1 |
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#include <cmath> |
2 |
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#include "Atom.hpp" |
3 |
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#include "SRI.hpp" |
4 |
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#include "AbstractClasses.hpp" |
20 |
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// |
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// Hoover, W. G., 1986, Phys. Rev. A, 34, 2499. |
22 |
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|
23 |
< |
NPTf::NPTf ( SimInfo *theInfo, ForceFields* the_ff): |
24 |
< |
Integrator( theInfo, the_ff ) |
23 |
> |
template<typename T> NPTf<T>::NPTf ( SimInfo *theInfo, ForceFields* the_ff): |
24 |
> |
T( theInfo, the_ff ) |
25 |
|
{ |
26 |
< |
int i; |
26 |
> |
int i, j; |
27 |
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chi = 0.0; |
28 |
< |
for(i = 0; i < 9; i++) eta[i] = 0.0; |
28 |
> |
integralOfChidt = 0.0; |
29 |
> |
|
30 |
> |
for(i = 0; i < 3; i++) |
31 |
> |
for (j = 0; j < 3; j++) |
32 |
> |
eta[i][j] = 0.0; |
33 |
> |
|
34 |
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have_tau_thermostat = 0; |
35 |
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have_tau_barostat = 0; |
36 |
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have_target_temp = 0; |
37 |
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have_target_pressure = 0; |
38 |
+ |
|
39 |
+ |
have_chi_tolerance = 0; |
40 |
+ |
have_eta_tolerance = 0; |
41 |
+ |
have_pos_iter_tolerance = 0; |
42 |
+ |
|
43 |
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oldPos = new double[3*nAtoms]; |
44 |
+ |
oldVel = new double[3*nAtoms]; |
45 |
+ |
oldJi = new double[3*nAtoms]; |
46 |
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#ifdef IS_MPI |
47 |
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Nparticles = mpiSim->getTotAtoms(); |
48 |
+ |
#else |
49 |
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Nparticles = theInfo->n_atoms; |
50 |
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#endif |
51 |
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} |
52 |
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|
53 |
< |
void NPTf::moveA() { |
53 |
> |
template<typename T> NPTf<T>::~NPTf() { |
54 |
> |
delete[] oldPos; |
55 |
> |
delete[] oldVel; |
56 |
> |
delete[] oldJi; |
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> |
} |
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|
59 |
> |
template<typename T> void NPTf<T>::moveA() { |
60 |
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|
61 |
< |
int i,j,k; |
37 |
< |
int atomIndex, aMatIndex; |
61 |
> |
int i, j, k; |
62 |
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DirectionalAtom* dAtom; |
63 |
< |
double Tb[3]; |
64 |
< |
double ji[3]; |
63 |
> |
double Tb[3], ji[3]; |
64 |
> |
double A[3][3], I[3][3]; |
65 |
> |
double angle, mass; |
66 |
> |
double vel[3], pos[3], frc[3]; |
67 |
> |
|
68 |
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double rj[3]; |
42 |
– |
double ident[3][3], eta1[3][3], eta2[3][3], hmnew[3][3]; |
43 |
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double hm[9]; |
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double vx, vy, vz; |
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double scx, scy, scz; |
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double instaTemp, instaPress, instaVol; |
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double tt2, tb2; |
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double angle; |
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double press[9]; |
