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#include "utils/simError.h" |
48 |
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#include "types/NonBondedInteractionType.hpp" |
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#include "types/DirectionalAtomType.hpp" |
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#include "io/Globals.hpp" |
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52 |
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namespace OpenMD { |
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Electrostatic::Electrostatic(): name_("Electrostatic"), initialized_(false), |
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forceField_(NULL), info_(NULL) {} |
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forceField_(NULL) {} |
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void Electrostatic::initialize() { |
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59 |
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Globals* simParams_; |
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summationMap_["HARD"] = esm_HARD; |
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summationMap_["SWITCHING_FUNCTION"] = esm_SWITCHING_FUNCTION; |
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} else { |
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// throw error |
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sprintf( painCave.errMsg, |
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"SimInfo error: Unknown electrostaticSummationMethod.\n" |
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"Electrostatic::initialize: Unknown electrostaticSummationMethod.\n" |
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"\t(Input file specified %s .)\n" |
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"\telectrostaticSummationMethod must be one of: \"none\",\n" |
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"\t\"shifted_potential\", \"shifted_force\", or \n" |
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haveDielectric_ = true; |
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} |
431 |
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432 |
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void Electrostatic::calcForce(InteractionData idat) { |
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void Electrostatic::calcForce(InteractionData &idat) { |
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// utility variables. Should clean these up and use the Vector3d and |
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// Mat3x3d to replace as many as we can in future versions: |
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} |
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594 |
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idat.vpair += vterm; |
594 |
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idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
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dVdr += dudr * rhat; |
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ri3 = ri2 * riji; |
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vterm = - pref * ct_j * ( ri2 - preRF2_ * idat.rij ); |
610 |
< |
idat.vpair += vterm; |
610 |
> |
idat.vpair[2] += vterm; |
611 |
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epot += idat.sw * vterm; |
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dVdr += -preSw * (ri3 * (uz_j - 3.0 * ct_j * rhat) - preRF2_*uz_j); |
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// calculate the potential |
646 |
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pot_term = scale * c2; |
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vterm = -pref * ct_j * pot_term; |
648 |
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idat.vpair += vterm; |
648 |
> |
idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
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|
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// calculate derivatives for forces and torques |
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qyy_j * (cy2*c3 - c2ri) + |
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qzz_j * (cz2*c3 - c2ri) ); |
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vterm = pref * pot_term; |
695 |
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idat.vpair += vterm; |
695 |
> |
idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
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|
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// calculate derivatives for the forces and torques |
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ri3 = ri2 * riji; |
721 |
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722 |
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vterm = pref * ct_i * ( ri2 - preRF2_ * idat.rij ); |
723 |
< |
idat.vpair += vterm; |
723 |
> |
idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
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|
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dVdr += preSw * (ri3 * (uz_i - 3.0 * ct_i * rhat) - preRF2_ * uz_i); |
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// calculate the potential |
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pot_term = c2 * scale; |
762 |
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vterm = pref * ct_i * pot_term; |
763 |
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idat.vpair += vterm; |
763 |
> |
idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
765 |
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|
766 |
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// calculate derivatives for the forces and torques |
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|
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vterm = pref * ( ri3 * (ct_ij - 3.0 * ct_i * ct_j) - |
785 |
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preRF2_ * ct_ij ); |
786 |
< |
idat.vpair += vterm; |
786 |
> |
idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
788 |
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|
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a1 = 5.0 * ct_i * ct_j - ct_ij; |
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// calculate the potential |
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pot_term = (ct_ij * c2ri - ctidotj * c3); |
844 |
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vterm = pref * pot_term; |
845 |
< |
idat.vpair += vterm; |
845 |
> |
idat.vpair[2] += vterm; |
846 |
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epot += idat.sw * vterm; |
847 |
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|
848 |
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// calculate derivatives for the forces and torques |
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qzz_i * (cz2 * c3 - c2ri) ); |
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|
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vterm = pref * pot_term; |
897 |
< |
idat.vpair += vterm; |
897 |
> |
idat.vpair[2] += vterm; |
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epot += idat.sw * vterm; |
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// calculate the derivatives for the forces and torques |
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} |
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} |
911 |
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912 |
< |
idat.pot += epot; |
912 |
> |
idat.pot[2] += epot; |
913 |
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idat.f1 += dVdr; |
914 |
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915 |
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if (i_is_Dipole || i_is_Quadrupole) |
929 |
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return; |
930 |
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} |
931 |
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932 |
< |
void Electrostatic::calcSkipCorrection(SkipCorrectionData skdat) { |
932 |
> |
void Electrostatic::calcSkipCorrection(SkipCorrectionData &skdat) { |
933 |
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934 |
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if (!initialized_) initialize(); |
935 |
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963 |
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964 |
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if (summationMethod_ == esm_REACTION_FIELD) { |
965 |
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RealType riji, ri2, ri3; |
966 |
< |
RealType q_i, mu_i, ct_i; |
967 |
< |
RealType q_j, mu_j, ct_j; |
968 |
< |
RealType preVal, rfVal, vterm, dudr, pref, myPot; |
966 |
> |
RealType mu_i, ct_i; |
967 |
> |
RealType mu_j, ct_j; |
968 |
> |
RealType preVal, rfVal, vterm, dudr, pref, myPot(0.0); |
969 |
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Vector3d dVdr, uz_i, uz_j, duduz_i, duduz_j, rhat; |
970 |
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|
971 |
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// some variables we'll need independent of electrostatic type: |
1020 |
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} |
1021 |
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1022 |
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// accumulate the forces and torques resulting from the self term |
1023 |
< |
skdat.pot += myPot; |
1023 |
> |
skdat.pot[2] += myPot; |
1024 |
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skdat.f1 += dVdr; |
1025 |
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|
1026 |
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if (i_is_Dipole) |
1030 |
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} |
1031 |
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} |
1032 |
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|
1033 |
< |
void Electrostatic::calcSelfCorrection(SelfCorrectionData scdat) { |
1033 |
> |
void Electrostatic::calcSelfCorrection(SelfCorrectionData &scdat) { |
1034 |
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RealType mu1, preVal, chg1, self; |
1035 |
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|
1036 |
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if (!initialized_) initialize(); |
1046 |
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if (i_is_Dipole) { |
1047 |
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mu1 = data.dipole_moment; |
1048 |
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preVal = pre22_ * preRF2_ * mu1 * mu1; |
1049 |
< |
scdat.pot -= 0.5 * preVal; |
1049 |
> |
scdat.pot[2] -= 0.5 * preVal; |
1050 |
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|
1051 |
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// The self-correction term adds into the reaction field vector |
1052 |
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Vector3d uz_i = scdat.eFrame.getColumn(2); |
1063 |
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} else { |
1064 |
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self = - 0.5 * rcuti_ * chg1 * (chg1 + scdat.skippedCharge) * pre11_; |
1065 |
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} |
1066 |
< |
scdat.pot += self; |
1066 |
> |
scdat.pot[2] += self; |
1067 |
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} |
1068 |
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} |
1069 |
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} |