1 |
#include "GridBuilder.hpp" |
2 |
#include "MatVec3.h" |
3 |
#define PI 3.14159265359 |
4 |
|
5 |
|
6 |
GridBuilder::GridBuilder(RigidBody* rb, int bandWidth) { |
7 |
rbMol = rb; |
8 |
bandwidth = bandWidth; |
9 |
thetaStep = PI / bandwidth; |
10 |
thetaMin = thetaStep / 2.0; |
11 |
phiStep = thetaStep * 2.0; |
12 |
|
13 |
//zero out the rot mats |
14 |
for (i=0; i<3; i++) { |
15 |
for (j=0; j<3; j++) { |
16 |
rotX[i][j] = 0.0; |
17 |
rotZ[i][j] = 0.0; |
18 |
rbMatrix[i][j] = 0.0; |
19 |
} |
20 |
} |
21 |
} |
22 |
|
23 |
GridBuilder::~GridBuilder() { |
24 |
} |
25 |
|
26 |
void GridBuilder::launchProbe(int forceField, vector<double> sigmaGrid, vector<double> sGrid, |
27 |
vector<double> epsGrid){ |
28 |
ofstream sigmaOut("sigma.grid"); |
29 |
ofstream sOut("s.grid"); |
30 |
ofstream epsOut("eps.grid"); |
31 |
double startDist; |
32 |
double phiVal; |
33 |
double thetaVal; |
34 |
double minDist = 10.0; //minimum start distance |
35 |
|
36 |
sList = sGrid; |
37 |
sigList = sigmaGrid; |
38 |
epsList = epsGrid; |
39 |
forcefield = forceField; |
40 |
|
41 |
//first determine the start distance - we always start at least minDist away |
42 |
startDist = rbMol->findMaxExtent() + minDist; |
43 |
if (startDist < minDist) |
44 |
startDist = minDist; |
45 |
|
46 |
//set the initial orientation of the body and loop over theta values |
47 |
phiVal = 0.0; |
48 |
thetaVal = thetaMin; |
49 |
rotBody(phiVal, thetaVal); |
50 |
for (k=0; k<bandwidth; k++){ |
51 |
//loop over phi values starting with phi = 0.0 |
52 |
for (j=0; j<bandwidth; j++){ |
53 |
releaseProbe(startDist); |
54 |
|
55 |
sigList.push_back(sigDist); |
56 |
sList.push_back(sDist); |
57 |
epsList.push_back(epsVal); |
58 |
|
59 |
phiVal += phiStep; |
60 |
rotBody(phiVal, thetaVal); |
61 |
} |
62 |
phiVal = 0.0; |
63 |
thetaVal += thetaStep; |
64 |
rotBody(phiVal, thetaVal); |
65 |
printf("step theta %i\n",k); |
66 |
} |
67 |
} |
68 |
|
69 |
void GridBuilder::releaseProbe(double farPos){ |
70 |
int tooClose; |
71 |
double tempPotEnergy; |
72 |
double interpRange; |
73 |
double interpFrac; |
74 |
|
75 |
probeCoor = farPos; |
76 |
potProgress.clear(); |
77 |
distProgress.clear(); |
78 |
tooClose = 0; |
79 |
epsVal = 0; |
80 |
rhoStep = 0.1; //the distance the probe atom moves between steps |
81 |
|
82 |
|
83 |
while (!tooClose){ |
84 |
calcEnergy(); |
85 |
potProgress.push_back(potEnergy); |
86 |
distProgress.push_back(probeCoor); |
87 |
|
88 |
//if we've reached a new minimum, save the value and position |
89 |
if (potEnergy < epsVal){ |
90 |
epsVal = potEnergy; |
91 |
sDist = probeCoor; |
92 |
} |
93 |
|
94 |
//test if the probe reached the origin - if so, stop stepping closer |
95 |
if (probeCoor < 0){ |
96 |
sigDist = 0.0; |
97 |
tooClose = 1; |
98 |
} |
99 |
|
100 |
//test if the probe beyond the contact point - if not, take a step closer |
101 |
if (potEnergy < 0){ |
102 |
sigDist = probeCoor; |
103 |
tempPotEnergy = potEnergy; |
104 |
probeCoor -= rhoStep; |
105 |
} |
106 |
else { |
107 |
//do a linear interpolation to obtain the sigDist |
108 |
interpRange = potEnergy - tempPotEnergy; |
109 |
interpFrac = potEnergy / interpRange; |
110 |
interpFrac = interpFrac * rhoStep; |
111 |
sigDist = probeCoor + interpFrac; |
112 |
|
113 |
//end the loop |
114 |
tooClose = 1; |
115 |
} |
116 |
} |
117 |
} |
118 |
|
119 |
void GridBuilder::calcEnergy(){ |
120 |
double rXij, rYij, rZij; |
121 |
double rijSquared; |
122 |
double rValSquared, rValPowerSix; |
123 |
double rparHe, epsHe; |
124 |
double atomRpar, atomEps; |
125 |
double rbAtomPos[3]; |
126 |
|
127 |
//first get the probe atom parameters |
128 |
switch(forcefield){ |
129 |
case 1:{ |
130 |
rparHe = 1.4800; |
131 |
epsHe = -0.021270; |
132 |
}; break; |
133 |
case 2:{ |
134 |
rparHe = 1.14; |
135 |
epsHe = 0.0203; |
136 |
}; break; |
137 |
case 3:{ |
138 |
rparHe = 2.28; |
139 |