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const double p_convert = 1.63882576e8; |
71 |
> |
double sc[3]; |
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> |
double eta2ij; |
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> |
double press[3][3], vScale[3][3], hm[3][3], hmnew[3][3], scaleMat[3][3]; |
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double bigScale, smallScale, offDiagMax; |
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> |
double COM[3]; |
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|
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tt2 = tauThermostat * tauThermostat; |
78 |
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tb2 = tauBarostat * tauBarostat; |
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|
80 |
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instaTemp = tStats->getTemperature(); |
81 |
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tStats->getPressureTensor(press); |
57 |
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|
58 |
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for (i=0; i < 9; i++) press[i] *= p_convert; |
59 |
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|
82 |
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instaVol = tStats->getVolume(); |
61 |
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|
62 |
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// first evolve chi a half step |
83 |
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|
84 |
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chi += dt2 * ( instaTemp / targetTemp - 1.0) / tt2; |
84 |
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tStats->getCOM(COM); |
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|
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//calculate scale factor of veloity |
87 |
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for (i = 0; i < 3; i++ ) { |
88 |
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for (j = 0; j < 3; j++ ) { |
89 |
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vScale[i][j] = eta[i][j]; |
90 |
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|
91 |
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if (i == j) { |
92 |
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vScale[i][j] += chi; |
93 |
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} |
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} |
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} |
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|
97 |
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eta[0] += dt2 * instaVol * (press[0] - targetPressure) / (NkBT*tb2); |
67 |
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eta[1] += dt2 * instaVol * press[1] / (NkBT*tb2); |
68 |
< |
eta[2] += dt2 * instaVol * press[2] / (NkBT*tb2); |
69 |
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eta[3] += dt2 * instaVol * press[3] / (NkBT*tb2); |
70 |
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eta[4] += dt2 * instaVol * (press[4] - targetPressure) / (NkBT*tb2); |
71 |
< |
eta[5] += dt2 * instaVol * press[5] / (NkBT*tb2); |
72 |
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eta[6] += dt2 * instaVol * press[6] / (NkBT*tb2); |
73 |
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eta[7] += dt2 * instaVol * press[7] / (NkBT*tb2); |
74 |
< |
eta[8] += dt2 * instaVol * (press[8] - targetPressure) / (NkBT*tb2); |
75 |
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|
97 |
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//evolve velocity half step |
