# | Line 6 | Line 6 | |
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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. | |
# | Line 37 | Line 28 | |
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) : | |
# | Line 50 | Line 50 | namespace oopse { | |
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: | |
# | Line 60 | Line 60 | namespace oopse { | |
60 | Vector3d pos3 = atom1_->getPos(); | |
61 | Vector3d pos4 = atom4_->getPos(); | |
62 | ||
63 | < | Vector3d r21 = pos1 - pos2; |
64 | < | Vector3d r32 = pos2 - pos3; |
63 | > | Vector3d r31 = pos1 - pos3; |
64 | > | Vector3d r23 = pos3 - pos2; |
65 | Vector3d r43 = pos3 - pos4; | |
66 | ||
67 | // Calculate the cross products and distances | |
68 | < | Vector3d A = cross(r21, r32); |
68 | > | Vector3d A = cross(r31, r43); |
69 | RealType rA = A.length(); | |
70 | < | Vector3d B = cross(r32, r43); |
70 | > | Vector3d B = cross(r43, r23); |
71 | RealType rB = B.length(); | |
72 | < | Vector3d C = cross(r32, A); |
73 | < | RealType rC = C.length(); |
72 | > | //Vector3d C = cross(r23, A); |
73 | > | //RealType rC = C.length(); |
74 | ||
75 | A.normalize(); | |
76 | B.normalize(); | |
77 | < | C.normalize(); |
77 | > | //C.normalize(); |
78 | ||
79 | // Calculate the sin and cos | |
80 | RealType cos_phi = dot(A, B) ; | |
81 | if (cos_phi > 1.0) cos_phi = 1.0; | |
82 | < | if (cos_phi < -1.0) cos_phi = -1.0; |
82 | > | if (cos_phi < -1.0) cos_phi = -1.0; |
83 | ||
84 | RealType dVdcosPhi; | |
85 | inversionType_->calcForce(cos_phi, potential_, dVdcosPhi); | |
86 | < | Vector3d f1; |
87 | < | Vector3d f2; |
88 | < | Vector3d f3; |
86 | > | Vector3d f1 ; |
87 | > | Vector3d f2 ; |
88 | > | Vector3d f3 ; |
89 | ||
90 | Vector3d dcosdA = (cos_phi * A - B) /rA; | |
91 | Vector3d dcosdB = (cos_phi * B - A) /rB; | |
92 | ||
93 | < | f1 = dVdcosPhi * cross(r32, dcosdA); |
94 | < | f2 = dVdcosPhi * ( cross(r43, dcosdB) - cross(r21, dcosdA)); |
95 | < | f3 = dVdcosPhi * cross(dcosdB, r32); |
93 | > | f1 = dVdcosPhi * cross(r43, dcosdA); |
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 | ||
107 | < | atom3_->addFrc(f1); |
108 | < | atom1_->addFrc(f2 - f1); |
109 | < | atom2_->addFrc(f3 - f2); |
110 | < | atom4_->addFrc(-f3); |
107 | > | atom2_->addFrc(f1); |
108 | > | atom1_->addFrc(f2 - f1 + f3); |
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 |
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