| 40 |
|
* [5] Vardeman, Stocker & Gezelter, J. Chem. Theory Comput. 7, 834 (2011). |
| 41 |
|
*/ |
| 42 |
|
|
| 43 |
+ |
#ifdef IS_MPI |
| 44 |
+ |
#include <mpi.h> |
| 45 |
+ |
#endif |
| 46 |
+ |
|
| 47 |
|
#include <stdio.h> |
| 48 |
|
#include <string.h> |
| 49 |
|
|
| 50 |
|
#include <cmath> |
| 51 |
+ |
#include <numeric> |
| 52 |
|
#include "nonbonded/Electrostatic.hpp" |
| 53 |
|
#include "utils/simError.h" |
| 54 |
|
#include "types/NonBondedInteractionType.hpp" |
| 60 |
|
#include "utils/PhysicalConstants.hpp" |
| 61 |
|
#include "math/erfc.hpp" |
| 62 |
|
#include "math/SquareMatrix.hpp" |
| 63 |
+ |
#include "primitives/Molecule.hpp" |
| 64 |
+ |
#include "flucq/FluctuatingChargeForces.hpp" |
| 65 |
|
|
| 66 |
|
namespace OpenMD { |
| 67 |
|
|
| 68 |
|
Electrostatic::Electrostatic(): name_("Electrostatic"), initialized_(false), |
| 62 |
– |
forceField_(NULL), info_(NULL), |
| 69 |
|
haveCutoffRadius_(false), |
| 70 |
|
haveDampingAlpha_(false), |
| 71 |
|
haveDielectric_(false), |
| 72 |
< |
haveElectroSplines_(false) |
| 73 |
< |
{} |
| 72 |
> |
haveElectroSplines_(false), |
| 73 |
> |
info_(NULL), forceField_(NULL) |
| 74 |
> |
|
| 75 |
> |
{ |
| 76 |
> |
flucQ_ = new FluctuatingChargeForces(info_); |
| 77 |
> |
} |
| 78 |
|
|
| 79 |
+ |
void Electrostatic::setForceField(ForceField *ff) { |
| 80 |
+ |
forceField_ = ff; |
| 81 |
+ |
flucQ_->setForceField(forceField_); |
| 82 |
+ |
} |
| 83 |
+ |
|
| 84 |
+ |
void Electrostatic::setSimulatedAtomTypes(set<AtomType*> &simtypes) { |
| 85 |
+ |
simTypes_ = simtypes; |
| 86 |
+ |
flucQ_->setSimulatedAtomTypes(simTypes_); |
| 87 |
+ |
} |
| 88 |
+ |
|
| 89 |
|
void Electrostatic::initialize() { |
| 90 |
|
|
| 91 |
|
Globals* simParams_ = info_->getSimParams(); |
| 211 |
|
simError(); |
| 212 |
|
} |
| 213 |
|
|
| 214 |
< |
if (screeningMethod_ == DAMPED) { |
| 214 |
> |
if (screeningMethod_ == DAMPED || summationMethod_ == esm_EWALD_FULL) { |
| 215 |
|
if (!simParams_->haveDampingAlpha()) { |
| 216 |
|
// first set a cutoff dependent alpha value |
| 217 |
|
// we assume alpha depends linearly with rcut from 0 to 20.5 ang |
| 218 |
|
dampingAlpha_ = 0.425 - cutoffRadius_* 0.02; |
| 219 |
< |
if (dampingAlpha_ < 0.0) dampingAlpha_ = 0.0; |
| 200 |
< |
|
| 219 |
> |
if (dampingAlpha_ < 0.0) dampingAlpha_ = 0.0; |
| 220 |
|
// throw warning |
| 221 |
|
sprintf( painCave.errMsg, |
| 222 |
|
"Electrostatic::initialize: dampingAlpha was not specified in the\n" |
| 232 |
|
haveDampingAlpha_ = true; |
| 233 |
|
} |
| 234 |
|
|
| 235 |
+ |
|
| 236 |
|
Etypes.clear(); |
| 237 |
|
Etids.clear(); |
| 238 |
|
FQtypes.clear(); |
| 264 |
|
|
| 265 |
|
RealType b0c, b1c, b2c, b3c, b4c, b5c; |
| 266 |
|
RealType db0c_1, db0c_2, db0c_3, db0c_4, db0c_5; |
| 267 |
< |
RealType a2, expTerm, invArootPi; |
| 267 |
> |
RealType a2, expTerm, invArootPi(0.0); |
| 268 |
|
|
| 269 |
|
RealType r = cutoffRadius_; |
| 270 |
|
RealType r2 = r * r; |
| 282 |
|
b3c = (5.0 * b2c + pow(2.0*a2, 3) * expTerm * invArootPi) / r2; |
| 283 |
|
b4c = (7.0 * b3c + pow(2.0*a2, 4) * expTerm * invArootPi) / r2; |
| 284 |
|
b5c = (9.0 * b4c + pow(2.0*a2, 5) * expTerm * invArootPi) / r2; |
| 265 |
– |
//selfMult1_ = - 2.0 * a2 * invArootPi; |
| 266 |
– |
//selfMult2_ = - 4.0 * a2 * a2 * invArootPi / 3.0; |
| 267 |
– |
//selfMult4_ = - 8.0 * a2 * a2 * a2 * invArootPi / 5.0; |
| 285 |
|
// Half the Smith self piece: |
| 286 |
|
selfMult1_ = - a2 * invArootPi; |
| 287 |
|
selfMult2_ = - 2.0 * a2 * a2 * invArootPi / 3.0; |
| 305 |
|
db0c_3 = 3.0*r*b2c - r2*r*b3c; |
| 306 |
|
db0c_4 = 3.0*b2c - 6.0*r2*b3c + r2*r2*b4c; |
| 307 |
|
db0c_5 = -15.0*r*b3c + 10.0*r2*r*b4c - r2*r2*r*b5c; |
| 291 |
– |
|
| 292 |
– |
selfMult1_ -= b0c; |
| 293 |
– |
selfMult2_ += (db0c_2 + 2.0*db0c_1*ric) / 3.0; |
| 294 |
– |
selfMult4_ -= (db0c_4 + 4.0*db0c_3*ric) / 15.0; |
| 308 |
|
|
| 309 |
+ |
if (summationMethod_ != esm_EWALD_FULL) { |
| 310 |
+ |
selfMult1_ -= b0c; |
| 311 |
+ |