98 |
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for( i=0; i<nAtoms; i++ ){ |
77 |
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atomIndex = i * 3; |
78 |
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aMatIndex = i * 9; |
79 |
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|
80 |
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// velocity half step |
81 |
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|
82 |
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vx = vel[atomIndex]; |
83 |
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vy = vel[atomIndex+1]; |
84 |
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vz = vel[atomIndex+2]; |
85 |
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|
86 |
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scx = (chi + eta[0])*vx + eta[1]*vy + eta[2]*vz; |
87 |
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scy = eta[3]*vx + (chi + eta[4])*vy + eta[5]*vz; |
88 |
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scz = eta[6]*vx + eta[7]*vy + (chi + eta[8])*vz; |
89 |
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|
90 |
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vx += dt2 * ((frc[atomIndex] /atoms[i]->getMass())*eConvert - scx); |
91 |
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vy += dt2 * ((frc[atomIndex+1]/atoms[i]->getMass())*eConvert - scy); |
92 |
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vz += dt2 * ((frc[atomIndex+2]/atoms[i]->getMass())*eConvert - scz); |
99 |
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|
100 |
< |
vel[atomIndex] = vx; |
101 |
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vel[atomIndex+1] = vy; |
96 |
< |
vel[atomIndex+2] = vz; |
100 |
> |
atoms[i]->getVel( vel ); |
101 |
> |
atoms[i]->getFrc( frc ); |
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|
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// position whole step |
103 |
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mass = atoms[i]->getMass(); |
104 |
> |
|
105 |
> |
info->matVecMul3( vScale, vel, sc ); |
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|
107 |
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rj[0] = pos[atomIndex]; |
108 |
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rj[1] = pos[atomIndex+1]; |
109 |
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rj[2] = pos[atomIndex+2]; |
107 |
> |
for (j=0; j < 3; j++) { |
108 |
> |
// velocity half step (use chi from previous step here): |
109 |
> |
vel[j] += dt2 * ((frc[j] / mass) * eConvert - sc[j]); |
110 |
> |
|
111 |
> |
} |
112 |
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|
113 |
< |
info->wrapVector(rj); |
105 |
< |
|
106 |
< |
scx = eta[0]*rj[0] + eta[1]*rj[1] + eta[2]*rj[2]; |
107 |
< |
scy = eta[3]*rj[0] + eta[4]*rj[1] + eta[5]*rj[2]; |
108 |
< |
scz = eta[6]*rj[0] + eta[7]*rj[1] + eta[8]*rj[2]; |
109 |
< |
|
110 |
< |
pos[atomIndex] += dt * (vel[atomIndex] + scx); |
111 |
< |
pos[atomIndex+1] += dt * (vel[atomIndex+1] + scy); |
112 |
< |
pos[atomIndex+2] += dt * (vel[atomIndex+2] + scz); |
113 |
> |
atoms[i]->setVel( vel ); |
114 |
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|
115 |
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if( atoms[i]->isDirectional() ){ |
116 |
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|
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dAtom = (DirectionalAtom *)atoms[i]; |
118 |
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|
118 |
> |
|
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// get and convert the torque to body frame |
