| 213 |
|
haveDampingAlpha_ = true; |
| 214 |
|
} |
| 215 |
|
|
| 216 |
< |
// find all of the Electrostatic atom Types: |
| 217 |
< |
ForceField::AtomTypeContainer* atomTypes = forceField_->getAtomTypes(); |
| 218 |
< |
ForceField::AtomTypeContainer::MapTypeIterator i; |
| 219 |
< |
AtomType* at; |
| 216 |
> |
Etypes.clear(); |
| 217 |
> |
Etids.clear(); |
| 218 |
> |
FQtypes.clear(); |
| 219 |
> |
FQtids.clear(); |
| 220 |
> |
ElectrostaticMap.clear(); |
| 221 |
> |
Jij.clear(); |
| 222 |
> |
nElectro_ = 0; |
| 223 |
> |
nFlucq_ = 0; |
| 224 |
> |
|
| 225 |
> |
Etids.resize( forceField_->getNAtomType(), -1); |
| 226 |
> |
FQtids.resize( forceField_->getNAtomType(), -1); |
| 227 |
> |
|
| 228 |
> |
set<AtomType*>::iterator at; |
| 229 |
> |
for (at = simTypes_.begin(); at != simTypes_.end(); ++at) { |
| 230 |
> |
if ((*at)->isElectrostatic()) nElectro_++; |
| 231 |
> |
if ((*at)->isFluctuatingCharge()) nFlucq_++; |
| 232 |
> |
} |
| 233 |
|
|
| 234 |
< |
for (at = atomTypes->beginType(i); at != NULL; |
| 235 |
< |
at = atomTypes->nextType(i)) { |
| 236 |
< |
|
| 237 |
< |
if (at->isElectrostatic()) |
| 225 |
< |
addType(at); |
| 234 |
> |
Jij.resize(nFlucq_); |
| 235 |
> |
|
| 236 |
> |
for (at = simTypes_.begin(); at != simTypes_.end(); ++at) { |
| 237 |
> |
if ((*at)->isElectrostatic()) addType(*at); |
| 238 |
|
} |
| 239 |
|
|
| 240 |
|
if (summationMethod_ == esm_REACTION_FIELD) { |
| 410 |
|
v11 = g - gc - rmRc*hc; |
| 411 |
|
v21 = g*ri - gc*ric - rmRc*(hc - gc*ric)*ric; |
| 412 |
|
v22 = h - g*ri - (hc - gc*ric) - rmRc*(sc - (hc - gc*ric)*ric); |
| 413 |
< |
v31 = (h-g*ri)*ri - (hc-g*ric)*ric - rmRc*(sc-2.0*(hc-gc*ric)*ric)*ric; |
| 413 |
> |
v31 = (h-g*ri)*ri - (hc-gc*ric)*ric - rmRc*(sc-2.0*(hc-gc*ric)*ric)*ric; |
| 414 |
|
v32 = (s - 3.0*(h-g*ri)*ri) - (sc - 3.0*(hc-gc*ric)*ric) |
| 415 |
|
- rmRc*(tc - 3.0*(sc-2.0*(hc-gc*ric)*ric)*ric); |
| 416 |
|
v41 = (h - g*ri)*ri2 - (hc - gc*ric)*ric2 |
| 467 |
|
v11 = g - gc; |
| 468 |
|
v21 = g*ri - gc*ric; |
| 469 |
|
v22 = h - g*ri - (hc - gc*ric); |
| 470 |
< |
v31 = (h-g*ri)*ri - (hc-g*ric)*ric; |
| 470 |
> |
v31 = (h-g*ri)*ri - (hc-gc*ric)*ric; |
| 471 |
|
v32 = (s - 3.0*(h-g*ri)*ri) - (sc - 3.0*(hc-gc*ric)*ric); |
| 472 |
|
v41 = (h - g*ri)*ri2 - (hc - gc*ric)*ric2; |
| 473 |
|
v42 = (s-3.0*(h-g*ri)*ri)*ri - (sc-3.0*(hc-gc*ric)*ric)*ric; |
| 527 |
|
v11 = g - gc; |
| 528 |
|
v21 = g*ri - gc*ric; |
| 529 |
|
v22 = h - g*ri - (hc - gc*ric); |
| 530 |
< |
v31 = (h-g*ri)*ri - (hc-g*ric)*ric; |
| 530 |
> |
v31 = (h-g*ri)*ri - (hc-gc*ric)*ric; |
| 531 |
|
v32 = (s - 3.0*(h-g*ri)*ri) - (sc - 3.0*(hc-gc*ric)*ric); |
| 532 |
|
v41 = (h - g*ri)*ri2 - (hc - gc*ric)*ric2; |
| 533 |
|
v42 = (s-3.0*(h-g*ri)*ri)*ri - (sc-3.0*(hc-gc*ric)*ric)*ric; |
| 637 |
|
} |
| 638 |
|
|
| 639 |
|
void Electrostatic::addType(AtomType* atomType){ |
| 640 |
< |
|
| 640 |
> |
|
| 641 |
|
