| 3 |
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#define PI 3.14159265359 |
| 4 |
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| 5 |
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|
| 6 |
< |
GridBuilder::GridBuilder(RigidBody* rb, int bandWidth) { |
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> |
GridBuilder::GridBuilder(RigidBody* rb, int gridWidth) { |
| 7 |
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rbMol = rb; |
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< |
bandwidth = bandWidth; |
| 9 |
< |
thetaStep = PI / bandwidth; |
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> |
gridwidth = gridWidth; |
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> |
thetaStep = PI / gridwidth; |
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thetaMin = thetaStep / 2.0; |
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phiStep = thetaStep * 2.0; |
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|
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//zero out the rot mats |
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for (i=0; i<3; i++) { |
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for (j=0; j<3; j++) { |
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rotX[i][j] = 0.0; |
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rotZ[i][j] = 0.0; |
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rbMatrix[i][j] = 0.0; |
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} |
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} |
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} |
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|
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GridBuilder::~GridBuilder() { |
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} |
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void GridBuilder::launchProbe(int forceField, vector<double> sigmaGrid, vector<double> sGrid, |
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vector<double> epsGrid){ |
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> |
void GridBuilder::launchProbe(int forceField, vector<double> sigmaGrid, |
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vector<double> sGrid, vector<double> epsGrid){ |
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ofstream sigmaOut("sigma.grid"); |
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ofstream sOut("s.grid"); |
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ofstream epsOut("eps.grid"); |
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double startDist; |
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+ |
double phiVal; |
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+ |
double thetaVal; |
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double sigTemp, sTemp, epsTemp, sigProbe; |
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double minDist = 10.0; //minimum start distance |
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|
| 28 |
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sList = sGrid; |
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sigList = sigmaGrid; |
| 30 |
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epsList = epsGrid; |
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forcefield = forceField; |
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+ |
|
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//load the probe atom parameters |
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+ |
switch(forcefield){ |
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case 1:{ |
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rparHe = 1.4800; |
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+ |
epsHe = -0.021270; |
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}; break; |
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+ |
case 2:{ |
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rparHe = 1.14; |
| 41 |
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epsHe = 0.0203; |
| 42 |
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}; break; |
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case 3:{ |
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rparHe = 2.28; |
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epsHe = 0.020269601874; |
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}; break; |
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+ |
case 4:{ |
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+ |
rparHe = 2.5560; |
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+ |
epsHe = 0.0200; |
| 50 |
+ |
}; break; |
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+ |
case 5:{ |
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rparHe = 1.14; |
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+ |
epsHe = 0.0203; |
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+ |
}; break; |
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} |
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|
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< |
//first determine the start distance - we always start at least minDist away |
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> |
if (rparHe < 2.2) |
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> |
sigProbe = 2*rparHe/1.12246204831; |
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> |
else |
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> |
sigProbe = rparHe; |
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> |
|
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> |
//determine the start distance - we always start at least minDist away |
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startDist = rbMol->findMaxExtent() + minDist; |
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if (startDist < minDist) |
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startDist = minDist; |
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|
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< |
initBody(); |
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< |
for (k=0; k<bandwidth; k++){ |
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< |
printf("step theta...\n"); |
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< |
for (j=0; j<bandwidth; j++){ |
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> |
//set the initial orientation of the body and loop over theta values |
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> |
|
| 69 |
> |
for (k =0; k < gridwidth; k++) { |
| 70 |
> |
thetaVal = thetaMin + k*thetaStep; |
| 71 |
> |
printf("Theta step %i\n", k); |
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> |
for (j=0; j < gridwidth; j++) { |
| 73 |
> |
phiVal = j*phiStep; |
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> |
|