120 |
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|
121 |
< |
Tb[0] = dAtom->getTx(); |
121 |
< |
Tb[1] = dAtom->getTy(); |
122 |
< |
Tb[2] = dAtom->getTz(); |
123 |
< |
|
121 |
> |
dAtom->getTrq( Tb ); |
122 |
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dAtom->lab2Body( Tb ); |
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|
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// get the angular momentum, and propagate a half step |
125 |
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|
126 |
< |
ji[0] = dAtom->getJx(); |
127 |
< |
ji[1] = dAtom->getJy(); |
128 |
< |
ji[2] = dAtom->getJz(); |
126 |
> |
dAtom->getJ( ji ); |
127 |
> |
|
128 |
> |
for (j=0; j < 3; j++) |
129 |
> |
ji[j] += dt2 * (Tb[j] * eConvert - ji[j]*chi); |
130 |
|
|
132 |
– |
ji[0] += dt2 * (Tb[0] * eConvert - ji[0]*chi); |
133 |
– |
ji[1] += dt2 * (Tb[1] * eConvert - ji[1]*chi); |
134 |
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ji[2] += dt2 * (Tb[2] * eConvert - ji[2]*chi); |
135 |
– |
|
131 |
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// use the angular velocities to propagate the rotation matrix a |
132 |
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// full time step |
133 |
< |
|
133 |
> |
|
134 |
> |
dAtom->getA(A); |
135 |
> |
dAtom->getI(I); |
136 |
> |
|
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// rotate about the x-axis |
138 |
< |
angle = dt2 * ji[0] / dAtom->getIxx(); |
139 |
< |
this->rotate( 1, 2, angle, ji, &Amat[aMatIndex] ); |
140 |
< |
|
138 |
> |
angle = dt2 * ji[0] / I[0][0]; |
139 |
> |
this->rotate( 1, 2, angle, ji, A ); |
140 |
> |
|
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// rotate about the y-axis |
142 |
< |
angle = dt2 * ji[1] / dAtom->getIyy(); |
143 |
< |
this->rotate( 2, 0, angle, ji, &Amat[aMatIndex] ); |
142 |
> |
angle = dt2 * ji[1] / I[1][1]; |
143 |
> |
this->rotate( 2, 0, angle, ji, A ); |
144 |
|
|
145 |
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// rotate about the z-axis |
146 |
< |
angle = dt * ji[2] / dAtom->getIzz(); |
147 |
< |
this->rotate( 0, 1, angle, ji, &Amat[aMatIndex] ); |
146 |
> |
angle = dt * ji[2] / I[2][2]; |
147 |
> |
this->rotate( 0, 1, angle, ji, A); |
148 |
|
|
149 |
|
// rotate about the y-axis |
150 |
< |
angle = dt2 * ji[1] / dAtom->getIyy(); |
151 |
< |
this->rotate( 2, 0, angle, ji, &Amat[aMatIndex] ); |
150 |
> |
angle = dt2 * ji[1] / I[1][1]; |
151 |
> |
this->rotate( 2, 0, angle, ji, A ); |
152 |
|
|
153 |
|
// rotate about the x-axis |
154 |
< |
angle = dt2 * ji[0] / dAtom->getIxx(); |
155 |
< |
this->rotate( 1, 2, angle, ji, &Amat[aMatIndex] ); |
154 |
> |
angle = dt2 * ji[0] / I[0][0]; |
155 |
> |
this->rotate( 1, 2, angle, ji, A ); |
156 |
|
|
157 |
< |
dAtom->setJx( ji[0] ); |
158 |
< |
dAtom->setJy( ji[1] ); |
159 |
< |
dAtom->setJz( ji[2] ); |
157 |
> |
dAtom->setJ( ji ); |
158 |
> |
dAtom->setA( A ); |
159 |
> |
} |
160 |
> |
} |
161 |
> |
|
162 |
> |
// advance chi half step |
163 |
> |
chi += dt2 * ( instaTemp / targetTemp - 1.0) / tt2; |
164 |
> |
|
165 |
> |
//calculate the integral of chidt |
166 |
> |
integralOfChidt += dt2*chi; |
167 |
> |
|
168 |
> |
//advance eta half step |
169 |
> |
for(i = 0; i < 3; i ++) |
170 |
> |
for(j = 0; j < 3; j++){ |
171 |
> |
if( i == j) |
172 |
> |
eta[i][j] += dt2 * instaVol * |
173 |
> |
(press[i][j] - targetPressure/p_convert) / (NkBT*tb2); |
174 |
> |
else |
175 |
> |
eta[i][j] += dt2 * instaVol * press[i][j] / ( NkBT*tb2); |
176 |
|
} |
177 |
|
|
178 |
+ |
//save the old positions |
179 |
+ |
for(i = 0; i < nAtoms; i++){ |
180 |
+ |
atoms[i]->getPos(pos); |
181 |
+ |
