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1 : /* +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ 2 : Copyright (c) 2013-2023 The plumed team 3 : (see the PEOPLE file at the root of the distribution for a list of names) 4 : 5 : See http://www.plumed.org for more information. 6 : 7 : This file is part of plumed, version 2. 8 : 9 : plumed is free software: you can redistribute it and/or modify 10 : it under the terms of the GNU Lesser General Public License as published by 11 : the Free Software Foundation, either version 3 of the License, or 12 : (at your option) any later version. 13 : 14 : plumed is distributed in the hope that it will be useful, 15 : but WITHOUT ANY WARRANTY; without even the implied warranty of 16 : MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the 17 : GNU Lesser General Public License for more details. 18 : 19 : You should have received a copy of the GNU Lesser General Public License 20 : along with plumed. If not, see <http://www.gnu.org/licenses/>. 21 : +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ */ 22 : #include "CoordinationBase.h" 23 : #include "tools/SwitchingFunction.h" 24 : #include "core/ActionRegister.h" 25 : #include "core/PlumedMain.h" 26 : 27 : namespace PLMD { 28 : namespace colvar { 29 : 30 : //+PLUMEDOC COLVAR DHENERGY 31 : /* 32 : Calculate Debye-Huckel interaction energy among GROUPA and GROUPB. 33 : 34 : This variable calculates the electrostatic interaction among GROUPA and GROUPB 35 : using a Debye-Huckel approximation defined as 36 : \f[ 37 : \frac{1}{4\pi\epsilon_r\epsilon_0} 38 : \sum_{i\in A} \sum_{j \in B} q_i q_j 39 : \frac{e^{-\kappa |{\bf r}_{ij}|}}{|{\bf r}_{ij}|} 40 : \f] 41 : 42 : This collective variable can be used to analyze or induce electrostatically driven reactions \cite do13jctc. 43 : Notice that the value of the DHENERGY is returned in plumed units (see \ref UNITS). 44 : 45 : If GROUPB is empty, it will sum the N*(N-1)/2 pairs in GROUPA. This avoids computing 46 : twice permuted indexes (e.g. pair (i,j) and (j,i)) thus running at twice the speed. 47 : 48 : Notice that if there are common atoms between GROUPA and GROUPB their interaction is discarded. 49 : 50 : 51 : \par Examples 52 : 53 : \plumedfile 54 : # this is printing the electrostatic interaction between two groups of atoms 55 : dh: DHENERGY GROUPA=1-10 GROUPB=11-20 EPSILON=80.0 I=0.1 TEMP=300.0 56 : PRINT ARG=dh 57 : \endplumedfile 58 : 59 : */ 60 : //+ENDPLUMEDOC 61 : 62 : class DHEnergy : public CoordinationBase { 63 : double k; // Inverse Debye screening length 64 : double constant; 65 : double epsilon; 66 : 67 : public: 68 : explicit DHEnergy(const ActionOptions&); 69 : // active methods: 70 : static void registerKeywords( Keywords& keys ); 71 : double pairing(double distance,double&dfunc,unsigned i,unsigned j)const override; 72 : }; 73 : 74 : PLUMED_REGISTER_ACTION(DHEnergy,"DHENERGY") 75 : 76 10 : void DHEnergy::registerKeywords( Keywords& keys ) { 77 10 : CoordinationBase::registerKeywords(keys); 78 20 : keys.add("compulsory","I","1.0","Ionic