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/* |
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* Copyright (c) 2005 The University of Notre Dame. All Rights Reserved. |
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* |
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* The University of Notre Dame grants you ("Licensee") a |
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* non-exclusive, royalty free, license to use, modify and |
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* redistribute this software in source and binary code form, provided |
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* that the following conditions are met: |
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* |
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* 1. Redistributions of source code must retain the above copyright |
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* notice, this list of conditions and the following disclaimer. |
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* |
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* 2. Redistributions in binary form must reproduce the above copyright |
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* notice, this list of conditions and the following disclaimer in the |
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* documentation and/or other materials provided with the |
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* distribution. |
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* |
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* This software is provided "AS IS," without a warranty of any |
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* kind. All express or implied conditions, representations and |
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* warranties, including any implied warranty of merchantability, |
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* fitness for a particular purpose or non-infringement, are hereby |
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* excluded. The University of Notre Dame and its licensors shall not |
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* be liable for any damages suffered by licensee as a result of |
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* using, modifying or distributing the software or its |
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* derivatives. In no event will the University of Notre Dame or its |
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* licensors be liable for any lost revenue, profit or data, or for |
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* direct, indirect, special, consequential, incidental or punitive |
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* damages, however caused and regardless of the theory of liability, |
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* arising out of the use of or inability to use software, even if the |
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* University of Notre Dame has been advised of the possibility of |
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* such damages. |
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* |
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* SUPPORT OPEN SCIENCE! If you use OpenMD or its source code in your |
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* research, please cite the appropriate papers when you publish your |
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* work. Good starting points are: |
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* |
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* [1] Meineke, et al., J. Comp. Chem. 26, 252-271 (2005). |
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* [2] Fennell & Gezelter, J. Chem. Phys. 124, 234104 (2006). |
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* [3] Sun, Lin & Gezelter, J. Chem. Phys. 128, 24107 (2008). |
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* [4] Kuang & Gezelter, J. Chem. Phys. 133, 164101 (2010). |
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* [5] Vardeman, Stocker & Gezelter, J. Chem. Theory Comput. 7, 834 (2011). |
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*/ |
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|
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#include "brains/SimInfo.hpp" |
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#include "brains/Thermo.hpp" |
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#include "integrators/IntegratorCreator.hpp" |
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#include "integrators/NgammaT.hpp" |
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#include "primitives/Molecule.hpp" |
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#include "utils/PhysicalConstants.hpp" |
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#include "utils/simError.h" |
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|
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namespace OpenMD { |
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NgammaT::NgammaT(SimInfo* info) : NPT(info) { |
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Globals* simParams = info_->getSimParams(); |
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if (!simParams->haveSurfaceTension()) { |
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sprintf(painCave.errMsg, |
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"If you use the NgammaT integrator, you must set a surface tension.\n"); |
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painCave.severity = OPENMD_ERROR; |
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painCave.isFatal = 1; |
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simError(); |
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} else { |
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surfaceTension= simParams->getSurfaceTension()* PhysicalConstants::surfaceTensionConvert * PhysicalConstants::energyConvert; |
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} |
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|
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} |
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void NgammaT::evolveEtaA() { |
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Mat3x3d hmat = snap->getHmat(); |
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RealType hz = hmat(2, 2); |
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RealType Axy = hmat(0,0) * hmat(1, 1); |
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RealType sx = -hz * (press(0, 0) - targetPressure/PhysicalConstants::pressureConvert); |
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RealType sy = -hz * (press(1, 1) - targetPressure/PhysicalConstants::pressureConvert); |
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eta(0,0) -= dt2* Axy * (sx - surfaceTension) / (NkBT*tb2); |
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eta(1,1) -= dt2* Axy * (sy - surfaceTension) / (NkBT*tb2); |
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eta(2,2) = 0.0; |
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oldEta = eta; |
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} |
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|
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void NgammaT::evolveEtaB() { |
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Mat3x3d hmat = snap->getHmat(); |
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RealType hz = hmat(2, 2); |
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RealType Axy = hmat(0,0) * hmat(1, 1); |
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prevEta = eta; |
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RealType sx = -hz * (press(0, 0) - targetPressure/PhysicalConstants::pressureConvert); |
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RealType sy = -hz * (press(1, 1) - targetPressure/PhysicalConstants::pressureConvert); |
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eta(0,0) = oldEta(0, 0) - dt2 * Axy * (sx -surfaceTension) / (NkBT*tb2); |
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eta(1,1) = oldEta(1, 1) - dt2 * Axy * (sy -surfaceTension) / (NkBT*tb2); |
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eta(2,2) = 0.0; |
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} |
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|
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void NgammaT::calcVelScale(){ |
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|
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for (int i = 0; i < 3; i++ ) { |