selfMult2_ += (db0c_2 + 2.0*db0c_1*ric) / 3.0; |
| 312 |
+ |
selfMult4_ -= (db0c_4 + 4.0*db0c_3*ric) / 15.0; |
| 313 |
+ |
} |
| 314 |
+ |
|
| 315 |
|
// working variables for the splines: |
| 316 |
|
RealType ri, ri2; |
| 317 |
|
RealType b0, b1, b2, b3, b4, b5; |
| 347 |
|
vector<RealType> v31v, v32v; |
| 348 |
|
vector<RealType> v41v, v42v, v43v; |
| 349 |
|
|
| 331 |
– |
/* |
| 332 |
– |
vector<RealType> dv01v; |
| 333 |
– |
vector<RealType> dv11v; |
| 334 |
– |
vector<RealType> dv21v, dv22v; |
| 335 |
– |
vector<RealType> dv31v, dv32v; |
| 336 |
– |
vector<RealType> dv41v, dv42v, dv43v; |
| 337 |
– |
*/ |
| 338 |
– |
|
| 350 |
|
for (int i = 1; i < np_ + 1; i++) { |
| 351 |
|
r = RealType(i) * dx; |
| 352 |
|
rv.push_back(r); |
| 510 |
|
|
| 511 |
|
case esm_SWITCHING_FUNCTION: |
| 512 |
|
case esm_HARD: |
| 513 |
+ |
case esm_EWALD_FULL: |
| 514 |
|
|
| 515 |
|
v01 = f; |
| 516 |
|
v11 = g; |
| 569 |
|
|
| 570 |
|
break; |
| 571 |
|
|
| 560 |
– |
case esm_EWALD_FULL: |
| 572 |
|
case esm_EWALD_PME: |
| 573 |
|
case esm_EWALD_SPME: |
| 574 |
|
default : |
| 597 |
|
v41v.push_back(v41); |
| 598 |
|
v42v.push_back(v42); |
| 599 |
|
v43v.push_back(v43); |
| 589 |
– |
/* |
| 590 |
– |
dv01v.push_back(dv01); |
| 591 |
– |
dv11v.push_back(dv11); |
| 592 |
– |
dv21v.push_back(dv21); |
| 593 |
– |
dv22v.push_back(dv22); |
| 594 |
– |
dv31v.push_back(dv31); |
| 595 |
– |
dv32v.push_back(dv32); |
| 596 |
– |
dv41v.push_back(dv41); |
| 597 |
– |
dv42v.push_back(dv42); |
| 598 |
– |
dv43v.push_back(dv43); |
| 599 |
– |
*/ |
| 600 |
|
} |
| 601 |
|
|
| 602 |
|
// construct the spline structures and fill them with the values we've |
| 620 |
|
v42s->addPoints(rv, v42v); |
| 621 |
|
v43s = new CubicSpline(); |
| 622 |
|
v43s->addPoints(rv, v43v); |
| 623 |
– |
|
| 624 |
– |
/* |
| 625 |
– |
dv01s = new CubicSpline(); |
| 626 |
– |
dv01s->addPoints(rv, dv01v); |
| 627 |
– |
dv11s = new CubicSpline(); |
| 628 |
– |
dv11s->addPoints(rv, dv11v); |
| 629 |
– |
dv21s = new CubicSpline(); |
| 630 |
– |
dv21s->addPoints(rv, dv21v); |
| 631 |
– |
dv22s = new CubicSpline(); |
| 632 |
– |
dv22s->addPoints(rv, dv22v); |
| 633 |
– |
dv31s = new CubicSpline(); |
| 634 |
– |
dv31s->addPoints(rv, dv31v); |
| 635 |
– |
dv32s = new CubicSpline(); |
| 636 |
– |
dv32s->addPoints(rv, dv32v); |
| 637 |
– |
dv41s = new CubicSpline(); |
| 638 |
– |
dv41s->addPoints(rv, dv41v); |
| 639 |
– |
dv42s = new CubicSpline(); |
| 640 |
– |
dv42s->addPoints(rv, dv42v); |
| 641 |
– |
dv43s = new CubicSpline(); |
| 642 |
– |
dv43s->addPoints(rv, dv43v); |
| 643 |
– |
*/ |
| 623 |
|
|
| 624 |
|
haveElectroSplines_ = true; |
| 625 |
|
|
| 694 |
|
FQtids[atid] = fqtid; |
| 695 |
|
Jij[fqtid].resize(nFlucq_); |
| 696 |
|
|
| 697 |
< |
// Now, iterate over all known fluctuating and add to the coulomb integral map: |
| 697 |
> |
// Now, iterate over all known fluctuating and add to the |
| 698 |
> |
// coulomb integral map: |
| 699 |
|
|
| 700 |
|
std::set<int>::iterator it; |
| 701 |
|
for( it = FQtypes.begin(); it != FQtypes.end(); ++it) { |
| 769 |
|
Tb.zero(); // Torque on site b |
| 770 |
|
Ea.zero(); // Electric field at site a |
| 771 |
|
Eb.zero(); // Electric field at site b |
| 772 |
+ |
Pa = 0.0; // Site potential at site a |
| 773 |
+ |
Pb = 0.0; // Site potential at site b |
| 774 |
|
dUdCa = 0.0; // fluctuating charge force at site a |
| 775 |
|
dUdCb = 0.0; // fluctuating charge force at site a |
| 776 |
|
|
| 783 |
|
// Excluded potential that is still computed for fluctuating charges |
| 784 |
|
excluded_Pot= 0.0; |
| 785 |
|
|
| 804 |
– |
|
| 786 |
|
// some variables we'll need independent of electrostatic type: |
| 787 |
|
|
| 788 |
|
ri = 1.0 / *(idat.rij); |
| 845 |
|
if (idat.excluded) { |
| 846 |
|
*(idat.skippedCharge2) += C_a; |
| 847 |
|
} else { |
| 848 |
< |
// only do the field if we're not excluded: |
| 848 |
> |
// only do the field and site potentials if we're not excluded: |
| 849 |
|
Eb -= C_a * pre11_ * dv01 * rhat; |
| 850 |
