| [075357] | 1 | import pyMoleCuilder as mol | 
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|  | 2 | import sys, os, math | 
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|  | 3 | try: | 
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|  | 4 | import numpy | 
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|  | 5 | numpy_present = True | 
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|  | 6 | except ImportError: | 
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|  | 7 | numpy_present = False | 
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|  | 8 |  | 
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|  | 9 | if len(sys.argv) < 5: | 
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| [d083cc] | 10 | print('Usage: '+sys.argv[0]+' <input> <path> <steps> <no_atoms> <use bondgraph>') | 
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| [075357] | 11 | sys.exit(1) | 
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|  | 12 |  | 
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|  | 13 | steps=int(sys.argv[3]) | 
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|  | 14 | equilibrium_distance=1.6 | 
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|  | 15 | no_atoms=int(sys.argv[4]) | 
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|  | 16 | inputfile=sys.argv[1] | 
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|  | 17 | forcespath=sys.argv[2] | 
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|  | 18 | forcesfile="ising.forces" | 
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|  | 19 | use_bondgraph=sys.argv[5] | 
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|  | 20 |  | 
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|  | 21 | # creating input file | 
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|  | 22 | atomstart=7.6-1.6*math.floor(no_atoms/2) | 
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| [d083cc] | 23 | print("Creating "+inputfile) | 
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| [075357] | 24 | with open(inputfile, 'w') as f: | 
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|  | 25 | f.write("# ATOMDATA\ttype\tId\tx=3\tu=3\tF=3\tneighbors=4\n") | 
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|  | 26 | f.write("# Box\t20\t0\t0\t0\t20\t0\t0\t0\t20\n") | 
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|  | 27 | for i in range(1, no_atoms+1): | 
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|  | 28 | atompos=atomstart+1.6*float(i) | 
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|  | 29 | if i==math.floor(no_atoms/2+1): | 
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|  | 30 | atompos=atompos-.5 | 
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|  | 31 | if i==1: | 
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|  | 32 | f.write("C\t%d\t%lg\t10\t10\t0\t0\t0\t0\t0\t0\t%d\t0\t0\t0\n" % (i, atompos, i+1)); | 
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|  | 33 | elif i==no_atoms: | 
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|  | 34 | f.write("C\t%d\t%lg\t10\t10\t0\t0\t0\t0\t0\t0\t%d\t0\t0\t0\n" % (i, atompos, i-1)); | 
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|  | 35 | else: | 
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|  | 36 | f.write("C\t%d\t%lg\t10\t10\t0\t0\t0\t0\t0\t0\t%d\t%d\t0\t0\n" % (i, atompos, i-1, i+1)); | 
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|  | 37 |  | 
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| [d083cc] | 38 | print("Parsing from "+inputfile) | 
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| [075357] | 39 | mol.WorldInput(inputfile) | 
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|  | 40 | mol.SelectionAllAtoms() | 
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|  | 41 | mol.CommandVerbose("4") | 
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|  | 42 |  | 
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|  | 43 | # calculate damping factor from finite geometric series | 
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|  | 44 | # s_n/a = \sum^{n-1}_{k=0} r^k = (1-r^n)/(1-r) -> s_(n+1)/a -1 = \sum^{n}_{k=1} r^k = (1-r^(n+1))/(1-r) - 1 | 
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|  | 45 | # \sum^{n}_{k=1} r^k := 1 and 1 = (1-r^(n+1))/(1-r) - 1 -> 2*(1-r) = 1 - r^(n+1) -> 1 - 2*r + r^(n+1) = 0 | 
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|  | 46 | # find root: p[0] is coefficient of monomial with highest power | 
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|  | 47 | if numpy_present: | 
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|  | 48 | p=[0.] * (no_atoms+1) | 
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|  | 49 | p[0]=1. | 
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|  | 50 | p[no_atoms-1]=-2. | 
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|  | 51 | p[no_atoms]=1. | 
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|  | 52 | zeros=numpy.roots(p) | 
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|  | 53 | print("Roots of p "+str(p)+" are "+str(zeros)) | 
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|  | 54 | damping=numpy.real(zeros[-1]) | 
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| [d083cc] | 55 | print("Using damping factor of "+str(damping)) | 
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| [075357] | 56 | else: | 
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|  | 57 | if no_atoms == 2: | 
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|  | 58 | damping=0.5 | 
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|  | 59 | elif no_atoms == 5: | 