for(j = 0; j < 3; j++) |
182 |
+ |
oldPos[i*3 + j] = pos[j]; |
183 |
|
} |
184 |
+ |
|
185 |
+ |
//the first estimation of r(t+dt) is equal to r(t) |
186 |
+ |
|
187 |
+ |
for(k = 0; k < 4; k ++){ |
188 |
|
|
189 |
< |
// Scale the box after all the positions have been moved: |
189 |
> |
for(i =0 ; i < nAtoms; i++){ |
190 |
|
|
191 |
< |
// Use a taylor expansion for eta products: Hmat = Hmat . exp(dt * etaMat) |
192 |
< |
// Hmat = Hmat . ( Ident + dt * etaMat + dt^2 * etaMat*etaMat / 2) |
191 |
> |
atoms[i]->getVel(vel); |
192 |
> |
atoms[i]->getPos(pos); |
193 |
|
|
194 |
+ |
for(j = 0; j < 3; j++) |
195 |
+ |
rj[j] = (oldPos[i*3 + j] + pos[j])/2 - COM[j]; |
196 |
+ |
|
197 |
+ |
info->matVecMul3( eta, rj, sc ); |
198 |
+ |
|
199 |
+ |
for(j = 0; j < 3; j++) |
200 |
+ |
pos[j] = oldPos[i*3 + j] + dt*(vel[j] + sc[j]); |
201 |
|
|
202 |
< |
for(i=0; i<3; i++){ |
203 |
< |
for(j=0; j<3; j++){ |
174 |
< |
ident[i][j] = 0.0; |
175 |
< |
eta1[i][j] = eta[3*i+j]; |
176 |
< |
eta2[i][j] = 0.0; |
177 |
< |
for(k=0; k<3; k++){ |
178 |
< |
eta2[i][j] += eta[3*i+k] * eta[3*k+j]; |
179 |
< |
} |
202 |
> |
atoms[i]->setPos( pos ); |
203 |
> |
|
204 |
|
} |
181 |
– |
ident[i][i] = 1.0; |
182 |
– |
} |
205 |
|
|
206 |
< |
|
207 |
< |
info->getBoxM(hm); |
206 |
> |
} |
207 |
> |
|
208 |
|
|
209 |
+ |
// Scale the box after all the positions have been moved: |
210 |
+ |
|
211 |
+ |
// Use a taylor expansion for eta products: Hmat = Hmat . exp(dt * etaMat) |
212 |
+ |
// Hmat = Hmat . ( Ident + dt * etaMat + dt^2 * etaMat*etaMat / 2) |
213 |
+ |
|
214 |
+ |
bigScale = 1.0; |
215 |
+ |
smallScale = 1.0; |
216 |
+ |
offDiagMax = 0.0; |
217 |
+ |
|
218 |
|
for(i=0; i<3; i++){ |
219 |
< |
for(j=0; j<3; j++){ |
220 |
< |
hmnew[i][j] = 0.0; |
219 |
> |
for(j=0; j<3; j++){ |
220 |
> |
|
221 |
> |
// Calculate the matrix Product of the eta array (we only need |
222 |
> |
// the ij element right now): |
223 |
> |
|
224 |
> |
eta2ij = 0.0; |
225 |
|
for(k=0; k<3; k++){ |
226 |
< |
// remember that hmat has transpose ordering for Fortran compat: |
192 |
< |
hmnew[i][j] += hm[3*k+i] * (ident[k][j] |
193 |
< |
+ dt * eta1[k][j] |
194 |
< |
+ 0.5 * dt * dt * eta2[k][j]); |
226 |
> |
eta2ij += eta[i][k] * eta[k][j]; |
227 |
|
} |
228 |
+ |
|
229 |
+ |
scaleMat[i][j] = 0.0; |
230 |
+ |
// identity matrix (see above): |
231 |
+ |
if (i == j) scaleMat[i][j] = 1.0; |
232 |
+ |
// Taylor expansion for the exponential truncated at second order: |
233 |
+ |
scaleMat[i][j] += dt*eta[i][j] + 0.5*dt*dt*eta2ij; |
234 |
+ |
|
235 |
+ |
if (i != j) |
236 |
+ |
if (fabs(scaleMat[i][j]) > offDiagMax) |
237 |
+ |
offDiagMax = fabs(scaleMat[i][j]); |
238 |
|
} |
239 |
+ |
|
240 |
+ |
if (scaleMat[i][i] > bigScale) bigScale = scaleMat[i][i]; |
241 |
+ |
if (scaleMat[i][i] < smallScale) smallScale = scaleMat[i][i]; |
242 |
|
} |
243 |
|
|
244 |
< |
for (i = 0; i < 3; i++) { |
245 |
< |
for (j = 0; j < 3; j++) { |
246 |
< |
// remember that hmat has transpose ordering for Fortran compat: |
247 |
< |
hm[3*j + 1] = hmnew[i][j]; |
248 |
< |
} |
244 |
> |
if ((bigScale > 1.1) || (smallScale < 0.9)) { |
245 |
> |
sprintf( painCave.errMsg, |
246 |
> |
"NPTf error: Attempting a Box scaling of more than 10 percent.\n" |
247 |
> |
" Check your tauBarostat, as it is probably too small!\n\n" |
248 |
> |
" scaleMat = [%lf\t%lf\t%lf]\n" |
249 |
> |
" [%lf\t%lf\t%lf]\n" |
250 |
> |
" [%lf\t%lf\t%lf]\n", |
251 |
> |
scaleMat[0][0],scaleMat[0][1],scaleMat[0][2], |
252 |
> |
scaleMat[1][0],scaleMat[1][1],scaleMat[1][2], |
253 |
> |
scaleMat[2][0],scaleMat[2][1],scaleMat[2][2]); |
254 |
> |
painCave.isFatal = 1; |
255 |