+ |
Pb += C_a * pre11_ * v01; |
| 851 |
|
} |
| 852 |
|
} |
| 853 |
|
|
| 855 |
|
D_a = *(idat.dipole1); |
| 856 |
|
rdDa = dot(rhat, D_a); |
| 857 |
|
rxDa = cross(rhat, D_a); |
| 858 |
< |
if (!idat.excluded) |
| 858 |
> |
if (!idat.excluded) { |
| 859 |
|
Eb -= pre12_ * ((dv11-v11or) * rdDa * rhat + v11or * D_a); |
| 860 |
+ |
Pb += pre12_ * v11 * rdDa; |
| 861 |
+ |
} |
| 862 |
+ |
|
| 863 |
|
} |
| 864 |
|
|
| 865 |
|
if (a_is_Quadrupole) { |
| 869 |
|
rQa = rhat * Q_a; |
| 870 |
|
rdQar = dot(rhat, Qar); |
| 871 |
|
rxQar = cross(rhat, Qar); |
| 872 |
< |
if (!idat.excluded) |
| 872 |
> |
if (!idat.excluded) { |
| 873 |
|
Eb -= pre14_ * (trQa * rhat * dv21 + 2.0 * Qar * v22or |
| 874 |
|
+ rdQar * rhat * (dv22 - 2.0*v22or)); |
| 875 |
+ |
Pb += pre14_ * (v21 * trQa + v22 * rdQar); |
| 876 |
+ |
} |
| 877 |
|
} |
| 878 |
|
|
| 879 |
|
if (b_is_Charge) { |
| 887 |
|
} else { |
| 888 |
|
// only do the field if we're not excluded: |
| 889 |
|
Ea += C_b * pre11_ * dv01 * rhat; |
| 890 |
+ |
Pa += C_b * pre11_ * v01; |
| 891 |
+ |
|
| 892 |
|
} |
| 893 |
|
} |
| 894 |
|
|
| 896 |
|
D_b = *(idat.dipole2); |
| 897 |
|
rdDb = dot(rhat, D_b); |
| 898 |
|
rxDb = cross(rhat, D_b); |
| 899 |
< |
if (!idat.excluded) |
| 899 |
> |
if (!idat.excluded) { |
| 900 |
|
Ea += pre12_ * ((dv11-v11or) * rdDb * rhat + v11or * D_b); |
| 901 |
+ |
Pa += pre12_ * v11 * rdDb; |
| 902 |
+ |
} |
| 903 |
|
} |
| 904 |
|
|
| 905 |
|
if (b_is_Quadrupole) { |
| 909 |
|
rQb = rhat * Q_b; |
| 910 |
|
rdQbr = dot(rhat, Qbr); |
| 911 |
|
rxQbr = cross(rhat, Qbr); |
| 912 |
< |
if (!idat.excluded) |
| 912 |
> |
if (!idat.excluded) { |
| 913 |
|
Ea += pre14_ * (trQb * rhat * dv21 + 2.0 * Qbr * v22or |
| 914 |
|
+ rdQbr * rhat * (dv22 - 2.0*v22or)); |
| 915 |
+ |
Pa += pre14_ * (v21 * trQb + v22 * rdQbr); |
| 916 |
+ |
} |
| 917 |
|
} |
| 918 |
< |
|
| 918 |
> |
|
| 919 |
> |
|
| 920 |
|
if ((a_is_Fluctuating || b_is_Fluctuating) && idat.excluded) { |
| 921 |
|
J = Jij[FQtids[idat.atid1]][FQtids[idat.atid2]]; |
| 922 |
|
} |
| 923 |
< |
|
| 923 |
> |
|
| 924 |
|
if (a_is_Charge) { |
| 925 |
|
|
| 926 |
|
if (b_is_Charge) { |
| 927 |
|
pref = pre11_ * *(idat.electroMult); |
| 928 |
|
U += C_a * C_b * pref * v01; |
| 929 |
|
F += C_a * C_b * pref * dv01 * rhat; |
| 930 |
< |
|
| 930 |
> |
|
| 931 |
|
// If this is an excluded pair, there are still indirect |
| 932 |
|
// interactions via the reaction field we must worry about: |
| 933 |
|
|
| 936 |
|
indirect_Pot += rfContrib; |
| 937 |
|
indirect_F += rfContrib * 2.0 * ri * rhat; |
| 938 |
|
} |
| 939 |
< |
|
| 939 |
> |
|
| 940 |
|
// Fluctuating charge forces are handled via Coulomb integrals |
| 941 |
|
// for excluded pairs (i.e. those connected via bonds) and |
| 942 |
|
// with the standard charge-charge interaction otherwise. |
| 943 |
|
|
| 944 |
< |
if (idat.excluded) { |
| 944 |
> |
if (idat.excluded) { |
| 945 |
|
if (a_is_Fluctuating || b_is_Fluctuating) { |
| 946 |
|
coulInt = J->getValueAt( *(idat.rij) ); |
| 947 |
< |
if (a_is_Fluctuating) dUdCa += coulInt * C_b; |
| 948 |
< |
if (b_is_Fluctuating) dUdCb += coulInt * C_a; |
| 949 |
< |
excluded_Pot += C_a * C_b * coulInt; |
| 956 |
< |
} |
| 947 |
> |
if (a_is_Fluctuating) dUdCa += C_b * coulInt; |
| 948 |
> |
if (b_is_Fluctuating) dUdCb += C_a * coulInt; |
| 949 |
> |
} |
| 950 |
|
} else { |
| 951 |
|
if (a_is_Fluctuating) dUdCa += C_b * pref * v01; |
| 952 |
< |
if (a_is_Fluctuating) dUdCb += C_a * pref * v01; |
| 953 |
< |
} |
| 952 |
> |
if (b_is_Fluctuating) dUdCb += C_a * pref * v01; |
| 953 |
> |
} |
| 954 |
|
} |
| 955 |
|
|
| 956 |
|
if (b_is_Dipole) { |
| 1016 |
|
F -= pref * (rdDa * rdDb) * (dv22 - 2.0*v22or) * rhat; |
| 1017 |
|
Ta += pref * ( v21 * DaxDb - v22 * rdDb * rxDa); |
| 1018 |
|
Tb += pref * (-v21 * DaxDb - v22 * rdDa * rxDb); |
| 1026 |
– |
|
| 1019 |
|
// Even if we excluded this pair from direct interactions, we |
| 1020 |
|
// still have the reaction-field-mediated dipole-dipole |
