[bd2278d] | 1 | ! **************************************************************
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| 2 | !
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| 3 | ! This file contains the subroutines: enyshe
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| 4 | !
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| 5 | ! Copyright 2003-2005 Frank Eisenmenger, U.H.E. Hansmann,
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| 6 | ! Shura Hayryan, Chin-Ku
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| 7 | ! Copyright 2007 Frank Eisenmenger, U.H.E. Hansmann,
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| 8 | ! Jan H. Meinke, Sandipan Mohanty
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| 9 | !
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| 10 | ! **************************************************************
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[e40e335] | 11 |
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| 12 |
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| 13 | real*8 function enyshe(nml)
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| 14 |
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[bd2278d] | 15 | ! ............................................................................
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| 16 | !
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| 17 | ! PURPOSE: Calculate internal energy of molecule 'nml' with ECEPP parameters
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| 18 | !
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| 19 | ! CALLS: none
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| 20 | !
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| 21 | ! The function loops over all moving sets within the molecule. Within
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| 22 | ! this loop it loops over the van-der-Waals domains of each atom in the
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| 23 | ! moving set and finally over the atoms that belong to the 1-4 interaction
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| 24 | ! set.
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| 25 | ! ............................................................................
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[e40e335] | 26 |
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| 27 | include 'INCL.H'
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| 28 |
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[bd2278d] | 29 | ! If nml == 0 calculate the interaction between all pairs.
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[e40e335] | 30 | if (nml.eq.0) then
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| 31 | ntlvr = nvr
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| 32 | else
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| 33 | ntlvr=nvrml(nml)
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| 34 | endif
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| 35 |
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| 36 | if (ntlvr.eq.0) then
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| 37 | write (*,'(a,i4)')
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[bd2278d] | 38 | & ' enyshe> No variables defined in molecule #',nml
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[e40e335] | 39 | return
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| 40 | endif
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| 41 |
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| 42 | enyshe=0.0
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| 43 | eyel=0.0
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| 44 | eyvw=0.0
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| 45 | eyhb=0.0
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| 46 | eyvr=0.0
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| 47 | if (nml.eq.0) then
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| 48 | ifivr = ivrml1(1)
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| 49 | i1s = imsml1(ntlml) + nmsml(ntlml)
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| 50 | else
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[bd2278d] | 51 | ! Index of first variable in molecule.
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[e40e335] | 52 | ifivr=ivrml1(nml)
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[bd2278d] | 53 | ! Index of last moving set in molecule
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[e40e335] | 54 | i1s=imsml1(nml)+nmsml(nml)
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| 55 | endif
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[bd2278d] | 56 | ! Loop over moving sets/variables in reverse order
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[e40e335] | 57 | do io=ifivr+ntlvr-1,ifivr,-1
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[bd2278d] | 58 | ! The array iorvr contains the variables in an "apropriate" order.
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[e40e335] | 59 | iv=iorvr(io)
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[bd2278d] | 60 | ! Index of the primary moving atom for the variable with index iv
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[e40e335] | 61 | ia=iatvr(iv)
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[bd2278d] | 62 | ! Get the type of variable iv (valence length, valence angle, dihedral angle)
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[e40e335] | 63 | it=ityvr(iv)
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[bd2278d] | 64 | ! Class of variable iv's potential (Q: What are they)
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[e40e335] | 65 | ic=iclvr(iv)
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[bd2278d] | 66 | ! If iv is a dihedral angle ...
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[e40e335] | 67 | if (it.eq.3) then
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[bd2278d] | 68 | ! Barrier height * 1/2 of the potential of iv.
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[e40e335] | 69 | e0=e0to(ic)
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[bd2278d] | 70 | ! Calculate the periodic potential term. sgto is the sign of the barrier, rnto is
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| 71 | ! the periodicity and toat is torsion angle(?) associate with atom ia.
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[e40e335] | 72 | if (e0.ne.0.)
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[bd2278d] | 73 | & eyvr=eyvr+e0*(1.0+sgto(ic)*cos(toat(ia)*rnto(ic)))
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| 74 | ! else if iv is a valence angle ...
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[e40e335] | 75 | elseif (it.eq.2) then
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[bd2278d] | 76 | ! vr is the valence angle of ia
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[e40e335] | 77 | vr=baat(ia)
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[bd2278d] | 78 | ! else if iv is a valence length...
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[e40e335] | 79 | elseif (it.eq.1) then
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[bd2278d] | 80 | ! vr is the length of the valence bond
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[e40e335] | 81 | vr=blat(ia)
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| 82 | endif
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| 83 |
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[bd2278d] | 84 | ! ============================================ Energies & Atomic forces
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| 85 | ! index of next to last moving set
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[e40e335] | 86 | i2s=i1s-1
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[bd2278d] | 87 | ! index of first moving set associated with iv
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[e40e335] | 88 | i1s=imsvr1(iv)
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[bd2278d] | 89 | ! Loop over all moving sets starting from the one associated with vr to the end.
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[e40e335] | 90 | do ims=i1s,i2s
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[bd2278d] | 91 | ! First atom of the current moving set
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[e40e335] | 92 | i1=latms1(ims)
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[bd2278d] | 93 | ! Last atom of the current moving set
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[e40e335] | 94 | i2=latms2(ims)
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[bd2278d] | 95 | ! Loop over all atoms of the current moving set.
