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hc_torsol.c
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hc_torsol.c
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#include "hc.h"
//
//
// these subroutines deal with the toroidal part of the
// kinematic solution of a Hager &
// O'Connell flow code. they are based on Brad's original code, and later
// Bernhard Steinberger's modifications
//
// will incorporate the poloidal part of the plate velocities
//
//
// Thorsten Becker, [email protected]
//
// $Id: hc_torsol.c,v 1.8 2006/01/22 01:11:34 becker Exp becker $
//
// ****************************************************************
// * THIS IS THE MAIN PROGRAM FOR THE COMPONENT OF FLOW WITHOUT *
// * DENSITY CONTRASTS. IT USES SEVERAL INPUT/OUTPUT SUBROUTINES *
// * AND FUNCTIONS TO OBTAIN, CORRECT AND VERIFY A MODEL FROM THE *
// * USER. THE FINAL VERSION OF EACH MODEL IS STORED IN A FILE *
// * BEFORE THE PROGRAM EXECUTES POLSOL AND TORSOL TO OBTAIN THE *
// * POLOIDAL AND TOROIDAL COMPONENTS, RESPECTIVELY, OF THE *
// * EQUATIONS OF MOTION. *
// ****************************************************************
// Modified such that only toroidal component is calculated
// Poloidal component is included in densub.f
//
// input: r: radii on which output is defined (nrad+2)
//
// visc,rvisc: normalized viscosities and their radii (nvis)
//
// lmax: MAXIMUM DEGREES,
// nrad: NUMBER OF OUTPUT RADII
// (without top and bottom layers)
// nvis: NUMBER OF VISCOSITIES.
//
// pvel_tor: toroidal part of the plate velocities
// pkernel: print the two solution vectors to file
//
// input/output:
//
// tvec[nradp2 * lmaxp1 * 2 ]: solution kernel
//
// output:
//
// tor_sol[nradp2 * 2] SHOULD BE PASSED INITIALIZED AS ZEROES
//
//
//
//
void hc_torsol(struct hcs *hc,
int nrad,int nvis,int lmax,HC_PREC *r,
HC_PREC **rv,HC_PREC **visc, struct sh_lms *pvel_tor,
struct sh_lms *tor_sol,HC_HIGH_PREC *tvec,
hc_boolean verbose)
{
//
// ****************************************************************
// * evaluates AND PROPAGATES THE TWO TOROIDAL COMPONENTS IN THE *
// * EQUATIONS OF MOTION, AND NORMALIZES THESE SUCH THAT THE *
// * FIRST ELEMENT AT THE SURFACE IS 1.0. *
// ****************************************************************
//
HC_HIGH_PREC coef,*vecnor,hold,rlast,rnext,tloc[2],*tvec1,*tvec2;
HC_HIGH_PREC exp_fac[2],p[2][2],diflog,el,elp2,elm1,efdiff;
int l,jvisp1,jvis,i,j,nvisp1,lmaxp1,os;
hc_boolean qvis;
//
// PASSED PARAMETERS: NRADP2: NUMBER OF OUTPUT RADII,
// NVIS: NUMBER OF VISCOSITIES, nvisp1 = nvis+1
// LMAX: MAXIMUM DEGREES.
// ARRAYS: R: OUTPUT RADII,
// RV: VISCOSITY RADII,
// TVEC: TOROIDAL VECTORS,
// VISC: normalized VISCOSITIES.
// OTHER VAR: EXP_FAC[0],EXP_FAC[1]: EXPONENTIAL FACTORS IN PROPAGATOR,
// COEF,ELP2,ELM1: PARAMETERS IN PROPAGATOR,
// DIFLOG: DIFFERENCE IN LOGS OF RADII,
// EL,L: DEGREE,
// VECNOR: NORMALIZES TVEC_LOC TO TVEC(N,1),
// HOLD: TEMPORARY VAR.,
// P[0][0],P[0][1],P[1][0],P[1][1]: ELEMENTS OF THE PROPAGATOR MATRIX CORRES-
// PONDING TO P(1,1),P(1,2),P(2,1),P(2,2) RESPECTIVELY,
// RLAST,RNEXT: RADII FOR PROPAGATOR,
// TVEC_LOC1,TVEC_LOC2: VECTOR COMPONENTS.
//
/*
set up some pointers (without those the TVECSOL macro won't
work!)
