| 1 | /* | 
| 2 | * Copyright (c) 2005 The University of Notre Dame. All Rights Reserved. | 
| 3 | * | 
| 4 | * The University of Notre Dame grants you ("Licensee") a | 
| 5 | * non-exclusive, royalty free, license to use, modify and | 
| 6 | * redistribute this software in source and binary code form, provided | 
| 7 | * that the following conditions are met: | 
| 8 | * | 
| 9 | * 1. Redistributions of source code must retain the above copyright | 
| 10 | *    notice, this list of conditions and the following disclaimer. | 
| 11 | * | 
| 12 | * 2. Redistributions in binary form must reproduce the above copyright | 
| 13 | *    notice, this list of conditions and the following disclaimer in the | 
| 14 | *    documentation and/or other materials provided with the | 
| 15 | *    distribution. | 
| 16 | * | 
| 17 | * This software is provided "AS IS," without a warranty of any | 
| 18 | * kind. All express or implied conditions, representations and | 
| 19 | * warranties, including any implied warranty of merchantability, | 
| 20 | * fitness for a particular purpose or non-infringement, are hereby | 
| 21 | * excluded.  The University of Notre Dame and its licensors shall not | 
| 22 | * be liable for any damages suffered by licensee as a result of | 
| 23 | * using, modifying or distributing the software or its | 
| 24 | * derivatives. In no event will the University of Notre Dame or its | 
| 25 | * licensors be liable for any lost revenue, profit or data, or for | 
| 26 | * direct, indirect, special, consequential, incidental or punitive | 
| 27 | * damages, however caused and regardless of the theory of liability, | 
| 28 | * arising out of the use of or inability to use software, even if the | 
| 29 | * University of Notre Dame has been advised of the possibility of | 
| 30 | * such damages. | 
| 31 | * | 
| 32 | * SUPPORT OPEN SCIENCE!  If you use OpenMD or its source code in your | 
| 33 | * research, please cite the appropriate papers when you publish your | 
| 34 | * work.  Good starting points are: | 
| 35 | * | 
| 36 | * [1]  Meineke, et al., J. Comp. Chem. 26, 252-271 (2005). | 
| 37 | * [2]  Fennell & Gezelter, J. Chem. Phys. 124, 234104 (2006). | 
| 38 | * [3]  Sun, Lin & Gezelter, J. Chem. Phys. 128, 234107 (2008). | 
| 39 | * [4]  Kuang & Gezelter,  J. Chem. Phys. 133, 164101 (2010). | 
| 40 | * [5]  Vardeman, Stocker & Gezelter, J. Chem. Theory Comput. 7, 834 (2011). | 
| 41 | */ | 
| 42 |  | 
| 43 | #include "config.h" | 
| 44 | #include <cmath> | 
| 45 |  | 
| 46 | #include "primitives/Inversion.hpp" | 
| 47 |  | 
| 48 | namespace OpenMD { | 
| 49 |  | 
| 50 | Inversion::Inversion(Atom *atom1, Atom *atom2, Atom *atom3, | 
| 51 | Atom *atom4, InversionType *it) : | 
| 52 | ShortRangeInteraction(), inversionType_(it) { | 
| 53 |  | 
| 54 | atoms_.resize(4); | 
| 55 | atoms_[0] = atom1; | 
| 56 | atoms_[1] = atom2; | 
| 57 | atoms_[2] = atom3; | 
| 58 | atoms_[3] = atom4; | 
| 59 |  | 
| 60 | inversionKey_ = inversionType_->getKey(); | 
| 61 | } | 
| 62 |  | 
| 63 | void Inversion::calcForce(RealType& angle, bool doParticlePot) { | 
| 64 |  | 
