Ord Hermes1DFunction<Scalar>::value(Ord x) const
{
if (this->is_const)
return Ord(0);
else
{
throw Hermes::Exceptions::MethodNotOverridenException("Hermes1DFunction<Scalar>::value");
return Ord(99);
}
};
Ord Hermes3DFunction<Scalar>::derivative_z(Ord x, Ord y, Ord z) const
{
if (this->is_const)
return Ord(0);
else
{
throw Hermes::Exceptions::MethodNotOverridenException("Hermes3DFunction<Scalar>::derivative_z");
return Ord(99);
}
};
int CTranscription::TengHash(unsigned char c)
{
size_t n;
for(unsigned int i=0;i<equivs.count();i++)
{
n=equivs[i].find(c);
if(n != std::string::npos)
return Ord(equivs[i][0]);
}
return Ord(c);
}
bool TIniFile::ReadBool(const wxString &Section, const wxString &Ident,
bool Default)
{
bool result;
result = ReadInteger(Section, Ident, Ord(Default)) != 0;
return result;
}
Ord CustomWeakForm::CustomVectorFormSurface::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v, Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
for (int i = 0; i < n; i++)
result += -wt[i] * v->val[i];
return result;
}
Ord CustomWeakFormHeatRK::CustomFormResidualVol::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v,
Geom<Ord> *e, ExtData<Ord> *ext) const
{
Func<Ord>* u_prev_newton = u_ext[0];
// Return the polynomial order of the gradient increased by five to account for lambda(x, y).
return (u_prev_newton->dx[0] * v->dx[0] + u_prev_newton->dy[0] * v->dy[0]) * Ord(5);
}
Ord CustomWeakForm::JacobianFormSurf_0_0::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vj, Func<Ord> *vi, Geom<Ord> *e, ExtData<Ord> *ext) const
{
Ord result = Ord(0);
for (int i = 0; i < n; i++)
result += wt[i] * (kappa * vj->val[i] * vi->val[i]);
return result;
}
Ord CustomWeakForm::ResidualFormSurf_0::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vi, Geom<Ord> *e, ExtData<Ord> *ext) const
{
Ord result = Ord(0);
Func<Ord>* t_prev_newton = u_ext[0];
for (int i = 0; i < n; i++)
result += wt[i] * (kappa * t_prev_newton->val[i] * vi->val[i]);
return result;
}
Ord CustomWeakForm::JacobianFormVol_0_1::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vj, Func<Ord> *vi, Geom<Ord> *e, ExtData<Ord> *ext) const
{
Ord result = Ord(0);
Func<Ord>* domegady = ext->fn[0];
for (int i = 0; i < n; i++)
result += wt[i] * (- domegady->val[i] * vj->val[i] * vi->val[i] );
return result;
}
Ord CustomWeakForm::JacobianFormVol_1_0::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vj, Func<Ord> *vi, Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
Func<Ord>* domegadt = ext[0];
for (int i = 0; i < n; i++)
result += wt[i] * ( domegadt->val[i] * vj->val[i] * vi->val[i] );
return result;
}
Ord WeakFormNSSimpleLinearization::VectorFormVolVel::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v, Geom<Ord> *e, ExtData<Ord> *ext) const
{
Ord result = Ord(0);
if(!Stokes) {
Func<Ord>* vel_prev_time = ext->fn[0]; // this form is used with both velocity components
result = int_u_v<Ord, Ord>(n, wt, vel_prev_time, v) / time_step;
}
return result;
}