*/
nvisp1 = nvis + 1; /* length of rv and visc */
//nradp2 = nrad + 2; /* radius array */
lmaxp1 = lmax+1; /* length of 0:lmax array */
/*
add one item at end of rv and visc arrays
*/
hc_dvecrealloc(rv,nvisp1,"hc_torsol: rv");
hc_dvecrealloc(visc,nvisp1,"hc_torsol: visc");
/* local reference to viscosity and radii of viscosity */
#define HC_TVISC(i) (*(*visc+(i)))
#define HC_TVR(i) (*(*rv+(i)))
HC_TVR(nvis) = 1.1; /* last entry in radius array, why is
this 1.1? probably because it has to
be > 1
*/
HC_TVISC(nvis) = HC_TVISC(nvis-1); /* last entry in viscosity array */
#ifdef DEBUG
if(hc->nradp2 != nrad + 2){
fprintf(stderr,"hc_torsol: radius number mismatch\n");
exit(-1);
}
/*
test size of expansions
*/
j = hc->nradp2 * 2;
for(i=0;i < j;i++){
if(tor_sol[i].lmax < pvel_tor->lmax){
fprintf(stderr,"hc_torsol: error: toroidal expansion %i has lmax %i, plates have %i\n",
i+1,tor_sol[i].lmax, pvel_tor->lmax);
exit(-1);
}
if(tor_sol[i].type != pvel_tor->type)
HC_ERROR("hc_torsol","torsol type error");
}
#endif
if(verbose)
fprintf(stderr,"hc_torsol: toroidal velocities lmax %i and type %i\n",
pvel_tor->lmax,pvel_tor->type);
/*
make room for toroidal scaling vectors f(l) and initialize as zeroes
*/
/* solution factors as f(l,r) */
/* set local pointes */
tvec1 = tvec;
tvec2 = (tvec + hc->nradp2 * lmaxp1);
//
// (PREVENTS THE REQUESTING OF NON-EXISTANT VALUES)
//
// FOR EACH DEGREE (L) CALCULATE, NORMALIZE AND OUTPUT SOLUTION
//
for(l=1;l < lmaxp1;l++){
/*
loop through all l > 0
*/
el = (HC_PREC)l;
//
// SET THE PARAMETERS
//
elp2 = el + 2.0;
elm1 = el - 1.0;
coef = 1.0 / (2.0 * el + 1.0);
//
// INITIALIZE THE PROPAGATION AT THE CORE
//
jvisp1 = 1; /* viscosity layer counters */
jvis = 0;
rlast = r[0]; /* radius of core */
/*
initialize
*/
tloc[0] = 1.0; /* there seems to be no best ordering for
addressing this array, later we need l to
be the fastest increasing index */
tloc[1] = 0.0;
//
// FIND THE TWO TOROIDAL COMPONENTS AT EACH RADIUS
// start radius loop
//
/*
lowest level
*/
os = l;
tvec1[os] = tloc[0];
tvec2[os] = tloc[1];
for(i=1;i < hc->nradp2;i++){ /* loop through radii */
os += lmaxp1;
//
// TEST FOR CHANGE IN VISCOSITY IN NEXT LAYER
//
qvis = FALSE;
do{
if(HC_TVR(jvisp1) > r[i])
qvis = TRUE;
rnext = HC_TVR(jvisp1); /* */
//
// IF NO VISC. CHANGE BEFORE NEXT OUTPUT RADIUS, PROPAGATE DIRECTLY
//
if(qvis)
rnext = r[i];
diflog = log(rnext / rlast);
exp_fac[0] = exp( el * diflog);
exp_fac[1] = exp(-(el + 1.0) * diflog);
//
// PROPAGATOR SET UP LINEARLY TO AVOID EXCESS MULTIPLICATIONS
//
efdiff = exp_fac[0] - exp_fac[1];
p[0][0] = elp2 * exp_fac[0] + elm1 * exp_fac[1];
p[0][1] = efdiff / HC_TVISC(jvis);
p[1][0] = elp2 * elm1 * HC_TVISC(jvis) * efdiff;
p[1][1] = elm1 * exp_fac[0] + elp2 * exp_fac[1];
//
// PROPAGATE LAST VECTOR TO GET NEW VECTOR
//
rlast = rnext;
hold = tloc[0];
tloc[0] = (p[0][0] * hold + p[0][1] * tloc[1]);
tloc[1] = (p[1][0] * hold + p[1][1] * tloc[1]);
tloc[0] *= coef;
tloc[1] *= coef;
if(!qvis){
jvis = jvisp1;
jvisp1++;
}
}while(!qvis);
tvec1[os] = tloc[0];
tvec2[os] = tloc[1];
} /* end layer loop */
} /* end l loop */
//
// set tvec(l,nradp2-1,0) = 1.0 and normalize all vectors to
// this
//
hc_hvecalloc(&vecnor,lmaxp1,"hc_torsol: vecnor");
os = (hc->nradp2-1) * lmaxp1;
vecnor[0] = 1.0;
for(l=1;l < lmaxp1;l++)
vecnor[l] = 1.0 / tvec1[os+l];
/* normalize */
for(i=os=0;i < hc->nradp2;i++,os+=lmaxp1)
for(l=0;l < lmaxp1;l++){
tvec1[os+l] *= vecnor[l];
tvec2[os+l] *= vecnor[l];
}
free(vecnor);
/*
the toroidal solution corresponds to the toroidal part of the plate
motions scaled by the toroidal solution vectors which are functions
of l and depth
*/
for(os=i=j=0;i < hc->nradp2;i++,os+=lmaxp1,j+=2){
/*
assign toroidal plate motion fields to solution expansion
*/
sh_aexp_equals_bexp_coeff((tor_sol+j+0),pvel_tor);
sh_aexp_equals_bexp_coeff((tor_sol+j+1),pvel_tor);
/*
scale with the toroidal solution at this depth
*/
sh_scale_expansion_l_factor((tor_sol+j+0),(tvec1+os));
sh_scale_expansion_l_factor((tor_sol+j+1),(tvec2+os));
}
if(verbose)
fprintf(stderr,"hc_torsol: done\n");
}
#undef HC_TVISC
#undef HC_TVR