> |
simError(); |
256 |
> |
} else if (offDiagMax > 0.1) { |
257 |
> |
sprintf( painCave.errMsg, |
258 |
> |
"NPTf error: Attempting an off-diagonal Box scaling of more than 10 percent.\n" |
259 |
> |
" Check your tauBarostat, as it is probably too small!\n\n" |
260 |
> |
" scaleMat = [%lf\t%lf\t%lf]\n" |
261 |
> |
" [%lf\t%lf\t%lf]\n" |
262 |
> |
" [%lf\t%lf\t%lf]\n", |
263 |
> |
scaleMat[0][0],scaleMat[0][1],scaleMat[0][2], |
264 |
> |
scaleMat[1][0],scaleMat[1][1],scaleMat[1][2], |
265 |
> |
scaleMat[2][0],scaleMat[2][1],scaleMat[2][2]); |
266 |
> |
painCave.isFatal = 1; |
267 |
> |
simError(); |
268 |
> |
} else { |
269 |
> |
info->getBoxM(hm); |
270 |
> |
info->matMul3(hm, scaleMat, hmnew); |
271 |
> |
info->setBoxM(hmnew); |
272 |
|
} |
205 |
– |
|
206 |
– |
info->setBoxM(hm); |
273 |
|
|
274 |
|
} |
275 |
|
|
276 |
< |
void NPTf::moveB( void ){ |
277 |
< |
int i,j,k; |
278 |
< |
int atomIndex; |
276 |
> |
template<typename T> void NPTf<T>::moveB( void ){ |
277 |
> |
|
278 |
> |
int i, j, k; |
279 |
|
DirectionalAtom* dAtom; |
280 |
< |
double Tb[3]; |
281 |
< |
double ji[3]; |
282 |
< |
double press[9]; |
283 |
< |
double instaTemp, instaVol; |
280 |
> |
double Tb[3], ji[3]; |
281 |
> |
double vel[3], frc[3]; |
282 |
> |
double mass; |
283 |
> |
|
284 |
> |
double instaTemp, instaPress, instaVol; |
285 |
|
double tt2, tb2; |
286 |
< |
double vx, vy, vz; |
287 |
< |
double scx, scy, scz; |
288 |
< |
const double p_convert = 1.63882576e8; |
286 |
> |
double sc[3]; |
287 |
> |
double press[3][3], vScale[3][3]; |
288 |
> |
double oldChi, prevChi; |
289 |
> |
double oldEta[3][3], preEta[3][3], diffEta; |
290 |
|
|
291 |
|
tt2 = tauThermostat * tauThermostat; |
292 |
|
tb2 = tauBarostat * tauBarostat; |
293 |
|
|
226 |
– |
instaTemp = tStats->getTemperature(); |
227 |
– |
tStats->getPressureTensor(press); |
294 |
|
|
295 |
< |
for (i=0; i < 9; i++) press[i] *= p_convert; |
295 |
> |
// Set things up for the iteration: |
296 |
|
|
297 |
< |
instaVol = tStats->getVolume(); |
232 |
< |
|
233 |
< |
// first evolve chi a half step |
297 |
> |
oldChi = chi; |
298 |
|
|
299 |
< |
chi += dt2 * ( instaTemp / targetTemp - 1.0) / tt2; |
300 |
< |
|
301 |
< |
eta[0] += dt2 * instaVol * (press[0] - targetPressure) / (NkBT*tb2); |
238 |
< |
eta[1] += dt2 * instaVol * press[1] / (NkBT*tb2); |
239 |
< |
eta[2] += dt2 * instaVol * press[2] / (NkBT*tb2); |
240 |
< |
eta[3] += dt2 * instaVol * press[3] / (NkBT*tb2); |
241 |
< |
eta[4] += dt2 * instaVol * (press[4] - targetPressure) / (NkBT*tb2); |
242 |
< |
eta[5] += dt2 * instaVol * press[5] / (NkBT*tb2); |
243 |
< |
eta[6] += dt2 * instaVol * press[6] / (NkBT*tb2); |
244 |
< |
eta[7] += dt2 * instaVol * press[7] / (NkBT*tb2); |
245 |
< |
eta[8] += dt2 * instaVol * (press[8] - targetPressure) / (NkBT*tb2); |
299 |
> |
for(i = 0; i < 3; i++) |
300 |
> |
for(j = 0; j < 3; j++) |
301 |
> |
oldEta[i][j] = eta[i][j]; |
302 |
|
|
303 |
|
for( i=0; i<nAtoms; i++ ){ |
248 |
– |
atomIndex = i * 3; |
304 |
|
|
305 |
< |
// velocity half step |
305 |
> |
atoms[i]->getVel( vel ); |
306 |
> |
|
307 |
> |
for (j=0; j < 3; j++) |
308 |
> |
oldVel[3*i + j] = vel[j]; |
309 |
> |
|
310 |
> |
if( atoms[i]->isDirectional() ){ |
311 |
> |
|
312 |
> |
dAtom = (DirectionalAtom *)atoms[i]; |
313 |
> |
|
314 |
> |
dAtom->getJ( ji ); |
315 |
> |
|
316 |
> |
for (j=0; j < 3; j++) |
317 |
> |
oldJi[3*i + j] = ji[j]; |
318 |
> |
|
319 |
> |
} |
320 |
> |
} |
321 |
> |
|
322 |
> |
// do the iteration: |
323 |
> |
|
324 |
> |
instaVol = tStats->getVolume(); |
325 |
> |
|
326 |
> |
for (k=0; k < 4; k++) { |
327 |
|
|
328 |
< |
vx = vel[atomIndex]; |