strength (M)"); 79 20 : keys.add("compulsory","TEMP","300.0","Simulation temperature (K)"); 80 20 : keys.add("compulsory","EPSILON","80.0","Dielectric constant of solvent"); 81 20 : keys.setValueDescription("scalar","the value of the DHENERGY"); 82 10 : } 83 : 84 : /* 85 : Global constants in SI unit used in this calculation: 86 : N_A = 6.0221412927 * 10^(23) mol^(-1) : Avogadro number 87 : q = 1.60217656535 * 10^(-19) C : proton charge 88 : e_0 = 8.854187817620 * 10^(-12) C^2/(N*m^2) : vacuum's dielectric constant 89 : k_B = 1.380648813 * 10^(-23) N*m/K : Boltzmann constant 90 : In SI unit, Debye Huckel CV is defined as: 91 : DHen = \sum_i\sum_j (q_i*q_j*q^2*N_A)/(4*pi*eps*e_0) * exp(-k*|f_ij|)/(|f_ij|) 92 : + \sum_i\sum_j (q_i*q_j*q^2*N_A)/(4*pi*epp*e_0) * (1/|r_ij| - 1/|f_ij|) 93 : = (q^2*N_A)/(4*pi*e_0) * \sum_i\sum_j q_i*q_j * (exp(-k*|f_ij|)/(eps*|f_ij|) + 1/epp*(1/|r_ij| - 1/|f_ij|)) 94 : (in which |f_ij| = \sqrt(|r_ij|^2+\sigma_i*\sigma_j*exp(-|r_ij|^2/4*\sigma_i*\sigma_j)), 95 : \sigma_i and \sigma_j are the effective Born radius.) 96 : For an efficient calculation, we group constants and variables into groups: 97 : constant = (q^2*N_A)/(4*pi*e_0) 98 : tmp = 1/eps*exp(-k*|f_ij|)/(|f_ij|) + 1/epp*(1/|r_ij| - 1/|f_ij|) 99 : 100 : To speed up the loop calculation, constant can be modified as followed: 101 : constant= (q^2*N_A)/(4*pi*e_0*10^(-9))*10^(-3) (kJ/mol) 102 : = ((1.60217656535*10^(-19))^2*6.0221412927*10^(23)*10^(-3))/(4*3.14159265*8.854187817620*10^(-12)*10^(-9)) 103 : = 138.935458111 (kJ/mol) 104 : 105 : */ 106 : 107 8 : DHEnergy::DHEnergy(const ActionOptions&ao): 108 : Action(ao), 109 : CoordinationBase(ao), 110 8 : k(0.0), 111 8 : constant(0.0) 112 : { 113 : double I,T; 114 8 : parse("I",I); 115 8 : parse("TEMP",T); 116 8 : parse("EPSILON",epsilon); 117 8 : checkRead(); 118 8 : if( usingNaturalUnits() ) error("DHENERGY cannot be used for calculations performed with natural units"); 119 8 : constant=138.935458111/getUnits().getEnergy()/getUnits().getLength()*getUnits().getCharge()*getUnits().getCharge(); 120 8 : k=std::sqrt(I/(epsilon*T))*502.903741125*getUnits().getLength(); 121 8 : checkRead(); 122 8 : log<<" with solvent dielectric constant "<<epsilon<<"\n"; 123 8 : log<<" at temperature "<<T<<" K\n"; 124 8 : log<<" at ionic strength "<<I<< "M\n"; 125 8 : log<<" these parameters correspond to a screening length of "<<(1.0/k)<<"\n"; 126 16 : log<<" Bibliography "<<plumed.cite("Do, Carloni, Varani and Bussi, J. Chem. Theory Comput. 9, 1720 (2013)")<<" \n"; 127 8 : } 128 : 129 840 : double DHEnergy::pairing(double distance2,double&dfunc,unsigned i,unsigned j)const { 130 840 : double distance=std::sqrt(distance2); 131 840 : if(getAbsoluteIndex(i)==getAbsoluteIndex(j)) { 132 0 : dfunc=0.0; 133 0 : return 0.0; 134 : } 135 840 : double invdistance=1.0/distance; 136 840 : double tmp=std::exp(-k*distance)*invdistance*constant*getCharge(i)*getCharge(j)/epsilon; 137 840 : double dtmp=-(k+invdistance)*tmp; 138 840 : dfunc=dtmp*invdistance; 139 840 : return tmp; 140 : } 141 : 142 : } 143 : 144 : }