Ord DefaultResidualMagnetostatics::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v,
Geom<Ord> *e, ExtData<Ord> *ext) const {
Ord planar_part = 0;
for (int i = 0; i < n; i++) {
Ord B_i = sqrt(sqr(u_ext[0]->dx[i]) + sqr(u_ext[0]->dy[i]));
planar_part += wt[i] * const_coeff*spline_coeff->get_value(B_i) *
(u_ext[0]->dx[i] * v->dx[i] + u_ext[0]->dy[i] * v->dy[i]);
}
return planar_part * Ord(order_increase);
}
Ord CustomWeakFormPicard::CustomResidual::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v,
Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
for (int i = 0; i < n; i++)
{
result += wt[i] * f->value(e->x[i], e->y[i]) * v->val[i];
}
return result;
}
Ord WeakFormNSNewton::VectorFormNS_2::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v, Geom<Ord> *e, Func<Ord>* *ext) const
{
Ord result = Ord(0);
Func<Ord>* xvel_prev_newton = u_ext[0];
Func<Ord>* yvel_prev_newton = u_ext[1];
for (int i = 0; i < n; i++)
result += wt[i] * (xvel_prev_newton->dx[i] * v->val[i] + yvel_prev_newton->dy[i] * v->val[i]);
return result;
}
Ord CustomWeakForm::CustomFormAdvection::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *u, Func<Ord> *v,
Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
for (int i = 0; i < n; i++)
{
result += wt[i] * (ext[0]->dx[i] * u->dx[i] + ext[0]->dy[i] * u->dy[i]) * v->val[i];
}
return result;
}
static int
OpDec(int p, const char *type, Atom a, Term m)
{
int i;
AtomEntry *ae = RepAtom(a);
OpEntry *info;
if (m == TermProlog)
m = PROLOG_MODULE;
else if (m == USER_MODULE)
m = PROLOG_MODULE;
for (i = 1; i <= 7; ++i)
if (strcmp(type, optypes[i]) == 0)
break;
if (i > 7) {
Yap_Error(DOMAIN_ERROR_OPERATOR_SPECIFIER,MkAtomTerm(Yap_LookupAtom(type)),"op/3");
return(FALSE);
}
if (p) {
if (i == 1 || i == 2 || i == 4)
p |= DcrlpFlag;
if (i == 1 || i == 3 || i == 6)
p |= DcrrpFlag;
}
WRITE_LOCK(ae->ARWLock);
info = Yap_GetOpPropForAModuleHavingALock(ae, m);
if (EndOfPAEntr(info)) {
info = (OpEntry *) Yap_AllocAtomSpace(sizeof(OpEntry));
info->KindOfPE = Ord(OpProperty);
info->OpModule = m;
info->OpName = a;
//LOCK(OpListLock);
info->OpNext = OpList;
OpList = info;
//UNLOCK(OpListLock);
AddPropToAtom(ae, (PropEntry *)info);
INIT_RWLOCK(info->OpRWLock);
WRITE_LOCK(info->OpRWLock);
WRITE_UNLOCK(ae->ARWLock);
info->Prefix = info->Infix = info->Posfix = 0;
} else {
WRITE_LOCK(info->OpRWLock);
WRITE_UNLOCK(ae->ARWLock);
}
if (i <= 3) {
GET_LD
if (truePrologFlag(PLFLAG_ISO) &&
info->Posfix != 0) /* there is a posfix operator */ {
/* ISO dictates */
WRITE_UNLOCK(info->OpRWLock);
Yap_Error(PERMISSION_ERROR_CREATE_OPERATOR,MkAtomTerm(a),"op/3");
return FALSE;
}
info->Infix = p;
} else if (i <= 5) {
Ord WeakFormNSNewton::BilinearFormNonsymVel_1_0::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *u, Func<Ord> *v, Geom<Ord> *e,
ExtData<Ord> *ext) const
{
Ord result = Ord(0);
if(!Stokes) {
Func<Ord>* yvel_prev_newton = u_ext[0];
for (int i = 0; i < n; i++)
result += wt[i] * (u->val[i] * v->val[i] * yvel_prev_newton->dx[i]);
