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root/OpenMD/trunk/src/primitives/Inversion.cpp
Revision: 1890
Committed: Tue Jun 18 21:06:25 2013 UTC (11 years, 10 months ago) by gezelter
File size: 5139 byte(s)
Log Message:
Adding HarmonicInversionType for GROMOS and CHARMM style force fields.

File Contents

# User Rev Content
1 cli2 1275 /*
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 gezelter 1390 * 1. Redistributions of source code must retain the above copyright
10 cli2 1275 * notice, this list of conditions and the following disclaimer.
11     *
12 gezelter 1390 * 2. Redistributions in binary form must reproduce the above copyright
13 cli2 1275 * 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 gezelter 1390 *
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 gezelter 1879 * [3] Sun, Lin & Gezelter, J. Chem. Phys. 128, 234107 (2008).
39 gezelter 1782 * [4] Kuang & Gezelter, J. Chem. Phys. 133, 164101 (2010).
40     * [5] Vardeman, Stocker & Gezelter, J. Chem. Theory Comput. 7, 834 (2011).
41 cli2 1275 */
42    
43 gezelter 1782 #include "config.h"
44     #include <cmath>
45    
46 cli2 1275 #include "primitives/Inversion.hpp"
47    
48 gezelter 1390 namespace OpenMD {
49 cli2 1275
50     Inversion::Inversion(Atom *atom1, Atom *atom2, Atom *atom3,
51     Atom *atom4, InversionType *it) :
52     atom1_(atom1), atom2_(atom2), atom3_(atom3), atom4_(atom4),
53 gezelter 1890 inversionType_(it) {
54     inversionKey_ = inversionType_->getKey();
55     }
56 cli2 1275
57 gezelter 1782 void Inversion::calcForce(RealType& angle, bool doParticlePot) {
58 cli2 1275
59 gezelter 1390 // In OpenMD's version of an inversion, the central atom
60 cli2 1275 // comes first. However, to get the planarity in a typical cosine
61     // version of this potential (i.e. Amber-style), the central atom
62     // is treated as atom *3* in a standard torsion form:
63    
64     Vector3d pos1 = atom2_->getPos();
65 cli2 1303 Vector3d pos2 = atom3_->getPos();
66     Vector3d pos3 = atom1_->getPos();
67     Vector3d pos4 = atom4_->getPos();
68 cli2 1275
69 cli2 1303 Vector3d r31 = pos1 - pos3;
70     Vector3d r23 = pos3 - pos2;
71     Vector3d r43 = pos3 - pos4;
72 cli2 1275
73     // Calculate the cross products and distances
74 cli2 1303 Vector3d A = cross(r31, r43);
75 cli2 1275 RealType rA = A.length();
76 cli2 1303 Vector3d B = cross(r43, r23);
77 cli2 1275 RealType rB = B.length();
78 cli2 1290 //Vector3d C = cross(r23, A);
79     //RealType rC = C.length();
80 cli2 1275
81     A.normalize();
82     B.normalize();
83 cli2 1290 //C.normalize();
84 cli2 1275
85     // Calculate the sin and cos
86     RealType cos_phi = dot(A, B) ;
87 gezelter 1309 if (cos_phi > 1.0) cos_phi = 1.0;
88     if (cos_phi < -1.0) cos_phi = -1.0;
89 cli2 1275
90     RealType dVdcosPhi;
91 gezelter 1890 switch (inversionKey_) {
92     case itCosAngle:
93     inversionType_->calcForce(cos_phi, potential_, dVdcosPhi);
94     break;
95     case itAngle:
96     RealType phi = acos(cos_phi);
97     RealType dVdPhi;
98     inversionType_->calcForce(phi, potential_, dVdPhi);
99     RealType sin_phi = sqrt(1.0 - cos_phi * cos_phi);
100     if (fabs(sin_phi) < 1.0E-6) {
101     sin_phi = 1.0E-6;
102     }
103     dVdcosPhi = dVdPhi / sin_phi;
104     break;
105     }
106    
107 cli2 1290 Vector3d f1 ;
108     Vector3d f2 ;
109     Vector3d f3 ;
110 cli2 1275
111     Vector3d dcosdA = (cos_phi * A - B) /rA;
112     Vector3d dcosdB = (cos_phi * B - A) /rB;
113    
114 cli2 1303 f1 = dVdcosPhi * cross(r43, dcosdA);
115     f2 = dVdcosPhi * ( cross(r23, dcosdB) - cross(r31, dcosdA));
116     f3 = dVdcosPhi * cross(dcosdB, r43);
117 cli2 1275
118 gezelter 1390 // In OpenMD's version of an improper torsion, the central atom
119 cli2 1275 // comes first. However, to get the planarity in a typical cosine
120     // version of this potential (i.e. Amber-style), the central atom
121     // is treated as atom *3* in a standard torsion form:
122    
123     // AMBER: I - J - K - L (e.g. K is sp2 hybridized carbon)
124 gezelter 1390 // OpenMD: I - (J - K - L) (e.g. I is sp2 hybridized carbon)
125 cli2 1275
126     // Confusing enough? Good.
127    
128 cli2 1290 atom2_->addFrc(f1);
129     atom1_->addFrc(f2 - f1 + f3);
130     atom4_->addFrc(-f2);
131     atom3_->addFrc(-f3);
132    
133 gezelter 1782 if (doParticlePot) {
134     atom1_->addParticlePot(potential_);
135     atom2_->addParticlePot(potential_);
136     atom3_->addParticlePot(potential_);
137     atom4_->addParticlePot(potential_);
138     }
139    
140 cli2 1275 angle = acos(cos_phi) /M_PI * 180.0;
141     }
142    
143     }

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