329 |
< |
vy = vel[atomIndex+1]; |
254 |
< |
vz = vel[atomIndex+2]; |
255 |
< |
|
256 |
< |
scx = (chi + eta[0])*vx + eta[1]*vy + eta[2]*vz; |
257 |
< |
scy = eta[3]*vx + (chi + eta[4])*vy + eta[5]*vz; |
258 |
< |
scz = eta[6]*vx + eta[7]*vy + (chi + eta[8])*vz; |
259 |
< |
|
260 |
< |
vx += dt2 * ((frc[atomIndex] /atoms[i]->getMass())*eConvert - scx); |
261 |
< |
vy += dt2 * ((frc[atomIndex+1]/atoms[i]->getMass())*eConvert - scy); |
262 |
< |
vz += dt2 * ((frc[atomIndex+2]/atoms[i]->getMass())*eConvert - scz); |
328 |
> |
instaTemp = tStats->getTemperature(); |
329 |
> |
tStats->getPressureTensor(press); |
330 |
|
|
331 |
< |
vel[atomIndex] = vx; |
332 |
< |
vel[atomIndex+1] = vy; |
333 |
< |
vel[atomIndex+2] = vz; |
331 |
> |
// evolve chi another half step using the temperature at t + dt/2 |
332 |
> |
|
333 |
> |
prevChi = chi; |
334 |
> |
chi = oldChi + dt2 * ( instaTemp / targetTemp - 1.0) / tt2; |
335 |
|
|
336 |
< |
if( atoms[i]->isDirectional() ){ |
336 |
> |
for(i = 0; i < 3; i++) |
337 |
> |
for(j = 0; j < 3; j++) |
338 |
> |
preEta[i][j] = eta[i][j]; |
339 |
> |
|
340 |
> |
//advance eta half step and calculate scale factor for velocity |
341 |
> |
for(i = 0; i < 3; i ++) |
342 |
> |
for(j = 0; j < 3; j++){ |
343 |
> |
if( i == j){ |
344 |
> |
eta[i][j] = oldEta[i][j] + dt2 * instaVol * |
345 |
> |
(press[i][j] - targetPressure/p_convert) / (NkBT*tb2); |
346 |
> |
vScale[i][j] = eta[i][j] + chi; |
347 |
> |
} |
348 |
> |
else |
349 |
> |
{ |
350 |
> |
eta[i][j] = oldEta[i][j] + dt2 * instaVol * press[i][j] / (NkBT*tb2); |
351 |
> |
vScale[i][j] = eta[i][j]; |
352 |
> |
} |
353 |
> |
} |
354 |
> |
|
355 |
> |
//advance velocity half step |
356 |
> |
for( i=0; i<nAtoms; i++ ){ |
357 |
> |
|
358 |
> |
atoms[i]->getFrc( frc ); |
359 |
> |
atoms[i]->getVel(vel); |
360 |
|
|
361 |
< |
dAtom = (DirectionalAtom *)atoms[i]; |
361 |
> |
mass = atoms[i]->getMass(); |
362 |
|
|
363 |
< |
// get and convert the torque to body frame |
363 |
> |
info->matVecMul3( vScale, vel, sc ); |
364 |
> |
|
365 |
> |
for (j=0; j < 3; j++) { |
366 |
> |
// velocity half step (use chi from previous step here): |
367 |
> |
vel[j] = oldVel[3*i+j] + dt2 * ((frc[j] / mass) * eConvert - sc[j]); |
368 |
> |
} |
369 |
|
|
370 |
< |
Tb[0] = dAtom->getTx(); |
275 |
< |
Tb[1] = dAtom->getTy(); |
276 |
< |
Tb[2] = dAtom->getTz(); |
370 |
> |
atoms[i]->setVel( vel ); |
371 |
|
|
372 |
< |
dAtom->lab2Body( Tb ); |
372 |
> |
if( atoms[i]->isDirectional() ){ |
373 |
> |
|
374 |
> |
dAtom = (DirectionalAtom *)atoms[i]; |
375 |
> |
|
376 |
> |
// get and convert the torque to body frame |
377 |
> |
|
378 |
> |
dAtom->getTrq( Tb ); |
379 |
> |
dAtom->lab2Body( Tb ); |
380 |
> |
|
381 |
> |
for (j=0; j < 3; j++) |
382 |
> |
ji[j] = oldJi[3*i + j] + dt2 * (Tb[j] * eConvert - oldJi[3*i+j]*chi); |
383 |
|
|
384 |
< |
// get the angular momentum, and complete the angular momentum |
385 |
< |
// half step |
282 |
< |
|
283 |
< |
ji[0] = dAtom->getJx(); |
284 |
< |
ji[1] = dAtom->getJy(); |
285 |
< |
ji[2] = dAtom->getJz(); |
286 |
< |
|
287 |
< |
ji[0] += dt2 * (Tb[0] * eConvert - ji[0]*chi); |
288 |
< |
ji[1] += dt2 * (Tb[1] * eConvert - ji[1]*chi); |
289 |
< |
ji[2] += dt2 * (Tb[2] * eConvert - ji[2]*chi); |
290 |
< |
|
291 |
< |
dAtom->setJx( ji[0] ); |
292 |
< |
dAtom->setJy( ji[1] ); |
293 |
< |
dAtom->setJz( ji[2] ); |
384 |
> |
dAtom->setJ( ji ); |
385 |
> |
} |
386 |
|
} |
387 |
+ |
|
388 |
+ |
|
389 |
+ |
diffEta = 0; |
390 |
+ |
for(i = 0; i < 3; i++) |
391 |
+ |
diffEta += pow(preEta[i][i] - eta[i][i], 2); |
392 |
+ |
|
393 |
+ |
if (fabs(prevChi - chi) <= chiTolerance && sqrt(diffEta / 3) <= etaTolerance) |