| 1021 |
|
// interaction: |
| 1075 |
|
trQaQb = QaQb.trace(); |
| 1076 |
|
rQaQb = rhat * QaQb; |
| 1077 |
|
QaQbr = QaQb * rhat; |
| 1078 |
< |
QaxQb = cross(Q_a, Q_b); |
| 1078 |
> |
QaxQb = mCross(Q_a, Q_b); |
| 1079 |
|
rQaQbr = dot(rQa, Qbr); |
| 1080 |
|
rQaxQbr = cross(rQa, Qbr); |
| 1081 |
|
|
| 1106 |
|
// + 4.0 * cross(rhat, QbQar) |
| 1107 |
|
|
| 1108 |
|
Tb += pref * 2.0 * cross(rhat,Qbr) * rdQar * v43; |
| 1117 |
– |
|
| 1109 |
|
} |
| 1110 |
|
} |
| 1111 |
|
|
| 1114 |
|
*(idat.eField2) += Eb * *(idat.electroMult); |
| 1115 |
|
} |
| 1116 |
|
|
| 1117 |
+ |
if (idat.doSitePotential) { |
| 1118 |
+ |
*(idat.sPot1) += Pa * *(idat.electroMult); |
| 1119 |
+ |
*(idat.sPot2) += Pb * *(idat.electroMult); |
| 1120 |
+ |
} |
| 1121 |
+ |
|
| 1122 |
|
if (a_is_Fluctuating) *(idat.dVdFQ1) += dUdCa * *(idat.sw); |
| 1123 |
|
if (b_is_Fluctuating) *(idat.dVdFQ2) += dUdCb * *(idat.sw); |
| 1124 |
|
|
| 1165 |
|
bool i_is_Quadrupole = data.is_Quadrupole; |
| 1166 |
|
bool i_is_Fluctuating = data.is_Fluctuating; |
| 1167 |
|
RealType C_a = data.fixedCharge; |
| 1168 |
< |
RealType self(0.0), preVal, DdD, trQ, trQQ; |
| 1168 |
> |
RealType self(0.0), preVal, DdD(0.0), trQ, trQQ; |
| 1169 |
|
|
| 1170 |
|
if (i_is_Dipole) { |
| 1171 |
|
DdD = data.dipole.lengthSquare(); |
| 1173 |
|
|
| 1174 |
|
if (i_is_Fluctuating) { |
| 1175 |
|
C_a += *(sdat.flucQ); |
| 1176 |
< |
// dVdFQ is really a force, so this is negative the derivative |
| 1177 |
< |
*(sdat.dVdFQ) -= *(sdat.flucQ) * data.hardness + data.electronegativity; |
| 1178 |
< |
(*(sdat.excludedPot))[ELECTROSTATIC_FAMILY] += (*sdat.flucQ) * |
| 1179 |
< |
(*(sdat.flucQ) * data.hardness * 0.5 + data.electronegativity); |
| 1176 |
> |
|
| 1177 |
> |
flucQ_->getSelfInteraction(sdat.atid, *(sdat.flucQ), |
| 1178 |
> |
(*(sdat.excludedPot))[ELECTROSTATIC_FAMILY], |
| 1179 |
> |
*(sdat.flucQfrc) ); |
| 1180 |
> |
|
| 1181 |
|
} |
| 1182 |
|
|
| 1183 |
|
switch (summationMethod_) { |
| 1199 |
|
|
| 1200 |
|
case esm_SHIFTED_FORCE: |
| 1201 |
|
case esm_SHIFTED_POTENTIAL: |
| 1202 |
+ |
case esm_TAYLOR_SHIFTED: |
| 1203 |
+ |
case esm_EWALD_FULL: |
| 1204 |
|
if (i_is_Charge) |
| 1205 |
|
self += selfMult1_ * pre11_ * C_a * (C_a + *(sdat.skippedCharge)); |
| 1206 |
|
if (i_is_Dipole) |
| 1225 |
|
// 12 angstroms seems to be a reasonably good guess for most |
| 1226 |
|
// cases. |
| 1227 |
|
return 12.0; |
| 1228 |
+ |
} |
| 1229 |
+ |
|
| 1230 |
+ |
|
| 1231 |
+ |
void Electrostatic::ReciprocalSpaceSum(RealType& pot) { |
| 1232 |
+ |
|
| 1233 |
+ |
RealType kPot = 0.0; |
| 1234 |
+ |
RealType kVir = 0.0; |
| 1235 |
+ |
|
| 1236 |
+ |
const RealType mPoleConverter = 0.20819434; // converts from the |
| 1237 |
+ |
// internal units of |
| 1238 |
+ |
// Debye (for dipoles) |
| 1239 |
+ |
// or Debye-angstroms |
| 1240 |
+ |
// (for quadrupoles) to |
| 1241 |
+ |
// electron angstroms or |
| 1242 |
+ |
// electron-angstroms^2 |
| 1243 |
+ |
|
| 1244 |
+ |
const RealType eConverter = 332.0637778; // convert the |
| 1245 |
+ |
// Charge-Charge |
| 1246 |
+ |
// electrostatic |
| 1247 |
+ |
// interactions into kcal / |
| 1248 |
+ |
// mol assuming distances |
| 1249 |
+ |
// are measured in |
| 1250 |
+ |
// angstroms. |
| 1251 |
+ |
|
| 1252 |
+ |
Mat3x3d hmat = info_->getSnapshotManager()->getCurrentSnapshot()->getHmat(); |
| 1253 |
+ |
Vector3d box = hmat.diagonals(); |
| 1254 |
+ |
RealType boxMax = box.max(); |
| 1255 |
+ |
|
| 1256 |
+ |
//int kMax = int(2.0 * M_PI / (pow(dampingAlpha_,2)*cutoffRadius_ * boxMax) ); |
| 1257 |
+ |
int kMax = 7; |
| 1258 |
+ |
int kSqMax = kMax*kMax + 2; |
| 1259 |
+ |
|
| 1260 |
+ |
int kLimit = kMax+1; |
| 1261 |
+ |
int kLim2 = 2*kMax+1; |
| 1262 |
+ |
int kSqLim = kSqMax; |
| 1263 |
+ |
|
| 1264 |
+ |
vector<RealType> AK(kSqLim+1, 0.0); |
| 1265 |
+ |
RealType xcl = 2.0 * M_PI / box.x(); |
| 1266 |
+ |
RealType ycl = 2.0 * M_PI / box.y(); |
| 1267 |
+ |
RealType zcl = 2.0 * M_PI / box.z(); |
| 1268 |
+ |