}
return result;
}
Ord CustomWeakForm::JacobianFormVol_1_1::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vj, Func<Ord> *vi, Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
Func<Ord>* domegady = ext[1];
for (int i = 0; i < n; i++)
result += wt[i] * ( 1.5 * vj->val[i] * vi->val[i] / tau
+ (vj->dx[i] * vi->dx[i] + vj->dy[i] * vi->dy[i]) / Le
+ domegady->val[i] * vj->val[i] * vi->val[i] );
return result;
}
Ord CustomWeakFormPicard::CustomJacobian::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *u, Func<Ord> *v,
Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
for (int i = 0; i < n; i++)
{
result += wt[i] * lambda->value(u_ext[0]->val[i]) * (u->dx[i] * v->dx[i] + u->dy[i] * v->dy[i]);
}
return result;
}
Ord WeakFormNSSimpleLinearization::BilinearFormNonsymVel::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *u, Func<Ord> *v, Geom<Ord> *e,
ExtData<Ord> *ext) const
{
Ord result = Ord(0);
if(!Stokes) {
Func<Ord>* xvel_prev_time = ext->fn[0];
Func<Ord>* yvel_prev_time = ext->fn[1];
result = int_w_nabla_u_v<Ord, Ord>(n, wt, xvel_prev_time, yvel_prev_time, u, v);
}
return result;
}
Ord WeakFormNSNewton::BilinearFormNonsymVel_0_1::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *u, Func<Ord> *v, GeomVol<Ord> *e,
Func<Ord>* *ext) const
{
Ord result = Ord(0);
if (!Stokes)
{
Func<Ord>* xvel_prev_newton = u_ext[0];
for (int i = 0; i < n; i++)
result += wt[i] * u->val[i] * xvel_prev_newton->dy[i] * v->val[i];
}
return result;
}
void Distribute(SLList *L,int i,ArrType f,ArrType e) /*Distribute() function */
{ int j,p;
for(j=0;j<RD;j++)
f[j]=0;
for(p=L->r[0].next;p;p=L->r[p].next)
{ j=Ord(L->r[p].keys[i]); /*call Ord() */
if(!f[j])
f[j]=p;
else
L->r[e[j]].next=p;
e[j]=p;
}/*end of for */
}/*end of Distrubute() function */
END
/*---------------------------------------------------------------------------*/
static void ChkZero(char *Asc, Byte *erg)
{
if ((strlen(Asc) > 1) && ((*Asc == '<') || (*Asc == '>')))
{
*erg = Ord(*Asc == '<') + 1;
strmov(Asc, Asc + 1);
}
else
*erg = 0;
}
Ord ErrorForm::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *u, Func<Ord> *v, Geom<Ord> *e,
ExtData<Ord> *ext) const
{
switch (projNormType)
{
case HERMES_L2_NORM:
return l2_error_form_axisym<Ord, Ord>(n, wt, u_ext, u, v, e, ext);
case HERMES_H1_NORM:
return h1_error_form_axisym<Ord, Ord>(n, wt, u_ext, u, v, e, ext);
default:
error("Only the H1 and L2 norms are currently implemented.");
return Ord();
}
}
Ord CustomResidual2::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v,
Geom<Ord> *e, ExtData<Ord> *ext) const
{
Ord result = Ord(0);
for (int i = 0; i < n; i++)
{
result += wt[i] * ( d_v*d_v * (u_ext[1]->dx[i]*v->dx[i] + u_ext[1]->dy[i]*v->dy[i])
- u_ext[0]->val[i]*v->val[i]
+ u_ext[1]->val[i]*v->val[i]
- g2->value(e->x[i], e->y[i])*v->val[i]
);
}
return result;
}
Ord CustomWeakForm::ResidualFormVol_0::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vi, Geom<Ord> *e, Func<Ord> **ext) const
{
Ord result = Ord(0);