| 65 | // In OpenMD's version of an inversion, the central atom | 
| 66 | // comes first.  However, to get the planarity in a typical cosine | 
| 67 | // version of this potential (i.e. Amber-style), the central atom | 
| 68 | // is treated as atom *3* in a standard torsion form: | 
| 69 |  | 
| 70 | Vector3d pos1 = atoms_[1]->getPos(); | 
| 71 | Vector3d pos2 = atoms_[2]->getPos(); | 
| 72 | Vector3d pos3 = atoms_[0]->getPos(); | 
| 73 | Vector3d pos4 = atoms_[3]->getPos(); | 
| 74 |  | 
| 75 | Vector3d r31 = pos1 - pos3; | 
| 76 | Vector3d r23 = pos3 - pos2; | 
| 77 | Vector3d r43 = pos3 - pos4; | 
| 78 |  | 
| 79 | //  Calculate the cross products and distances | 
| 80 | Vector3d A = cross(r31, r43); | 
| 81 | RealType rA = A.length(); | 
| 82 | Vector3d B = cross(r43, r23); | 
| 83 | RealType rB = B.length(); | 
| 84 | //Vector3d C = cross(r23, A); | 
| 85 | //RealType rC = C.length(); | 
| 86 |  | 
| 87 | A.normalize(); | 
| 88 | B.normalize(); | 
| 89 | //C.normalize(); | 
| 90 |  | 
| 91 | //  Calculate the sin and cos | 
| 92 | RealType cos_phi = dot(A, B) ; | 
| 93 | if (cos_phi > 1.0) cos_phi = 1.0; | 
| 94 | if (cos_phi < -1.0) cos_phi = -1.0; | 
| 95 |  | 
| 96 | RealType dVdcosPhi; | 
| 97 | switch (inversionKey_) { | 
| 98 | case itCosAngle: | 
| 99 | inversionType_->calcForce(cos_phi, potential_, dVdcosPhi); | 
| 100 | break; | 
| 101 | case itAngle: | 
| 102 | RealType phi = acos(cos_phi); | 
| 103 | RealType dVdPhi; | 
| 104 | inversionType_->calcForce(phi, potential_, dVdPhi); | 
| 105 | RealType sin_phi = sqrt(1.0 - cos_phi * cos_phi); | 
| 106 | if (fabs(sin_phi) < 1.0E-6) { | 
| 107 | sin_phi = 1.0E-6; | 
| 108 | } | 
| 109 | dVdcosPhi = dVdPhi / sin_phi; | 
| 110 | break; | 
| 111 | } | 
| 112 |  | 
| 113 | Vector3d f1 ; | 
| 114 | Vector3d f2 ; | 
| 115 | Vector3d f3 ; | 
| 116 |  | 
| 117 | Vector3d dcosdA = (cos_phi * A - B) /rA; | 
| 118 | Vector3d dcosdB = (cos_phi * B - A) /rB; | 
| 119 |  | 
| 120 | f1 = dVdcosPhi * cross(r43, dcosdA); | 
| 121 | f2 = dVdcosPhi * ( cross(r23, dcosdB) - cross(r31, dcosdA)); | 
| 122 | f3 = dVdcosPhi * cross(dcosdB, r43); | 
| 123 |  | 
| 124 | // In OpenMD's version of an improper torsion, the central atom | 
| 125 | // comes first.  However, to get the planarity in a typical cosine | 
| 126 | // version of this potential (i.e. Amber-style), the central atom | 
| 127 | // is treated as atom *3* in a standard torsion form: | 
| 128 |  | 
| 129 | //  AMBER:   I - J - K - L   (e.g. K is sp2 hybridized carbon) | 
| 130 | //  OpenMD:  I - (J - K - L)  (e.g. I is sp2 hybridized carbon) | 
| 131 |  | 
| 132 | // Confusing enough?  Good. | 
| 133 |  | 
| 134 | atoms_[1]->addFrc(f1); | 
| 135 | atoms_[0]->addFrc(f2 - f1 + f3); | 
| 136 | atoms_[3]->addFrc(-f2); | 
| 137 | atoms_[2]->addFrc(-f3); | 
| 138 |  | 
| 139 | if (doParticlePot) { | 
| 140 | atoms_[0]->addParticlePot(potential_); | 
| 141 | atoms_[1]->addParticlePot(potential_); | 
| 142 | atoms_[2]->addParticlePot(potential_); | 
| 143 | atoms_[3]->addParticlePot(potential_); | 
| 144 | } | 
| 145 |  | 
| 146 | angle = acos(cos_phi) /M_PI * 180.0; | 
| 147 | } | 
| 148 |  | 
| 149 | } |