394 |
+ |
break; |
395 |
|
} |
396 |
+ |
|
397 |
+ |
//calculate integral of chida |
398 |
+ |
integralOfChidt += dt2*chi; |
399 |
+ |
|
400 |
+ |
|
401 |
|
} |
402 |
|
|
403 |
< |
int NPTi::readyCheck() { |
403 |
> |
template<typename T> void NPTf<T>::resetIntegrator() { |
404 |
> |
int i,j; |
405 |
> |
|
406 |
> |
chi = 0.0; |
407 |
> |
|
408 |
> |
for(i = 0; i < 3; i++) |
409 |
> |
for (j = 0; j < 3; j++) |
410 |
> |
eta[i][j] = 0.0; |
411 |
> |
|
412 |
> |
} |
413 |
> |
|
414 |
> |
template<typename T> int NPTf<T>::readyCheck() { |
415 |
> |
|
416 |
> |
//check parent's readyCheck() first |
417 |
> |
if (T::readyCheck() == -1) |
418 |
> |
return -1; |
419 |
|
|
420 |
|
// First check to see if we have a target temperature. |
421 |
|
// Not having one is fatal. |
422 |
|
|
423 |
|
if (!have_target_temp) { |
424 |
|
sprintf( painCave.errMsg, |
425 |
< |
"NPTi error: You can't use the NPTi integrator\n" |
425 |
> |
"NPTf error: You can't use the NPTf integrator\n" |
426 |
|
" without a targetTemp!\n" |
427 |
|
); |
428 |
|
painCave.isFatal = 1; |
432 |
|
|
433 |
|
if (!have_target_pressure) { |
434 |
|
sprintf( painCave.errMsg, |
435 |
< |
"NPTi error: You can't use the NPTi integrator\n" |
435 |
> |
"NPTf error: You can't use the NPTf integrator\n" |
436 |
|
" without a targetPressure!\n" |
437 |
|
); |
438 |
|
painCave.isFatal = 1; |
444 |
|
|
445 |
|
if (!have_tau_thermostat) { |
446 |
|
sprintf( painCave.errMsg, |
447 |
< |
"NPTi error: If you use the NPTi\n" |
447 |
> |
"NPTf error: If you use the NPTf\n" |
448 |
|
" integrator, you must set tauThermostat.\n"); |
449 |
|
painCave.isFatal = 1; |
450 |
|
simError(); |
455 |
|
|
456 |
|
if (!have_tau_barostat) { |
457 |
|
sprintf( painCave.errMsg, |
458 |
< |
"NPTi error: If you use the NPTi\n" |
458 |
> |
"NPTf error: If you use the NPTf\n" |
459 |
|
" integrator, you must set tauBarostat.\n"); |
460 |
|
painCave.isFatal = 1; |
461 |
|
simError(); |
464 |
|
|
465 |
|
// We need NkBT a lot, so just set it here: |
466 |
|
|
467 |
< |
NkBT = (double)info->ndf * kB * targetTemp; |
467 |
> |
NkBT = (double)Nparticles * kB * targetTemp; |
468 |
> |
fkBT = (double)info->ndf * kB * targetTemp; |
469 |
|
|
470 |
|
return 1; |
471 |
|
} |
472 |
+ |
|
473 |
+ |
template<typename T> double NPTf<T>::getConservedQuantity(void){ |
474 |
+ |
|
475 |
+ |
double conservedQuantity; |
476 |
+ |
double tb2; |
477 |
+ |
double trEta; |
478 |
+ |
double U; |
479 |
+ |
double thermo; |
480 |
+ |
double integral; |
481 |
+ |
double baro; |
482 |
+ |
double PV; |
483 |
+ |
|
484 |
+ |
U = tStats->getTotalE(); |
485 |
+ |
thermo = (fkBT * tauThermostat * tauThermostat * chi * chi / 2.0) / eConvert; |
486 |
+ |
|
487 |
+ |
tb2 = tauBarostat * tauBarostat; |
488 |
+ |
trEta = info->matTrace3(eta); |
489 |
+ |
baro = ((double)info->ndfTrans * kB * targetTemp * tb2 * trEta * trEta / 2.0) / eConvert; |
490 |
+ |
|
491 |
+ |
integral = ((double)(info->ndf + 1) * kB * targetTemp * integralOfChidt) /eConvert; |
492 |
+ |
|
493 |
+ |
PV = (targetPressure * tStats->getVolume() / p_convert) / eConvert; |
494 |
+ |
|
495 |
+ |
|
496 |
+ |
cout.width(8); |
497 |
+ |
cout.precision(8); |
498 |
+ |
|
499 |
+ |
cout << info->getTime() << "\t" |
500 |
+ |
<< chi << "\t" |
501 |
+ |
<< trEta << "\t" |
502 |
+ |
<< U << "\t" |
503 |
+ |
<< thermo << "\t" |
504 |
+ |
<< baro << "\t" |
505 |
+ |
<< integral << "\t" |
506 |
+ |
<< PV << "\t" |
507 |
+ |
<< U+thermo+integral+PV+baro << endl; |
508 |
+ |
|
509 |
+ |
conservedQuantity = U+thermo+integral+PV+baro; |
510 |
+ |
return conservedQuantity; |
511 |
+ |
|
512 |
+ |
} |