ElectrostaticAtomData electrostaticAtomData; |
| 642 |
|
electrostaticAtomData.is_Charge = false; |
| 643 |
|
electrostaticAtomData.is_Dipole = false; |
| 673 |
|
electrostaticAtomData.slaterZeta = fqa.getSlaterZeta(); |
| 674 |
|
} |
| 675 |
|
|
| 676 |
< |
pair<map<int,AtomType*>::iterator,bool> ret; |
| 677 |
< |
ret = ElectrostaticList.insert( pair<int,AtomType*>(atomType->getIdent(), |
| 678 |
< |
atomType) ); |
| 676 |
> |
int atid = atomType->getIdent(); |
| 677 |
> |
int etid = Etypes.size(); |
| 678 |
> |
int fqtid = FQtypes.size(); |
| 679 |
> |
|
| 680 |
> |
pair<set<int>::iterator,bool> ret; |
| 681 |
> |
ret = Etypes.insert( atid ); |
| 682 |
|
if (ret.second == false) { |
| 683 |
|
sprintf( painCave.errMsg, |
| 684 |
|
"Electrostatic already had a previous entry with ident %d\n", |
| 685 |
< |
atomType->getIdent() ); |
| 685 |
> |
atid); |
| 686 |
|
painCave.severity = OPENMD_INFO; |
| 687 |
|
painCave.isFatal = 0; |
| 688 |
|
simError(); |
| 689 |
|
} |
| 690 |
|
|
| 691 |
< |
ElectrostaticMap[atomType] = electrostaticAtomData; |
| 691 |
> |
Etids[ atid ] = etid; |
| 692 |
> |
ElectrostaticMap.push_back(electrostaticAtomData); |
| 693 |
|
|
| 694 |
< |
// Now, iterate over all known types and add to the mixing map: |
| 695 |
< |
|
| 696 |
< |
map<AtomType*, ElectrostaticAtomData>::iterator it; |
| 697 |
< |
for( it = ElectrostaticMap.begin(); it != ElectrostaticMap.end(); ++it) { |
| 698 |
< |
AtomType* atype2 = (*it).first; |
| 699 |
< |
ElectrostaticAtomData eaData2 = (*it).second; |
| 700 |
< |
if (eaData2.is_Fluctuating && electrostaticAtomData.is_Fluctuating) { |
| 701 |
< |
|
| 694 |
> |
if (electrostaticAtomData.is_Fluctuating) { |
| 695 |
> |
ret = FQtypes.insert( atid ); |
| 696 |
> |
if (ret.second == false) { |
| 697 |
> |
sprintf( painCave.errMsg, |
| 698 |
> |
"Electrostatic already had a previous fluctuating charge entry with ident %d\n", |
| 699 |
> |
atid ); |
| 700 |
> |
painCave.severity = OPENMD_INFO; |
| 701 |
> |
painCave.isFatal = 0; |
| 702 |
> |
simError(); |
| 703 |
> |
} |
| 704 |
> |
FQtids[atid] = fqtid; |
| 705 |
> |
Jij[fqtid].resize(nFlucq_); |
| 706 |
> |
|
| 707 |
> |
// Now, iterate over all known fluctuating and add to the coulomb integral map: |
| 708 |
> |
|
| 709 |
> |
std::set<int>::iterator it; |
| 710 |
> |
for( it = FQtypes.begin(); it != FQtypes.end(); ++it) { |
| 711 |
> |
int etid2 = Etids[ (*it) ]; |
| 712 |
> |
int fqtid2 = FQtids[ (*it) ]; |
| 713 |
> |
ElectrostaticAtomData eaData2 = ElectrostaticMap[ etid2 ]; |
| 714 |
|
RealType a = electrostaticAtomData.slaterZeta; |
| 715 |
|
RealType b = eaData2.slaterZeta; |
| 716 |
|
int m = electrostaticAtomData.slaterN; |
| 717 |
|
int n = eaData2.slaterN; |
| 718 |
< |
|
| 718 |
> |
|
| 719 |
|
// Create the spline of the coulombic integral for s-type |
| 720 |
|
// Slater orbitals. Add a 2 angstrom safety window to deal |
