 #16
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파일: ljcluster.py 프로젝트: spraharsh/pele
 def get_potential(self):
     return LJ()
예제 #17
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# finalize the rigid body setup
for rb in rb_sites:
    rb.finalize_setup()

# define a new rigid body system    
rbsystem = rigidbody.RBSystem()
rbsystem.add_sites(rb_sites)

print len(rbsystem.sites), len(rbsystem.indices)

rbcoords = rbsystem.coords_adapter(np.zeros(len(rbsystem.sites)*6))

for site, com in zip(rbsystem.sites, rbcoords.posRigid):
    com[:] = ref.coords[site.indices[0]] - site.atom_positions[0]
     
# for simplicity just use a lj potential here
pot = LJ(sigma=2.)
# get the flattened coordinate array
print pot.getEnergy(ref.coords.flatten())
rbpot = rigidbody.RBPotentialWrapper(rbsystem, pot)
print rbpot.getEnergy(rbcoords.coords)
e, g = rbpot.getEnergyGradient(rbcoords.coords)
g_n = rbpot.NumericalDerivative(rbcoords.coords, eps=1e-4)
cg = rbsystem.coords_adapter(g-g_n) 
print cg.posRigid
print cg.rotRigid
ret = lbfgs_py(rbcoords.coords, rbpot)
print ret.energy
xyz.write_xyz(open("quenched.xyz", "w"), rbsystem.to_atomistic(ret.coords), atomtypes=ref.atomtypes)

예제 #18
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 def get_potential(self, eps, sig, boxl=None):
     # return LJ(self.natoms, sig=sig, boxl = boxl)
     return LJ(eps, sig, boxl=boxl)
예제 #19
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import _pele
import numpy as np
import time
import sys
import _lj
import _lbfgs
from pele.optimize import mylbfgs
N = 100
natoms = [
    10, 13, 20, 30, 31, 38, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130, 140,
    150
]

print("benchmarking lennard jones potential, %d atoms, %d calls", natoms, N)
pot_old = LJ()
pot = _lj.LJ()

clbfgs = _lbfgs.LBFGS(pot)

res = open("results.txt", "w")

for na in natoms:
    t0 = time.time()
    for i in range(N):
        x = np.random.random(3 * na) - 0.5
        ret = clbfgs.run(x)

    t1 = time.time()
    for i in range(N):
        x = np.random.random(3 * na) - 0.5
예제 #20
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import _pele
import numpy as np
import time
import sys
import _lj
import _lbfgs
from pele.optimize import mylbfgs
from . import _lj_cython
import _pythonpotential

N = int(sys.argv[2])
natoms = int(sys.argv[1])

print("benchmarking lennard jones potential, %d atoms, %d calls" % (natoms, N))
pot_old = LJ()
pot = _lj.LJ()

t0 = time.time()
for i in range(N):
    x = 1. * (np.random.random(3 * natoms) - 0.5)
    clbfgs = _lbfgs.LBFGS_CPP(pot, x, tol=1e-4)
    ret = clbfgs.run()

t1 = time.time()
for i in range(N):
    x = 1. * (np.random.random(3 * natoms) - 0.5)
    ret = mylbfgs(x, pot_old, tol=1e-4)

t2 = time.time()
예제 #21
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파일: otp.py 프로젝트: js850/pele
 def getEnergy(self, coords):
     atom_coords = self.aatopology.to_atomistic(coords)
     return LJ.getEnergy(self, atom_coords.flatten())
예제 #22
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파일: ATLJ.py 프로젝트: spraharsh/pele
 def __init__(self, eps=1.0, sig=1.0, Z=1.):
     """ simple lennard jones potential"""
     self.sig = sig
     self.eps = eps
     self.Z = Z
     self.lj = LJ(self.sig, self.eps)
예제 #23
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    def setUp(self):
        from pele.potentials import LJ

        self.x0 = np.zeros(6)
        self.x0[0] = 2.
        self.pot = LJ()
예제 #24
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파일: otp.py 프로젝트: js850/pele
 def __init__(self, aatopology):
     self.aatopology = aatopology
     LJ.__init__(self)