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> |
rbMol->setEuler(0.0, thetaVal, phiVal); |
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> |
|
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releaseProbe(startDist); |
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|
| 79 |
< |
sigList.push_back(sigDist); |
| 80 |
< |
sList.push_back(sDist); |
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< |
epsList.push_back(epsVal); |
| 82 |
< |
|
| 83 |
< |
stepPhi(phiStep); |
| 79 |
> |
//translate the values to sigma, s, and epsilon of the rigid body |
| 80 |
> |
sigTemp = 2*sigDist - sigProbe; |
| 81 |
> |
sTemp = (2*(sDist - sigDist))/(0.122462048309) - sigProbe; |
| 82 |
> |
epsTemp = pow(epsVal, 2)/fabs(epsHe); |
| 83 |
> |
|
| 84 |
> |
sigList.push_back(sigTemp); |
| 85 |
> |
sList.push_back(sTemp); |
| 86 |
> |
epsList.push_back(epsTemp); |
| 87 |
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} |
| 56 |
– |
stepTheta(thetaStep); |
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} |
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/* |
| 59 |
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//write out the grid files |
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– |
printf("the grid size is %d\n",sigmaGrid.size()); |
| 61 |
– |
for (k=0; k<sigmaGrid.size(); k++){ |
| 62 |
– |
sigmaOut << sigmaGrid[k] << "\n0\n"; |
| 63 |
– |
sOut << sGrid[k] << "\n0\n"; |
| 64 |
– |
epsOut << epsGrid[k] << "\n0\n"; |
| 65 |
– |
} |
| 66 |
– |
*/ |
| 89 |
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} |
| 90 |
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|
| 69 |
– |
void GridBuilder::initBody(){ |
| 70 |
– |
//set up the rigid body in the starting configuration |
| 71 |
– |
stepTheta(thetaMin); |
| 72 |
– |
} |
| 73 |
– |
|
| 91 |
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void GridBuilder::releaseProbe(double farPos){ |
| 92 |
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int tooClose; |
| 93 |
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double tempPotEnergy; |
| 100 |
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tooClose = 0; |
| 101 |
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epsVal = 0; |
| 102 |
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rhoStep = 0.1; //the distance the probe atom moves between steps |
| 103 |
< |
|
| 87 |
< |
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| 103 |
> |
|
| 104 |
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while (!tooClose){ |
| 105 |
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calcEnergy(); |
| 106 |
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potProgress.push_back(potEnergy); |
| 141 |
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double rXij, rYij, rZij; |
| 142 |
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double rijSquared; |
| 143 |
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double rValSquared, rValPowerSix; |
| 128 |
– |
double rparHe, epsHe; |
| 144 |
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double atomRpar, atomEps; |
| 145 |
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double rbAtomPos[3]; |
| 146 |
< |
|
| 132 |
< |
//first get the probe atom parameters |
| 133 |
< |
switch(forcefield){ |
| 134 |
< |
case 1:{ |
| 135 |
< |
rparHe = 1.4800; |
| 136 |
< |
epsHe = -0.021270; |
| 137 |
< |
}; break; |
| 138 |
< |
case 2:{ |
| 139 |
< |
rparHe = 1.14; |
| 140 |
< |
epsHe = 0.0203; |
| 141 |
< |
}; break; |
| 142 |
< |
case 3:{ |
| 143 |
< |
rparHe = 2.28; |
| 144 |
< |
epsHe = 0.020269601874; |
| 145 |
< |
}; break; |
| 146 |
< |
case 4:{ |
| 147 |
< |
rparHe = 2.5560; |
| 148 |
< |
epsHe = 0.0200; |
| 149 |
< |
}; break; |
| 150 |
< |
case 5:{ |
| 151 |
< |
rparHe = 1.14; |
| 152 |
< |
epsHe = 0.0203; |
| 153 |
< |
}; break; |
| 154 |
< |
} |
| 155 |
< |
|
| 146 |
> |
|
| 147 |
|
potEnergy = 0.0; |
| 148 |
< |
|
| 148 |
> |
|
| 149 |
|
for(i=0; i<rbMol->getNumAtoms(); i++){ |
| 150 |
|
rbMol->getAtomPos(rbAtomPos, i); |
| 151 |
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|
| 155 |
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|
| 156 |
|
rijSquared = rXij * rXij + rYij * rYij + rZij * rZij; |
| 157 |
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|
| 158 |
< |
//in the interest of keeping the code more compact, we are being less efficient by placing |
| 159 |
< |
//a switch statement in the calculation loop |
| 158 |
> |
//in the interest of keeping the code more compact, we are being less |
| 159 |
> |
//efficient by placing a switch statement in the calculation loop |
| 160 |
|
switch(forcefield){ |
| 161 |
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case 1:{ |
| 162 |
|
//we are using the CHARMm force field |
| 188 |
|
potEnergy += 4*sqrt(epsHe*atomEps)*(rValPowerSix * (rValPowerSix - 1.0)); |
| 189 |
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|
| 190 |
|
}; break; |
| 200 |
– |
|
| 191 |
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|
| 192 |
|
case 4:{ |
| 193 |
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//we are using the OPLS force field |
| 212 |
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} |
| 213 |
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} |
| 214 |
|
|
| 225 |
– |
void GridBuilder::stepTheta(double increment){ |
| 226 |
– |
//zero out the euler angles |
| 227 |
– |
for (l=0; l<3; l++) |
| 228 |
– |
angles[i] = 0.0; |
| 229 |
– |
|
| 230 |
– |
//the second euler angle is for rotation about the x-axis (we use the zxz convention) |
| 231 |
– |
angles[1] = increment; |
| 232 |
– |
|
| 233 |
– |
//obtain the rotation matrix through the rigid body class |
| 234 |
– |
rbMol->doEulerToRotMat(angles, rotX); |
| 235 |
– |
|
| 236 |
– |
//rotate the rigid body |
| 237 |
– |
rbMol->getA(rbMatrix); |
| 238 |
– |
matMul3(rotX, rbMatrix, rotatedMat); |
| 239 |
– |
rbMol->setA(rotatedMat); |
| 240 |
– |
} |
| 241 |
– |
|
| 242 |
– |
void GridBuilder::stepPhi(double increment){ |
| 243 |
– |
//zero out the euler angles |
| 244 |
– |
for (l=0; l<3; l++) |
| 245 |
– |
angles[i] = 0.0; |
| 246 |
– |
|
| 247 |
– |
//the phi euler angle is for rotation about the z-axis (we use the zxz convention) |
| 248 |
– |
angles[0] = increment; |
| 249 |
– |
|
| 250 |
– |
//obtain the rotation matrix through the rigid body class |
| 251 |
– |
rbMol->doEulerToRotMat(angles, rotZ); |
| 252 |
– |
|
| 253 |
– |
//rotate the rigid body |
| 254 |
– |
rbMol->getA(rbMatrix); |
| 255 |
– |
matMul3(rotZ, rbMatrix, rotatedMat); |
| 256 |
– |
rbMol->setA(rotatedMat); |
| 257 |
– |
} |
| 258 |
– |
|
| 215 |
|
void GridBuilder::printGridFiles(){ |
| 216 |
|
ofstream sigmaOut("sigma.grid"); |
| 217 |
|
ofstream sOut("s.grid"); |
| 222 |
|
sOut << sList[k] << "\n0\n"; |
| 223 |
|
epsOut << epsList[k] << "\n0\n"; |
| 224 |
|
} |
| 225 |
< |
} |
| 225 |
> |
} |