| 721 |
|
// with cutoffGroups that have charged atoms longer than the |
| 722 |
|
// cutoffRadius away from each other. |
| 723 |
< |
|
| 723 |
> |
|
| 724 |
|
RealType rval; |
| 725 |
|
RealType dr = (cutoffRadius_ + 2.0) / RealType(np_ - 1); |
| 726 |
|
vector<RealType> rvals; |
| 737 |
|
|
| 738 |
|
CubicSpline* J = new CubicSpline(); |
| 739 |
|
J->addPoints(rvals, Jvals); |
| 740 |
< |
|
| 741 |
< |
pair<AtomType*, AtomType*> key1, key2; |
| 742 |
< |
key1 = make_pair(atomType, atype2); |
| 743 |
< |
key2 = make_pair(atype2, atomType); |
| 744 |
< |
|
| 717 |
< |
Jij[key1] = J; |
| 718 |
< |
Jij[key2] = J; |
| 719 |
< |
} |
| 720 |
< |
} |
| 721 |
< |
|
| 740 |
> |
Jij[fqtid][fqtid2] = J; |
| 741 |
> |
Jij[fqtid2].resize( nFlucq_ ); |
| 742 |
> |
Jij[fqtid2][fqtid] = J; |
| 743 |
> |
} |
| 744 |
> |
} |
| 745 |
|
return; |
| 746 |
|
} |
| 747 |
|
|
| 767 |
|
|
| 768 |
|
void Electrostatic::calcForce(InteractionData &idat) { |
| 769 |
|
|
| 770 |
< |
RealType C_a, C_b; // Charges |
| 771 |
< |
Vector3d D_a, D_b; // Dipoles (space-fixed) |
| 772 |
< |
Mat3x3d Q_a, Q_b; // Quadrupoles (space-fixed) |
| 770 |
> |
if (!initialized_) initialize(); |
| 771 |
> |
|
| 772 |
> |
data1 = ElectrostaticMap[Etids[idat.atid1]]; |
| 773 |
> |
data2 = ElectrostaticMap[Etids[idat.atid2]]; |
| 774 |
|
|
| 775 |
< |
RealType ri; // Distance utility scalar |
| 776 |
< |
RealType rdDa, rdDb; // Dipole utility scalars |
| 777 |
< |
Vector3d rxDa, rxDb; // Dipole utility vectors |
| 778 |
< |
RealType rdQar, rdQbr, trQa, trQb; // Quadrupole utility scalars |
| 779 |
< |
Vector3d Qar, Qbr, rQa, rQb, rxQar, rxQbr; // Quadrupole utility vectors |
| 780 |
< |
RealType pref; |
| 781 |
< |
|
| 782 |
< |
RealType DadDb, trQaQb, DadQbr, DbdQar; // Cross-interaction scalars |
| 759 |
< |
RealType rQaQbr; |
| 760 |
< |
Vector3d DaxDb, DadQb, DbdQa, DaxQbr, DbxQar; // Cross-interaction vectors |
| 761 |
< |
Vector3d rQaQb, QaQbr, QaxQb, rQaxQbr; |
| 762 |
< |
Mat3x3d QaQb; // Cross-interaction matrices |
| 763 |
< |
|
| 764 |
< |
RealType U(0.0); // Potential |
| 765 |
< |
Vector3d F(0.0); // Force |
| 766 |
< |
Vector3d Ta(0.0); // Torque on site a |
| 767 |
< |
Vector3d Tb(0.0); // Torque on site b |
| 768 |
< |
Vector3d Ea(0.0); // Electric field at site a |
| 769 |
< |
Vector3d Eb(0.0); // Electric field at site b |
| 770 |
< |
RealType dUdCa(0.0); // fluctuating charge force at site a |
| 771 |
< |
RealType dUdCb(0.0); // fluctuating charge force at site a |
| 775 |
> |
U = 0.0; // Potential |
| 776 |
> |
F.zero(); // Force |
| 777 |
> |
Ta.zero(); // Torque on site a |
| 778 |
> |
Tb.zero(); // Torque on site b |
| 779 |
> |
Ea.zero(); // Electric field at site a |
| 780 |
> |
Eb.zero(); // Electric field at site b |
| 781 |
> |
dUdCa = 0.0; // fluctuating charge force at site a |
| 782 |
> |
dUdCb = 0.0; // fluctuating charge force at site a |