RealType rcl = 2.0 * M_PI / boxMax; |
| 1269 |
+ |
RealType rvol = 2.0 * M_PI /(box.x() * box.y() * box.z()); |
| 1270 |
+ |
|
| 1271 |
+ |
if(dampingAlpha_ < 1.0e-12) return; |
| 1272 |
+ |
|
| 1273 |
+ |
RealType ralph = -0.25/pow(dampingAlpha_,2); |
| 1274 |
+ |
|
| 1275 |
+ |
// Calculate and store exponential factors |
| 1276 |
+ |
|
| 1277 |
+ |
vector<vector<RealType> > elc; |
| 1278 |
+ |
vector<vector<RealType> > emc; |
| 1279 |
+ |
vector<vector<RealType> > enc; |
| 1280 |
+ |
vector<vector<RealType> > els; |
| 1281 |
+ |
vector<vector<RealType> > ems; |
| 1282 |
+ |
vector<vector<RealType> > ens; |
| 1283 |
+ |
|
| 1284 |
+ |
int nMax = info_->getNAtoms(); |
| 1285 |
+ |
|
| 1286 |
+ |
elc.resize(kLimit+1); |
| 1287 |
+ |
emc.resize(kLimit+1); |
| 1288 |
+ |
enc.resize(kLimit+1); |
| 1289 |
+ |
els.resize(kLimit+1); |
| 1290 |
+ |
ems.resize(kLimit+1); |
| 1291 |
+ |
ens.resize(kLimit+1); |
| 1292 |
+ |
|
| 1293 |
+ |
for (int j = 0; j < kLimit+1; j++) { |
| 1294 |
+ |
elc[j].resize(nMax); |
| 1295 |
+ |
emc[j].resize(nMax); |
| 1296 |
+ |
enc[j].resize(nMax); |
| 1297 |
+ |
els[j].resize(nMax); |
| 1298 |
+ |
ems[j].resize(nMax); |
| 1299 |
+ |
ens[j].resize(nMax); |
| 1300 |
+ |
} |
| 1301 |
+ |
|
| 1302 |
+ |
Vector3d t( 2.0 * M_PI ); |
| 1303 |
+ |
t.Vdiv(t, box); |
| 1304 |
+ |
|
| 1305 |
+ |
SimInfo::MoleculeIterator mi; |
| 1306 |
+ |
Molecule::AtomIterator ai; |
| 1307 |
+ |
int i; |
| 1308 |
+ |
Vector3d r; |
| 1309 |
+ |
Vector3d tt; |
| 1310 |
+ |
|
| 1311 |
+ |
for (Molecule* mol = info_->beginMolecule(mi); mol != NULL; |
| 1312 |
+ |
mol = info_->nextMolecule(mi)) { |
| 1313 |
+ |
for(Atom* atom = mol->beginAtom(ai); atom != NULL; |
| 1314 |
+ |
atom = mol->nextAtom(ai)) { |
| 1315 |
+ |
|
| 1316 |
+ |
i = atom->getLocalIndex(); |
| 1317 |
+ |
r = atom->getPos(); |
| 1318 |
+ |
info_->getSnapshotManager()->getCurrentSnapshot()->wrapVector(r); |
| 1319 |
+ |
|
| 1320 |
+ |
tt.Vmul(t, r); |
| 1321 |
+ |
|
| 1322 |
+ |
elc[1][i] = 1.0; |
| 1323 |
+ |
emc[1][i] = 1.0; |
| 1324 |
+ |
enc[1][i] = 1.0; |
| 1325 |
+ |
els[1][i] = 0.0; |
| 1326 |
+ |
ems[1][i] = 0.0; |
| 1327 |
+ |
ens[1][i] = 0.0; |
| 1328 |
+ |
|
| 1329 |
+ |
elc[2][i] = cos(tt.x()); |
| 1330 |
+ |
emc[2][i] = cos(tt.y()); |
| 1331 |
+ |
enc[2][i] = cos(tt.z()); |
| 1332 |
+ |
els[2][i] = sin(tt.x()); |
| 1333 |
+ |
ems[2][i] = sin(tt.y()); |
| 1334 |
+ |
ens[2][i] = sin(tt.z()); |
| 1335 |
+ |
|
| 1336 |
+ |
for(int l = 3; l <= kLimit; l++) { |
| 1337 |
+ |
elc[l][i]=elc[l-1][i]*elc[2][i]-els[l-1][i]*els[2][i]; |
| 1338 |
+ |
emc[l][i]=emc[l-1][i]*emc[2][i]-ems[l-1][i]*ems[2][i]; |
| 1339 |
+ |
enc[l][i]=enc[l-1][i]*enc[2][i]-ens[l-1][i]*ens[2][i]; |
| 1340 |
+ |
els[l][i]=els[l-1][i]*elc[2][i]+elc[l-1][i]*els[2][i]; |
| 1341 |
+ |
ems[l][i]=ems[l-1][i]*emc[2][i]+emc[l-1][i]*ems[2][i]; |
| 1342 |
+ |
ens[l][i]=ens[l-1][i]*enc[2][i]+enc[l-1][i]*ens[2][i]; |
| 1343 |
+ |
} |
| 1344 |
+ |
} |
| 1345 |
+ |
} |
| 1346 |
+ |
|
| 1347 |
+ |
// Calculate and store AK coefficients: |
| 1348 |
+ |
|
| 1349 |
+ |
RealType eksq = 1.0; |
| 1350 |
+ |
RealType expf = 0.0; |
| 1351 |
+ |
if (ralph < 0.0) expf = exp(ralph*rcl*rcl); |
| 1352 |
+ |
for (i = 1; i <= kSqLim; i++) { |
| 1353 |
+ |
RealType rksq = float(i)*rcl*rcl; |
| 1354 |
+ |
eksq = expf*eksq; |
| 1355 |
+ |
AK[i] = eConverter * eksq/rksq; |
| 1356 |
+ |
} |
| 1357 |
+ |
|
| 1358 |
+ |
/* |
| 1359 |
+ |
* Loop over all k vectors k = 2 pi (ll/Lx, mm/Ly, nn/Lz) |
| 1360 |
+ |
* the values of ll, mm and nn are selected so that the symmetry of |
| 1361 |
+ |
* reciprocal lattice is taken into account i.e. the following |
| 1362 |
+ |
* rules apply. |
| 1363 |
+ |
* |
| 1364 |
+ |
* ll ranges over the values 0 to kMax only. |
| 1365 |
+ |
* |
| 1366 |
+ |
* mm ranges over 0 to kMax when ll=0 and over |
| 1367 |
+ |
* -kMax to kMax otherwise. |
| 1368 |
+ |
* nn ranges over 1 to kMax when ll=mm=0 and over |
| 1369 |
+ |
* -kMax to kMax otherwise. |
| 1370 |
+ |
* |
