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 |
< |
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 |
|
|