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|  | 60 | damping=0.5436890126920764 | 
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|  | 61 |  | 
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|  | 62 | for i in range(0, steps): | 
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|  | 63 | # TODO: Python interface should have something to iterate over selected atoms | 
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|  | 64 | # and molecules and get information on their internal status | 
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|  | 65 |  | 
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|  | 66 | # read current atomic positions | 
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|  | 67 | outputfile=forcespath+'/'+forcesfile+'.xyz' | 
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|  | 68 | try: | 
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|  | 69 | os.remove(outputfile) | 
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|  | 70 | except: OSError | 
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|  | 71 | # | 
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|  | 72 | mol.WorldOutputAs(outputfile) | 
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|  | 73 | mol.wait() | 
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|  | 74 | distances=[] | 
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|  | 75 | coords=[0.,0.,0.] | 
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|  | 76 | try: | 
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|  | 77 | skiplines=2+i*(1+1+no_atoms+1) # no_atoms, comment, no_atoms atoms, empty line | 
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|  | 78 | with open(outputfile) as f: | 
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|  | 79 | for line in f: | 
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|  | 80 | if skiplines != 0: | 
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|  | 81 | skiplines=skiplines-1 | 
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|  | 82 | continue | 
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|  | 83 | line=line.replace('\t',' ') | 
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| [d083cc] | 84 | print("LINE: "+line) | 
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| [075357] | 85 | [elementtype, X, Y, Z] = line.split(' ', 4) | 
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|  | 86 | if coords!=[0.,0.,0.]: | 
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|  | 87 | distances.append(math.sqrt((coords[0]-float(X))**2+(coords[1]-float(Y))**2+(coords[2]-float(Z))**2)) | 
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|  | 88 | coords=[float(X),float(Y),float(Z)] | 
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|  | 89 | except IOError: | 
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| [d083cc] | 90 | print('Warning: '+outputfile+' not readable.') | 
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| [075357] | 91 | sys.exit(1) | 
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|  | 92 |  | 
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|  | 93 | assert(len(distances)==no_atoms-1) | 
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|  | 94 |  | 
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|  | 95 | # | 
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|  | 96 | # generate Ising model forces and store in file | 
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|  | 97 | # | 
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|  | 98 | # i.e. we have spring forces between neighboring atoms depending on their distance | 
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|  | 99 | forces=[] | 
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|  | 100 | for d in distances: | 
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|  | 101 | forces.append( d - equilibrium_distance ); | 
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|  | 102 |  | 
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|  | 103 | # generate new forces file | 
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|  | 104 |  | 
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|  | 105 | with open(forcespath+'/'+forcesfile, 'w') as f: | 
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|  | 106 | f.write('# atom\tf_x\tf_y\tf_z\n') | 
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|  | 107 | for i in range(len(distances)+1): | 
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|  | 108 | force=0 | 
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|  | 109 | if i!=0: | 
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|  | 110 | force=force-forces[i-1] | 
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|  | 111 | if (i != len(distances)): | 
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|  | 112 | force=force+forces[i] | 
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|  | 113 | f.write("%d\t%f\t0.\t0.\n" % (i+1, force)) | 
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|  | 114 |  | 
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|  | 115 | mol.WorldStepWorldTime("1") | 
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|  | 116 | mol.MoleculeForceAnnealing(forcespath+'/'+forcesfile, ".1", "%d" % (steps), "%d" % (no_atoms-1), "%lg" % (damping), use_bondgraph) | 
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|  | 117 | mol.wait() | 
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|  | 118 |  | 
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|  | 119 | sys.exit(0) | 
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