| 1371 |
+ |
* Hence the result of the summation must be doubled at the end. |
| 1372 |
+ |
*/ |
| 1373 |
+ |
|
| 1374 |
+ |
std::vector<RealType> clm(nMax, 0.0); |
| 1375 |
+ |
std::vector<RealType> slm(nMax, 0.0); |
| 1376 |
+ |
std::vector<RealType> ckr(nMax, 0.0); |
| 1377 |
+ |
std::vector<RealType> skr(nMax, 0.0); |
| 1378 |
+ |
std::vector<RealType> ckc(nMax, 0.0); |
| 1379 |
+ |
std::vector<RealType> cks(nMax, 0.0); |
| 1380 |
+ |
std::vector<RealType> dkc(nMax, 0.0); |
| 1381 |
+ |
std::vector<RealType> dks(nMax, 0.0); |
| 1382 |
+ |
std::vector<RealType> qkc(nMax, 0.0); |
| 1383 |
+ |
std::vector<RealType> qks(nMax, 0.0); |
| 1384 |
+ |
std::vector<Vector3d> dxk(nMax, V3Zero); |
| 1385 |
+ |
std::vector<Vector3d> qxk(nMax, V3Zero); |
| 1386 |
+ |
RealType rl, rm, rn; |
| 1387 |
+ |
Vector3d kVec; |
| 1388 |
+ |
Vector3d Qk; |
| 1389 |
+ |
Mat3x3d k2; |
| 1390 |
+ |
RealType ckcs, ckss, dkcs, dkss, qkcs, qkss; |
| 1391 |
+ |
int atid; |
| 1392 |
+ |
ElectrostaticAtomData data; |
| 1393 |
+ |
RealType C, dk, qk; |
| 1394 |
+ |
Vector3d D; |
| 1395 |
+ |
Mat3x3d Q; |
| 1396 |
+ |
|
| 1397 |
+ |
int mMin = kLimit; |
| 1398 |
+ |
int nMin = kLimit + 1; |
| 1399 |
+ |
for (int l = 1; l <= kLimit; l++) { |
| 1400 |
+ |
int ll = l - 1; |
| 1401 |
+ |
rl = xcl * float(ll); |
| 1402 |
+ |
for (int mmm = mMin; mmm <= kLim2; mmm++) { |
| 1403 |
+ |
int mm = mmm - kLimit; |
| 1404 |
+ |
int m = abs(mm) + 1; |
| 1405 |
+ |
rm = ycl * float(mm); |
| 1406 |
+ |
// Set temporary products of exponential terms |
| 1407 |
+ |
for (Molecule* mol = info_->beginMolecule(mi); mol != NULL; |
| 1408 |
+ |
mol = info_->nextMolecule(mi)) { |
| 1409 |
+ |
for(Atom* atom = mol->beginAtom(ai); atom != NULL; |
| 1410 |
+ |
atom = mol->nextAtom(ai)) { |
| 1411 |
+ |
|
| 1412 |
+ |
i = atom->getLocalIndex(); |
| 1413 |
+ |
if(mm < 0) { |
| 1414 |
+ |
clm[i]=elc[l][i]*emc[m][i]+els[l][i]*ems[m][i]; |
| 1415 |
+ |
slm[i]=els[l][i]*emc[m][i]-ems[m][i]*elc[l][i]; |
| 1416 |
+ |
} else { |
| 1417 |
+ |
clm[i]=elc[l][i]*emc[m][i]-els[l][i]*ems[m][i]; |
| 1418 |
+ |
slm[i]=els[l][i]*emc[m][i]+ems[m][i]*elc[l][i]; |
| 1419 |
+ |
} |
| 1420 |
+ |
} |
| 1421 |
+ |
} |
| 1422 |
+ |
for (int nnn = nMin; nnn <= kLim2; nnn++) { |
| 1423 |
+ |
int nn = nnn - kLimit; |
| 1424 |
+ |
int n = abs(nn) + 1; |
| 1425 |
+ |
rn = zcl * float(nn); |
| 1426 |
+ |
// Test on magnitude of k vector: |
| 1427 |
+ |
int kk=ll*ll + mm*mm + nn*nn; |
| 1428 |
+ |
if(kk <= kSqLim) { |
| 1429 |
+ |
kVec = Vector3d(rl, rm, rn); |
| 1430 |
+ |
k2 = outProduct(kVec, kVec); |
| 1431 |
+ |
// Calculate exp(ikr) terms |
| 1432 |
+ |
for (Molecule* mol = info_->beginMolecule(mi); mol != NULL; |
| 1433 |
+ |
mol = info_->nextMolecule(mi)) { |
| 1434 |
+ |
for(Atom* atom = mol->beginAtom(ai); atom != NULL; |
| 1435 |
+ |
atom = mol->nextAtom(ai)) { |
| 1436 |
+ |
i = atom->getLocalIndex(); |
| 1437 |
+ |
|
| 1438 |
+ |
if (nn < 0) { |
| 1439 |
+ |
ckr[i]=clm[i]*enc[n][i]+slm[i]*ens[n][i]; |
| 1440 |
+ |
skr[i]=slm[i]*enc[n][i]-clm[i]*ens[n][i]; |
| 1441 |
+ |
|
| 1442 |
+ |
} else { |
| 1443 |
+ |
ckr[i]=clm[i]*enc[n][i]-slm[i]*ens[n][i]; |
| 1444 |
+ |
skr[i]=slm[i]*enc[n][i]+clm[i]*ens[n][i]; |
| 1445 |
+ |
} |
| 1446 |
+ |
} |
| 1447 |
+ |
} |
| 1448 |
+ |
|
| 1449 |
+ |
// Calculate scalar and vector products for each site: |
| 1450 |
+ |
|
| 1451 |
+ |
for (Molecule* mol = info_->beginMolecule(mi); mol != NULL; |
| 1452 |
+ |
mol = info_->nextMolecule(mi)) { |
| 1453 |
+ |
for(Atom* atom = mol->beginAtom(ai); atom != NULL; |
| 1454 |
+ |
atom = mol->nextAtom(ai)) { |
| 1455 |
+ |
i = atom->getLocalIndex(); |
| 1456 |
+ |
int atid = atom->getAtomType()->getIdent(); |
| 1457 |
+ |
data = ElectrostaticMap[Etids[atid]]; |
| 1458 |
+ |
|
| 1459 |
+ |
if (data.is_Charge) { |
| 1460 |
+ |
C = data.fixedCharge; |
| 1461 |
+ |
if (atom->isFluctuatingCharge()) C += atom->getFlucQPos(); |
| 1462 |
+ |
ckc[i] = C * ckr[i]; |
| 1463 |
+ |
cks[i] = C * skr[i]; |