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[e40e335] | 96 | do i=i1,i2
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[bd2278d] | 97 | ! Atom class of current atom
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[e40e335] | 98 | ity=ityat(i)
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[bd2278d] | 99 | ! Point charge at current atom
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[e40e335] | 100 | cqi=conv*cgat(i)
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[bd2278d] | 101 | ! Cartesian coordinates of current atom
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[e40e335] | 102 | xi=xat(i)
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| 103 | yi=yat(i)
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| 104 | zi=zat(i)
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[bd2278d] | 105 | ! Loop over the atoms of the van der Waals domain belonging to atom i
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[e40e335] | 106 | do ivw=ivwat1(i),ivwat2(i)
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[bd2278d] | 107 | ! Loop over the atoms of the van der Waals domain of the atoms of the
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| 108 | ! van der Waals domain of atom i
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| 109 | ! Q: Which atoms are in these domains?
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[e40e335] | 110 | do j=lvwat1(ivw),lvwat2(ivw)
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[bd2278d] | 111 | ! Atom type of partner
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[e40e335] | 112 | jty=ityat(j)
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[bd2278d] | 113 | ! Differences in cartesian coordinates
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[e40e335] | 114 | xij=xat(j)-xi
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| 115 | yij=yat(j)-yi
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| 116 | zij=zat(j)-zi
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[bd2278d] | 117 | ! Cartesian distance and higher powers
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[e40e335] | 118 | rij2=xij*xij+yij*yij+zij*zij
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| 119 | rij4=rij2*rij2
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| 120 | rij6=rij4*rij2
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| 121 | rij=sqrt(rij2)
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[bd2278d] | 122 | ! Are we using a distance dependent dielectric constant?
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[e40e335] | 123 | if(epsd) then
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| 124 | sr=slp*rij
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| 125 | ep=plt-(sr*sr+2.0*sr+2.0)*(plt-1.0)*exp(-sr)/2.0
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| 126 | else
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| 127 | ep = 1.0d0
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| 128 | end if
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[bd2278d] | 129 | ! Coulomb interaction
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[e40e335] | 130 | eyel=eyel+cqi*cgat(j)/(rij*ep)
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[bd2278d] | 131 | ! If the two atoms cannot form a hydrogen bond use 6-12 Lennard-Jones potential
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[e40e335] | 132 | if (ihbty(ity,jty).eq.0) then
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| 133 | eyvw=eyvw+aij(ity,jty)/(rij6*rij6)
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[bd2278d] | 134 | & -cij(ity,jty)/rij6
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[e40e335] | 135 | else
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[bd2278d] | 136 | ! For hydrogen bonding use 10-12 Lennard-Jones potential
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[e40e335] | 137 | eyhb=eyhb+ahb(ity,jty)/(rij6*rij6)
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[bd2278d] | 138 | & -chb(ity,jty)/(rij6*rij4)
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[e40e335] | 139 | endif
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| 140 |
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| 141 | enddo
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| 142 | enddo
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| 143 |
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[bd2278d] | 144 | ! Loop over 1-4 interaction partners
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| 145 | ! The interactions between atoms that are three bonds apart in the protein are
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| 146 | ! dominated by quantum mechanical effects. They are treated separately.
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[e40e335] | 147 | do i14=i14at1(i),i14at2(i)
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| 148 | j=l14at(i14)
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| 149 |
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| 150 | jty=ityat(j)
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| 151 |
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| 152 | xij=xat(j)-xi
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| 153 | yij=yat(j)-yi
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| 154 | zij=zat(j)-zi
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| 155 | rij2=xij*xij+yij*yij+zij*zij
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| 156 | rij4=rij2*rij2
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| 157 | rij6=rij4*rij2
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| 158 | rij = sqrt(rij2)
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[bd2278d] | 159 | ! Are we using a distance dependent dielectric constant?
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[e40e335] | 160 | if(epsd) then
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| 161 | sr=slp*rij
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| 162 | ep=plt-(sr*sr+2.0*sr+2.0)*(plt-1.0)*exp(-sr)/2.0
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| 163 | else
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| 164 | ep=1.0d0
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| 165 | end if
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| 166 |
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| 167 | eyel=eyel+cqi*cgat(j)/(rij*ep)
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[bd2278d] | 168 | ! If hydrogen bonding is not possible use 6-12 Lennard-Jones potential.
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[e40e335] | 169 | if (ihbty(ity,jty).eq.0) then
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| 170 | eyvw=eyvw+a14(ity,jty)/(rij6*rij6)
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[bd2278d] | 171 | & -cij(ity,jty)/rij6
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[e40e335] | 172 | else
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[bd2278d] | 173 | ! Use 10-12 Lennard-Jones potential for hydrogen bonds.
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[e40e335] | 174 | eyhb=eyhb+ahb(ity,jty)/(rij6*rij6)
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[bd2278d] | 175 | & -chb(ity,jty)/(rij6*rij4)
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[e40e335] | 176 | endif
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| 177 |
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| 178 | enddo ! ... 1-4-partners of i
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| 179 |
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| 180 | enddo ! ... atoms i
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| 181 | enddo ! ... m.s.
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| 182 |
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| 183 | enddo ! ... variables
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| 184 |
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| 185 | eysm = eyel + eyvw + eyhb + eyvr
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| 186 |
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| 187 | enyshe=eysm
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| 188 | return
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| 189 | end
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| 190 |
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