| 6 |  | * redistribute this software in source and binary code form, provided | 
| 7 |  | * that the following conditions are met: | 
| 8 |  | * | 
| 9 | < | * 1. Acknowledgement of the program authors must be made in any | 
| 10 | < | *    publication of scientific results based in part on use of the | 
| 11 | < | *    program.  An acceptable form of acknowledgement is citation of | 
| 12 | < | *    the article in which the program was described (Matthew | 
| 13 | < | *    A. Meineke, Charles F. Vardeman II, Teng Lin, Christopher | 
| 14 | < | *    J. Fennell and J. Daniel Gezelter, "OOPSE: An Object-Oriented | 
| 15 | < | *    Parallel Simulation Engine for Molecular Dynamics," | 
| 16 | < | *    J. Comput. Chem. 26, pp. 252-271 (2005)) | 
| 17 | < | * | 
| 18 | < | * 2. Redistributions of source code must retain the above copyright | 
| 9 | > | * 1. Redistributions of source code must retain the above copyright | 
| 10 |  | *    notice, this list of conditions and the following disclaimer. | 
| 11 |  | * | 
| 12 | < | * 3. Redistributions in binary form must reproduce the above copyright | 
| 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. | 
| 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, 24107 (2008). | 
| 39 | + | * [4]  Vardeman & Gezelter, in progress (2009). | 
| 40 |  | */ | 
| 41 |  |  | 
| 42 |  | #include "primitives/Inversion.hpp" | 
| 43 |  |  | 
| 44 | < | namespace oopse { | 
| 44 | > | namespace OpenMD { | 
| 45 |  |  | 
| 46 |  | Inversion::Inversion(Atom *atom1, Atom *atom2, Atom *atom3, | 
| 47 |  | Atom *atom4, InversionType *it) : | 
| 50 |  |  | 
| 51 |  | void Inversion::calcForce(RealType& angle) { | 
| 52 |  |  | 
| 53 | < | // In OOPSE's version of an inversion, the central atom | 
| 53 | > | // In OpenMD's version of an inversion, the central atom | 
| 54 |  | // comes first.  However, to get the planarity in a typical cosine | 
| 55 |  | // version of this potential (i.e. Amber-style), the central atom | 
| 56 |  | // is treated as atom *3* in a standard torsion form: | 
| 60 |  | Vector3d pos3 = atom1_->getPos(); | 
| 61 |  | Vector3d pos4 = atom4_->getPos(); | 
| 62 |  |  | 
| 63 | – | /*std::ofstream myfile; | 
| 64 | – | myfile.open("Inversion", std::ios::app); | 
| 65 | – | myfile << atom1_->getType() << " - atom1; " | 
| 66 | – | << atom2_->getType() << " - atom2; " | 
| 67 | – | << atom3_->getType() << " - atom3; " | 
| 68 | – | << atom4_->getType() << " - atom4; " | 
| 69 | – | << std::endl; | 
| 70 | – | */ | 
| 63 |  | Vector3d r31 = pos1 - pos3; | 
| 64 |  | Vector3d r23 = pos3 - pos2; | 
| 65 |  | Vector3d r43 = pos3 - pos4; | 
| 78 |  |  | 
| 79 |  | //  Calculate the sin and cos | 
| 80 |  | RealType cos_phi = dot(A, B) ; | 
| 81 | < | if (cos_phi > 1.0) {cos_phi = 1.0; std::cout << "!!!! cos_phi is bigger than 1.0" | 
| 82 | < | << std::endl;} | 
| 91 | < | if (cos_phi < -1.0) {cos_phi = -1.0; std::cout << "!!!! cos_phi is less than -1.0" | 
| 92 | < | << std::endl;} | 
| 93 | < | //std::cout << "We actually use this inversion!!!!" << std::endl; | 
| 81 | > | if (cos_phi > 1.0) cos_phi = 1.0; | 
| 82 | > | if (cos_phi < -1.0) cos_phi = -1.0; | 
| 83 |  |  | 
| 84 |  | RealType dVdcosPhi; | 
| 96 | – | //cos_phi = 2.0*cos_phi*cos_phi - 1.0; | 
| 85 |  | inversionType_->calcForce(cos_phi, potential_, dVdcosPhi); | 
| 86 |  | Vector3d f1 ; | 
| 87 |  | Vector3d f2 ; | 
| 94 |  | f2 = dVdcosPhi * ( cross(r23, dcosdB) - cross(r31, dcosdA)); | 
| 95 |  | f3 = dVdcosPhi * cross(dcosdB, r43); | 
| 96 |  |  | 
| 97 | < | // In OOPSE's version of an improper torsion, the central atom | 
| 97 | > | // In OpenMD's version of an improper torsion, the central atom | 
| 98 |  | // comes first.  However, to get the planarity in a typical cosine | 
| 99 |  | // version of this potential (i.e. Amber-style), the central atom | 
| 100 |  | // is treated as atom *3* in a standard torsion form: | 
| 101 |  |  | 
| 102 |  | //  AMBER:   I - J - K - L   (e.g. K is sp2 hybridized carbon) | 
| 103 | < | //  OOPSE:   I - (J - K - L)  (e.g. I is sp2 hybridized carbon) | 
| 103 | > | //  OpenMD:  I - (J - K - L)  (e.g. I is sp2 hybridized carbon) | 
| 104 |  |  | 
| 105 |  | // Confusing enough?  Good. | 
| 106 |  |  | 
| 109 |  | atom4_->addFrc(-f2); | 
| 110 |  | atom3_->addFrc(-f3); | 
| 111 |  |  | 
| 112 | + | atom1_->addParticlePot(potential_); | 
| 113 | + | atom2_->addParticlePot(potential_); | 
| 114 | + | atom3_->addParticlePot(potential_); | 
| 115 | + | atom4_->addParticlePot(potential_); | 
| 116 | + |  | 
| 117 |  | angle = acos(cos_phi) /M_PI * 180.0; | 
| 118 |  | } | 
| 119 |  |  |