| 783 |
|
|
| 784 |
|
// Indirect interactions mediated by the reaction field. |
| 785 |
< |
RealType indirect_Pot(0.0); // Potential |
| 786 |
< |
Vector3d indirect_F(0.0); // Force |
| 787 |
< |
Vector3d indirect_Ta(0.0); // Torque on site a |
| 788 |
< |
Vector3d indirect_Tb(0.0); // Torque on site b |
| 785 |
> |
indirect_Pot = 0.0; // Potential |
| 786 |
> |
indirect_F.zero(); // Force |
| 787 |
> |
indirect_Ta.zero(); // Torque on site a |
| 788 |
> |
indirect_Tb.zero(); // Torque on site b |
| 789 |
|
|
| 790 |
|
// Excluded potential that is still computed for fluctuating charges |
| 791 |
< |
RealType excluded_Pot(0.0); |
| 791 |
> |
excluded_Pot= 0.0; |
| 792 |
|
|
| 782 |
– |
RealType rfContrib, coulInt; |
| 783 |
– |
|
| 784 |
– |
// spline for coulomb integral |
| 785 |
– |
CubicSpline* J; |
| 793 |
|
|
| 787 |
– |
if (!initialized_) initialize(); |
| 788 |
– |
|
| 789 |
– |
ElectrostaticAtomData data1 = ElectrostaticMap[idat.atypes.first]; |
| 790 |
– |
ElectrostaticAtomData data2 = ElectrostaticMap[idat.atypes.second]; |
| 791 |
– |
|
| 794 |
|
// some variables we'll need independent of electrostatic type: |
| 795 |
|
|
| 796 |
|
ri = 1.0 / *(idat.rij); |
| 797 |
< |
Vector3d rhat = *(idat.d) * ri; |
| 797 |
> |
rhat = *(idat.d) * ri; |
| 798 |
|
|
| 799 |
|
// logicals |
| 800 |
|
|
| 801 |
< |
bool a_is_Charge = data1.is_Charge; |
| 802 |
< |
bool a_is_Dipole = data1.is_Dipole; |
| 803 |
< |
bool a_is_Quadrupole = data1.is_Quadrupole; |
| 804 |
< |
bool a_is_Fluctuating = data1.is_Fluctuating; |
| 801 |
> |
a_is_Charge = data1.is_Charge; |
| 802 |
> |
a_is_Dipole = data1.is_Dipole; |
| 803 |
> |
a_is_Quadrupole = data1.is_Quadrupole; |
| 804 |
> |
a_is_Fluctuating = data1.is_Fluctuating; |
| 805 |
|
|
| 806 |
< |
bool b_is_Charge = data2.is_Charge; |
| 807 |
< |
bool b_is_Dipole = data2.is_Dipole; |
| 808 |
< |
bool b_is_Quadrupole = data2.is_Quadrupole; |
| 809 |
< |
bool b_is_Fluctuating = data2.is_Fluctuating; |
| 806 |
> |
b_is_Charge = data2.is_Charge; |
| 807 |
> |
b_is_Dipole = data2.is_Dipole; |
| 808 |
> |
b_is_Quadrupole = data2.is_Quadrupole; |
| 809 |
> |
b_is_Fluctuating = data2.is_Fluctuating; |
| 810 |
|
|
| 811 |
|
// Obtain all of the required radial function values from the |
| 812 |
|
// spline structures: |
| 913 |
|
} |
| 914 |
|
|
| 915 |
|
if ((a_is_Fluctuating || b_is_Fluctuating) && idat.excluded) { |
| 916 |
< |
J = Jij[idat.atypes]; |
| 916 |
> |
J = Jij[FQtids[idat.atid1]][FQtids[idat.atid2]]; |
| 917 |
|
} |
| 918 |
|
|
| 919 |
|
if (a_is_Charge) { |
| 1151 |
|
|
| 1152 |
|
if (!initialized_) initialize(); |
| 1153 |
|
|
| 1154 |
< |
ElectrostaticAtomData data = ElectrostaticMap[sdat.atype]; |
| 1154 |
> |
ElectrostaticAtomData data = ElectrostaticMap[Etids[sdat.atid]]; |
| 1155 |
|
|
| 1156 |
|
// logicals |
| 1157 |
|
bool i_is_Charge = data.is_Charge; |