| 1464 |
+ |
} |
| 1465 |
+ |
|
| 1466 |
+ |
if (data.is_Dipole) { |
| 1467 |
+ |
D = atom->getDipole() * mPoleConverter; |
| 1468 |
+ |
dk = dot(D, kVec); |
| 1469 |
+ |
dxk[i] = cross(D, kVec); |
| 1470 |
+ |
dkc[i] = dk * ckr[i]; |
| 1471 |
+ |
dks[i] = dk * skr[i]; |
| 1472 |
+ |
} |
| 1473 |
+ |
if (data.is_Quadrupole) { |
| 1474 |
+ |
Q = atom->getQuadrupole() * mPoleConverter; |
| 1475 |
+ |
Qk = Q * kVec; |
| 1476 |
+ |
qk = dot(kVec, Qk); |
| 1477 |
+ |
qxk[i] = -cross(kVec, Qk); |
| 1478 |
+ |
qkc[i] = qk * ckr[i]; |
| 1479 |
+ |
qks[i] = qk * skr[i]; |
| 1480 |
+ |
} |
| 1481 |
+ |
} |
| 1482 |
+ |
} |
| 1483 |
+ |
|
| 1484 |
+ |
// calculate vector sums |
| 1485 |
+ |
|
| 1486 |
+ |
ckcs = std::accumulate(ckc.begin(),ckc.end(),0.0); |
| 1487 |
+ |
ckss = std::accumulate(cks.begin(),cks.end(),0.0); |
| 1488 |
+ |
dkcs = std::accumulate(dkc.begin(),dkc.end(),0.0); |
| 1489 |
+ |
dkss = std::accumulate(dks.begin(),dks.end(),0.0); |
| 1490 |
+ |
qkcs = std::accumulate(qkc.begin(),qkc.end(),0.0); |
| 1491 |
+ |
qkss = std::accumulate(qks.begin(),qks.end(),0.0); |
| 1492 |
+ |
|
| 1493 |
+ |
#ifdef IS_MPI |
| 1494 |
+ |
MPI_Allreduce(MPI_IN_PLACE, &ckcs, 1, MPI_REALTYPE, |
| 1495 |
+ |
MPI_SUM, MPI_COMM_WORLD); |
| 1496 |
+ |
MPI_Allreduce(MPI_IN_PLACE, &ckss, 1, MPI_REALTYPE, |
| 1497 |
+ |
MPI_SUM, MPI_COMM_WORLD); |
| 1498 |
+ |
MPI_Allreduce(MPI_IN_PLACE, &dkcs, 1, MPI_REALTYPE, |
| 1499 |
+ |
MPI_SUM, MPI_COMM_WORLD); |
| 1500 |
+ |
MPI_Allreduce(MPI_IN_PLACE, &dkss, 1, MPI_REALTYPE, |
| 1501 |
+ |
MPI_SUM, MPI_COMM_WORLD); |
| 1502 |
+ |
MPI_Allreduce(MPI_IN_PLACE, &qkcs, 1, MPI_REALTYPE, |
| 1503 |
+ |
MPI_SUM, MPI_COMM_WORLD); |
| 1504 |
+ |
MPI_Allreduce(MPI_IN_PLACE, &qkss, 1, MPI_REALTYPE, |
| 1505 |
+ |
MPI_SUM, MPI_COMM_WORLD); |
| 1506 |
+ |
#endif |
| 1507 |
+ |
|
| 1508 |
+ |
// Accumulate potential energy and virial contribution: |
| 1509 |
+ |
|
| 1510 |
+ |
kPot += 2.0 * rvol * AK[kk]*((ckss+dkcs-qkss)*(ckss+dkcs-qkss) |
| 1511 |
+ |
+ (ckcs-dkss-qkcs)*(ckcs-dkss-qkcs)); |
| 1512 |
+ |
|
| 1513 |
+ |
kVir += 2.0 * rvol * AK[kk]*(ckcs*ckcs+ckss*ckss |
| 1514 |
+ |
+4.0*(ckss*dkcs-ckcs*dkss) |
| 1515 |
+ |
+3.0*(dkcs*dkcs+dkss*dkss) |
| 1516 |
+ |
-6.0*(ckss*qkss+ckcs*qkcs) |
| 1517 |
+ |
+8.0*(dkss*qkcs-dkcs*qkss) |
| 1518 |
+ |
+5.0*(qkss*qkss+qkcs*qkcs)); |
| 1519 |
+ |
|
| 1520 |
+ |
// Calculate force and torque for each site: |
| 1521 |
+ |
|
| 1522 |
+ |
for (Molecule* mol = info_->beginMolecule(mi); mol != NULL; |
| 1523 |
+ |
mol = info_->nextMolecule(mi)) { |
| 1524 |
+ |
for(Atom* atom = mol->beginAtom(ai); atom != NULL; |
| 1525 |
+ |
atom = mol->nextAtom(ai)) { |
| 1526 |
+ |
|
| 1527 |
+ |
i = atom->getLocalIndex(); |
| 1528 |
+ |
atid = atom->getAtomType()->getIdent(); |
| 1529 |
+ |
data = ElectrostaticMap[Etids[atid]]; |
| 1530 |
+ |
|
| 1531 |
+ |
RealType qfrc = AK[kk]*((cks[i]+dkc[i]-qks[i])*(ckcs-dkss-qkcs) |
| 1532 |
+ |
- (ckc[i]-dks[i]-qkc[i])*(ckss+dkcs-qkss)); |
| 1533 |
+ |
RealType qtrq1 = AK[kk]*(skr[i]*(ckcs-dkss-qkcs) |
| 1534 |
+ |
-ckr[i]*(ckss+dkcs-qkss)); |
| 1535 |
+ |
RealType qtrq2 = 2.0*AK[kk]*(ckr[i]*(ckcs-dkss-qkcs) |
| 1536 |
+ |
+skr[i]*(ckss+dkcs-qkss)); |
| 1537 |
+ |
|
| 1538 |
+ |
atom->addFrc( 4.0 * rvol * qfrc * kVec ); |
| 1539 |
+ |
|
| 1540 |
+ |
if (atom->isFluctuatingCharge()) { |
| 1541 |
+ |
atom->addFlucQFrc( - 2.0 * rvol * qtrq2 ); |
| 1542 |
+ |
} |
| 1543 |
+ |
|
| 1544 |
+ |
if (data.is_Dipole) { |
| 1545 |
+ |
atom->addTrq( 4.0 * rvol * qtrq1 * dxk[i] ); |
| 1546 |
+ |
} |
| 1547 |
+ |
if (data.is_Quadrupole) { |
| 1548 |
+ |
atom->addTrq( 4.0 * rvol * qtrq2 * qxk[i] ); |
| 1549 |
+ |
} |
| 1550 |
+ |
} |
| 1551 |
+ |
} |
| 1552 |
+ |
} |
| 1553 |
+ |
} |
| 1554 |
+ |
nMin = 1; |
| 1555 |
+ |
} |
| 1556 |
+ |
mMin = 1; |
| 1557 |
+ |
} |
| 1558 |
+ |
pot += kPot; |
| 1559 |
|
} |
| 1560 |
+ |
|
| 1561 |
+ |
void Electrostatic::getSitePotentials(Atom* a1, Atom* a2, bool excluded, |
| 1562 |
+ |