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for (int j = 0; j < 3; j++ ) { |
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vScale(i, j) = eta(i, j); |
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|
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if (i == j) { |
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vScale(i, j) += thermostat.first; |
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} |
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} |
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} |
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} |
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|
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void NgammaT::getVelScaleA(Vector3d& sc, const Vector3d& vel){ |
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sc = vScale * vel; |
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} |
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|
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void NgammaT::getVelScaleB(Vector3d& sc, int index ) { |
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sc = vScale * oldVel[index]; |
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} |
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|
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void NgammaT::getPosScale(const Vector3d& pos, const Vector3d& COM, int index, Vector3d& sc) { |
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|
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/**@todo */ |
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Vector3d rj = (oldPos[index] + pos)/(RealType)2.0 -COM; |
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sc = eta * rj; |
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} |
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|
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void NgammaT::scaleSimBox(){ |
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Mat3x3d scaleMat; |
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|
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scaleMat(0, 0) = exp(dt*eta(0, 0)); |
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scaleMat(1, 1) = exp(dt*eta(1, 1)); |
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scaleMat(2, 2) = exp(dt*eta(2, 2)); |
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Mat3x3d hmat = snap->getHmat(); |
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hmat = hmat *scaleMat; |
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snap->setHmat(hmat); |
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|
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} |
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|
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bool NgammaT::etaConverged() { |
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int i; |
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RealType diffEta, sumEta; |
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|
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sumEta = 0; |
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for(i = 0; i < 3; i++) { |
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sumEta += pow(prevEta(i, i) - eta(i, i), 2); |
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} |
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|
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diffEta = sqrt( sumEta / 3.0 ); |
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|
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return ( diffEta <= etaTolerance ); |
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} |
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|
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RealType NgammaT::calcConservedQuantity(){ |
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|
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thermostat = snap->getThermostat(); |
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loadEta(); |
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|
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// We need NkBT a lot, so just set it here: This is the RAW number |
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// of integrableObjects, so no subtraction or addition of constraints or |
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// orientational degrees of freedom: |
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NkBT = info_->getNGlobalIntegrableObjects()*PhysicalConstants::kB *targetTemp; |
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|
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// fkBT is used because the thermostat operates on more degrees of freedom |
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// than the barostat (when there are particles with orientational degrees |
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// of freedom). |
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fkBT = info_->getNdf()*PhysicalConstants::kB *targetTemp; |
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|
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|
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RealType totalEnergy = thermo.getTotalEnergy(); |
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|
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RealType thermostat_kinetic = fkBT * tt2 * thermostat.first * |
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thermostat.first /(2.0 * PhysicalConstants::energyConvert); |
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|
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RealType thermostat_potential = fkBT* thermostat.second / PhysicalConstants::energyConvert; |
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|
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SquareMatrix<RealType, 3> tmp = eta.transpose() * eta; |
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RealType trEta = tmp.trace(); |
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|
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RealType barostat_kinetic = NkBT * tb2 * trEta /(2.0 * PhysicalConstants::energyConvert); |
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|
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RealType barostat_potential = (targetPressure * thermo.getVolume() / PhysicalConstants::pressureConvert) /PhysicalConstants::energyConvert; |
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Mat3x3d hmat = snap->getHmat(); |
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RealType hz = hmat(2, 2); |
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RealType area = hmat(0,0) * hmat(1, 1); |
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|
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RealType conservedQuantity = totalEnergy + thermostat_kinetic + thermostat_potential + |
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barostat_kinetic + barostat_potential - surfaceTension * area/ PhysicalConstants::energyConvert; |
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|
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return conservedQuantity; |
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|
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} |
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|
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void NgammaT::loadEta() { |
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eta= snap->getBarostat(); |
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|
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//if (!eta.isDiagonal()) { |
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// sprintf( painCave.errMsg, |
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// "NgammaT error: the diagonal elements of eta matrix are not the same or etaMat is not a diagonal matrix"); |
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// painCave.isFatal = 1; |
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// simError(); |
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//} |
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} |
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|
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void NgammaT::saveEta() { |
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snap->setBarostat(eta); |
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} |
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|
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} |
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|
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