epsHe = 0.020269601874; |
140 |
}; break; |
141 |
case 4:{ |
142 |
rparHe = 2.5560; |
143 |
epsHe = 0.0200; |
144 |
}; break; |
145 |
case 5:{ |
146 |
rparHe = 1.14; |
147 |
epsHe = 0.0203; |
148 |
}; break; |
149 |
} |
150 |
|
151 |
potEnergy = 0.0; |
152 |
|
153 |
for(i=0; i<rbMol->getNumAtoms(); i++){ |
154 |
rbMol->getAtomPos(rbAtomPos, i); |
155 |
|
156 |
rXij = rbAtomPos[0]; |
157 |
rYij = rbAtomPos[1]; |
158 |
rZij = rbAtomPos[2] - probeCoor; |
159 |
|
160 |
rijSquared = rXij * rXij + rYij * rYij + rZij * rZij; |
161 |
|
162 |
//in the interest of keeping the code more compact, we are being less efficient by placing |
163 |
//a switch statement in the calculation loop |
164 |
switch(forcefield){ |
165 |
case 1:{ |
166 |
//we are using the CHARMm force field |
167 |
atomRpar = rbMol->getAtomRpar(i); |
168 |
atomEps = rbMol->getAtomEps(i); |
169 |
|
170 |
rValSquared = ((rparHe+atomRpar)*(rparHe+atomRpar)) / (rijSquared); |
171 |
rValPowerSix = rValSquared * rValSquared * rValSquared; |
172 |
potEnergy += sqrt(epsHe*atomEps)*(rValPowerSix * (rValPowerSix - 2.0)); |
173 |
}; break; |
174 |
|
175 |
case 2:{ |
176 |
//we are using the AMBER force field |
177 |
atomRpar = rbMol->getAtomRpar(i); |
178 |
atomEps = rbMol->getAtomEps(i); |
179 |
|
180 |
rValSquared = ((rparHe+atomRpar)*(rparHe+atomRpar)) / (rijSquared); |
181 |
rValPowerSix = rValSquared * rValSquared * rValSquared; |
182 |
potEnergy += sqrt(epsHe*atomEps)*(rValPowerSix * (rValPowerSix - 2.0)); |
183 |
}; break; |
184 |
|
185 |
case 3:{ |
186 |
//we are using Allen-Tildesley LJ parameters |
187 |
atomRpar = rbMol->getAtomRpar(i); |
188 |
atomEps = rbMol->getAtomEps(i); |
189 |
|
190 |
rValSquared = ((rparHe+atomRpar)*(rparHe+atomRpar)) / (4*rijSquared); |
191 |
rValPowerSix = rValSquared * rValSquared * rValSquared; |
192 |
potEnergy += 4*sqrt(epsHe*atomEps)*(rValPowerSix * (rValPowerSix - 1.0)); |
193 |
|
194 |
}; break; |
195 |
|
196 |
case 4:{ |
197 |
//we are using the OPLS force field |
198 |
atomRpar = rbMol->getAtomRpar(i); |
199 |
atomEps = rbMol->getAtomEps(i); |
200 |
|
201 |
rValSquared = (pow(sqrt(rparHe+atomRpar),2)) / (rijSquared); |
202 |
rValPowerSix = rValSquared * rValSquared * rValSquared; |
203 |
potEnergy += 4*sqrt(epsHe*atomEps)*(rValPowerSix * (rValPowerSix - 1.0)); |
204 |
}; break; |
205 |
|
206 |
case 5:{ |
207 |
//we are using the GAFF force field |
208 |
atomRpar = rbMol->getAtomRpar(i); |
209 |
atomEps = rbMol->getAtomEps(i); |
210 |
|
211 |
rValSquared = ((rparHe+atomRpar)*(rparHe+atomRpar)) / (rijSquared); |
212 |
rValPowerSix = rValSquared * rValSquared * rValSquared; |
213 |
potEnergy += sqrt(epsHe*atomEps)*(rValPowerSix * (rValPowerSix - 2.0)); |
214 |
}; break; |
215 |
} |
216 |
} |
217 |
} |
218 |
|
219 |
void GridBuilder::rotBody(double pValue, double tValue){ |
220 |
//zero out the euler angles |
221 |
for (l=0; l<3; l++) |
222 |
angles[i] = 0.0; |
223 |
|
224 |
//the phi euler angle is for rotation about the z-axis (we use the zxz convention) |
225 |
angles[0] = pValue; |
226 |
//the second euler angle is for rotation about the x-axis (we use the zxz convention) |
227 |
angles[1] = tValue; |
228 |
|
229 |
//obtain the rotation matrix through the rigid body class |
230 |
rbMol->doEulerToRotMat(angles, rotX); |
231 |
|
232 |
//start from the reference position |
233 |
identityMat3(rbMatrix); |
234 |
rbMol->setA(rbMatrix); |
235 |
|
236 |
//rotate the rigid body |
237 |
matMul3(rotX, rbMatrix, rotatedMat); |
238 |
rbMol->setA(rotatedMat); |
239 |
} |
240 |
|
241 |
void GridBuilder::printGridFiles(){ |
242 |
ofstream sigmaOut("sigma.grid"); |
243 |
ofstream sOut("s.grid"); |
244 |
ofstream epsOut("eps.grid"); |
245 |
|
246 |
for (k=0; k<sigList.size(); k++){ |
247 |
sigmaOut << sigList[k] << "\n0\n"; |
248 |
sOut << sList[k] << "\n0\n"; |
249 |
epsOut << epsList[k] << "\n0\n"; |
250 |
} |
251 |
} |