RealType &spot1, RealType &spot2) { |
| 1563 |
+ |
|
| 1564 |
+ |
if (!initialized_) { |
| 1565 |
+ |
cerr << "initializing\n"; |
| 1566 |
+ |
initialize(); |
| 1567 |
+ |
cerr << "done\n"; |
| 1568 |
+ |
} |
| 1569 |
+ |
|
| 1570 |
+ |
const RealType mPoleConverter = 0.20819434; |
| 1571 |
+ |
|
| 1572 |
+ |
AtomType* atype1 = a1->getAtomType(); |
| 1573 |
+ |
AtomType* atype2 = a2->getAtomType(); |
| 1574 |
+ |
int atid1 = atype1->getIdent(); |
| 1575 |
+ |
int atid2 = atype2->getIdent(); |
| 1576 |
+ |
data1 = ElectrostaticMap[Etids[atid1]]; |
| 1577 |
+ |
data2 = ElectrostaticMap[Etids[atid2]]; |
| 1578 |
+ |
|
| 1579 |
+ |
Pa = 0.0; // Site potential at site a |
| 1580 |
+ |
Pb = 0.0; // Site potential at site b |
| 1581 |
+ |
|
| 1582 |
+ |
Vector3d d = a2->getPos() - a1->getPos(); |
| 1583 |
+ |
info_->getSnapshotManager()->getCurrentSnapshot()->wrapVector(d); |
| 1584 |
+ |
RealType rij = d.length(); |
| 1585 |
+ |
// some variables we'll need independent of electrostatic type: |
| 1586 |
+ |
|
| 1587 |
+ |
RealType ri = 1.0 / rij; |
| 1588 |
+ |
rhat = d * ri; |
| 1589 |
+ |
|
| 1590 |
+ |
|
| 1591 |
+ |
if ((rij >= cutoffRadius_) || excluded) { |
| 1592 |
+ |
spot1 = 0.0; |
| 1593 |
+ |
spot2 = 0.0; |
| 1594 |
+ |
return; |
| 1595 |
+ |
} |
| 1596 |
+ |
|
| 1597 |
+ |
// logicals |
| 1598 |
+ |
|
| 1599 |
+ |
a_is_Charge = data1.is_Charge; |
| 1600 |
+ |
a_is_Dipole = data1.is_Dipole; |
| 1601 |
+ |
a_is_Quadrupole = data1.is_Quadrupole; |
| 1602 |
+ |
a_is_Fluctuating = data1.is_Fluctuating; |
| 1603 |
+ |
|
| 1604 |
+ |
b_is_Charge = data2.is_Charge; |
| 1605 |
+ |
b_is_Dipole = data2.is_Dipole; |
| 1606 |
+ |
b_is_Quadrupole = data2.is_Quadrupole; |
| 1607 |
+ |
b_is_Fluctuating = data2.is_Fluctuating; |
| 1608 |
+ |
|
| 1609 |
+ |
// Obtain all of the required radial function values from the |
| 1610 |
+ |
// spline structures: |
| 1611 |
+ |
|
| 1612 |
+ |
|
| 1613 |
+ |
if (a_is_Charge || b_is_Charge) { |
| 1614 |
+ |
v01 = v01s->getValueAt(rij); |
| 1615 |
+ |
} |
| 1616 |
+ |
if (a_is_Dipole || b_is_Dipole) { |
| 1617 |
+ |
v11 = v11s->getValueAt(rij); |
| 1618 |
+ |
v11or = ri * v11; |
| 1619 |
+ |
} |
| 1620 |
+ |
if (a_is_Quadrupole || b_is_Quadrupole) { |
| 1621 |
+ |
v21 = v21s->getValueAt(rij); |
| 1622 |
+ |
v22 = v22s->getValueAt(rij); |
| 1623 |
+ |
v22or = ri * v22; |
| 1624 |
+ |
} |
| 1625 |
+ |
|
| 1626 |
+ |
if (a_is_Charge) { |
| 1627 |
+ |
C_a = data1.fixedCharge; |
| 1628 |
+ |
|
| 1629 |
+ |
if (a_is_Fluctuating) { |
| 1630 |
+ |
C_a += a1->getFlucQPos(); |
| 1631 |
+ |
} |
| 1632 |
+ |
|
| 1633 |
+ |
Pb += C_a * pre11_ * v01; |
| 1634 |
+ |
} |
| 1635 |
+ |
|
| 1636 |
+ |
if (a_is_Dipole) { |
| 1637 |
+ |
D_a = a1->getDipole() * mPoleConverter; |
| 1638 |
+ |
rdDa = dot(rhat, D_a); |
| 1639 |
+ |
Pb += pre12_ * v11 * rdDa; |
| 1640 |
+ |
} |
| 1641 |
+ |
|
| 1642 |
+ |
if (a_is_Quadrupole) { |
| 1643 |
+ |
Q_a = a1->getQuadrupole() * mPoleConverter; |
| 1644 |
+ |
trQa = Q_a.trace(); |
| 1645 |
+ |
Qar = Q_a * rhat; |
| 1646 |
+ |
rdQar = dot(rhat, Qar); |
| 1647 |
+ |
Pb += pre14_ * (v21 * trQa + v22 * rdQar); |
| 1648 |
+ |
} |
| 1649 |
+ |
|
| 1650 |
+ |
if (b_is_Charge) { |
| 1651 |
+ |
C_b = data2.fixedCharge; |
| 1652 |
+ |
|
| 1653 |
+ |
if (b_is_Fluctuating) |
| 1654 |
+ |
C_b += a2->getFlucQPos(); |
| 1655 |
+ |
|
| 1656 |
+ |
Pa += C_b * pre11_ * v01; |
| 1657 |
+ |
} |
| 1658 |
+ |
|
| 1659 |
+ |
if (b_is_Dipole) { |
| 1660 |
+ |
D_b = a2->getDipole() * mPoleConverter; |
| 1661 |
+ |
rdDb = dot(rhat, D_b); |
| 1662 |
+ |
Pa += pre12_ * v11 * rdDb; |
| 1663 |
+ |
} |
| 1664 |
+ |
|
| 1665 |
+ |
if (b_is_Quadrupole) { |
| 1666 |
+ |
Q_a = a2->getQuadrupole() * mPoleConverter; |
| 1667 |
+ |
trQb = Q_b.trace(); |
| 1668 |
+ |
Qbr = Q_b * rhat; |
| 1669 |
+ |
rdQbr = dot(rhat, Qbr); |
| 1670 |
+ |
Pa += pre14_ * (v21 * trQb + v22 * rdQbr); |
| 1671 |
+ |
} |
| 1672 |
+ |
|
| 1673 |
+ |
spot1 = Pa; |
| 1674 |
+ |
spot2 = Pb; |
| 1675 |
+ |
} |
| 1676 |
|
} |