Func<Ord>* titer = u_ext[0];
Func<Ord>* t_prev_time_1 = ext[2];
Func<Ord>* t_prev_time_2 = ext[3];
Func<Ord>* omega = ext[6];
for (int i = 0; i < n; i++)
result += wt[i] * ( (3.0 * titer->val[i] - 4.0 * t_prev_time_1->val[i]
+ t_prev_time_2->val[i]) * vi->val[i] / (2.0 * tau) +
(titer->dx[i] * vi->dx[i] + titer->dy[i] * vi->dy[i]) -
omega->val[i] * vi->val[i]);
return result;
}
Ord CustomWeakForm::ResidualFormVol_1::ord(int n, double *wt, Func<Ord> *u_ext[],
Func<Ord> *vi, Geom<Ord> *e, ExtData<Ord> *ext) const
{
Ord result = Ord(0);
Func<Ord>* c_prev_newton = u_ext[1];
Func<Ord>* c_prev_time_1 = ext->fn[0];
Func<Ord>* c_prev_time_2 = ext->fn[1];
Func<Ord>* omega = ext->fn[2];
for (int i = 0; i < n; i++)
result += wt[i] * ( (3.0 * c_prev_newton->val[i] - 4.0 * c_prev_time_1->val[i] + c_prev_time_2->val[i])
* vi->val[i] / (2.0 * tau) +
(c_prev_newton->dx[i] * vi->dx[i] + c_prev_newton->dy[i] * vi->dy[i]) / Le +
omega->val[i] * vi->val[i]);
return result;
}
Ord WeakFormNSNewton::VectorFormNS_1::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *v, Geom<Ord> *e, Func<Ord>* *ext) const
{
Ord result = Ord(0);
Func<Ord>* yvel_prev_time = ext[0];
Func<Ord>* xvel_prev_newton = u_ext[0];
Func<Ord>* yvel_prev_newton = u_ext[1];
Func<Ord>* p_prev_newton = u_ext[2];
for (int i = 0; i < n; i++)
result += wt[i] * ((xvel_prev_newton->dx[i] * v->dx[i] + xvel_prev_newton->dy[i] * v->dy[i]) / Reynolds
- (p_prev_newton->val[i] * v->dx[i]));
if(!Stokes)
for (int i = 0; i < n; i++)
result += wt[i] * (((yvel_prev_newton->val[i] - yvel_prev_time->val[i]) * v->val[i] / time_step )
+ ((xvel_prev_newton->val[i] * xvel_prev_newton->dx[i]
+ yvel_prev_newton->val[i] * xvel_prev_newton->dy[i]) * v->val[i]));
return result;
}
Ord DefaultJacobianMagnetostatics::ord(int n, double *wt, Func<Ord> *u_ext[], Func<Ord> *u, Func<Ord> *v,
Geom<Ord> *e, ExtData<Ord> *ext) const {
Ord planar_part = 0;
for (int i = 0; i < n; i++) {
Ord B_i = sqrt(sqr(u_ext[0]->dx[i]) + sqr(u_ext[0]->dy[i]));
planar_part += wt[i] * const_coeff*spline_coeff->get_derivative(B_i) / B_i
* (u_ext[0]->dx[i] * u->dx[i] + u_ext[0]->dy[i] * u->dy[i])
* (u_ext[0]->dx[i] * v->dx[i] + u_ext[0]->dy[i] * v->dy[i]);
planar_part += wt[i] * const_coeff*spline_coeff->get_value(B_i)
* (u->dx[i] * v->dx[i] + u->dy[i] * v->dy[i]);
}
// This increase is for the axisymmetric part. We are not letting the
// Ord class do it since it would automatically choose the highest order
// due to the nonpolynomial 1/r term.
return planar_part * Ord(order_increase);
}
Geom<Ord> init_geom(int marker) {
_F_
Geom<Ord> e;
e.marker = marker;
static Ord x[] = { Ord(1) };
static Ord y[] = { Ord(1) };
static Ord z[] = { Ord(1) };
static Ord nx[] = { Ord(1) };
static Ord ny[] = { Ord(1) };
static Ord nz[] = { Ord(1) };
static Ord tx[] = { Ord(1) };
static Ord ty[] = { Ord(1) };
static Ord tz[] = { Ord(1) };
e.x = x; e.y = y; e.z = z;
e.nx = nx; e.ny = ny; e.nz = nz;
e.tx = tx; e.ty = ty; e.tz = tz;
return e;
}