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hc.c
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hc.c
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#include "hc.h"
/*
implementation of Hager & O'Connell (1981) method of solving mantle
circulation given internal density anomalies, only radially varying
viscosity, and either free-slip or plate velocity boundary condition
at surface
based on Hager & O'Connell (1981), Hager & Clayton (1989), and
Steinberger (2000)
the original code is due to Brad Hager, Rick O'Connell, and was
largely modified by Bernhard Steinberger
this version by Thorsten Becker (twb@ig.utexas.edu)
>>> SOME COMMENTS FROM THE ORIGINAL CODE <<<
C * It uses the following Numerical Recipes (Press et al.) routines:
C four1, realft, gauleg, rk4, rkdumb, ludcmp, lubksb;
C !!!!!!!!!!!!!!!!!!! rkqc, odeint !!!!!!!!!! take out !!!!!!
C and the following routines by R.J. O'Connell:
C shc2d, shd2c, ab2cs, cs2ab, plmbar, plvel2sh, pltgrid, pltvel,
C vshd2c, plmbar1.
C Further subroutines are: kinsub, evalpa,
C torsol (all based on "kinflow" by Hager & O'Connell),
C densub and evppot (based on "denflow" by Hager & O'Connell),
C sumsub (based on "sumkd" by Hager & O'Connell, but
C substantially speeded up),
C convert, derivs and shc2dd (based on R.J. O'Connell's shc2d).
C
C bugs found:
C * The combination of (1) high viscosity lithosphere
C (2) compressible flow (3) kinematic (plate driven) flow
C doesn't work properly. The problem presumably only occurs
C at degree 1 (I didn't make this sure) but this is sufficient
C to screw up everything. It will usually work to reduce the
C contrast between lithospheric and asthenospheric viscosity.
C Then make sure that (1) two viscosity structures give similar
C results for incompressible and (2) incompressible and compressible
C reduced viscosity look similar (e.g. anomalous mass flux vs. depth)
<<< END OLD COMMENTS
*/
int main(int argc, char **argv)
{
struct hcs *model; /* main structure, make sure to initialize with
zeroes */
struct sh_lms *sol_spectral=NULL, *geoid = NULL; /* solution expansions */
struct sh_lms *pvel=NULL; /* local plate velocity expansion */
int nsol,lmax,i;
FILE *out;
struct hc_parameters p[1]; /* parameters */
char filename[HC_CHAR_LENGTH],file_prefix[10];
HC_PREC *sol_spatial = NULL; /* spatial solution,
e.g. velocities */
static hc_boolean geoid_binary = FALSE; /* type of geoid output */
static HC_CPREC unitya[1] = {1.0};
strncpy(p->main_program_name,argv[0],HC_CHAR_LENGTH);
/*
(1)
initialize the model structure, this is needed to initialize some
of the default values before callign the parameter handling
routine this call also involves initializing the hc parameter
structure
*/
hc_struc_init(&model);
/*
(2)
init parameters to default values
*/
hc_init_parameters(p);
/*
handle command line arguments
*/
hc_handle_command_line(argc,argv,1,p);
/*
begin main program part
*/
#ifdef __TIMESTAMP__
if(p->verbose)
fprintf(stderr,"%s: starting version compiled on %s\n",argv[0],__TIMESTAMP__);
#else
if(p->verbose)
fprintf(stderr,"%s: starting main program\n",argv[0]);
#endif
/*
(3)
initialize all variables
- choose the internal spherical harmonics convention
- assign constants
- assign phase boundaries, if any
- read in viscosity structure
- assign density anomalies
- read in plate velocities
*/
hc_init_main(model,SH_RICK,p);
nsol = (model->nradp2) * 3; /*
number of solutions (r,pol,tor) * (nlayer+2)
total number of layers is nlayer +2,
because CMB and surface are added
to intermediate layers which are
determined by the spacing of the
density model
*/
if(p->free_slip) /* maximum degree is determined by the
density expansion */
lmax = model->dens_anom[0].lmax;
else /* max degree is determined by the
plate velocities */
lmax = model->pvel.p[0].lmax; /* shouldn't be larger than that*/
/*
make sure we have room for the plate velocities
*/
sh_allocate_and_init(&pvel,2,lmax,model->sh_type,1,p->verbose,FALSE);
/* init done */
/*
SOLUTION PART
*/
/*
make room for the spectral solution on irregular grid
*/
sh_allocate_and_init(&sol_spectral,nsol,lmax,model->sh_type,HC_VECTOR,
p->verbose,FALSE);
if(p->compute_geoid == 1)
/* make room for geoid solution at surface */
sh_allocate_and_init(&geoid,1,model->dens_anom[0].lmax,
model->sh_type,HC_SCALAR,p->verbose,FALSE);
else if(p->compute_geoid == 2) /* all layers (or kernels) */
sh_allocate_and_init(&geoid,model->nradp2,model->dens_anom[0].lmax,
model->sh_type,HC_SCALAR,p->verbose,FALSE);
/*
solve poloidal and toroidal part and sum
*/
if(!p->free_slip)
hc_select_pvel(p->pvel_time,&model->pvel,pvel,p->verbose);
hc_solve(model,p->free_slip,p->solution_mode,sol_spectral,
TRUE,TRUE,TRUE,p->print_pt_sol,p->compute_geoid,
pvel,model->dens_anom,geoid,
p->verbose,p->print_kernel_only);
/*
OUTPUT PART
*/
if(!p->print_kernel_only){
/*
output of spherical harmonics solution
*/
switch(p->solution_mode){
case HC_VEL:
sprintf(file_prefix,"vel");break;
case HC_RTRACTIONS:
sprintf(file_prefix,"rtrac");break;
case HC_HTRACTIONS:
sprintf(file_prefix,"htrac");break;
default:
HC_ERROR(argv[0],"solution mode undefined");break;
}
if(p->sol_binary_out)
sprintf(filename,"%s.%s",file_prefix,HC_SOLOUT_FILE_BINARY);
else
sprintf(filename,"%s.%s",file_prefix,HC_SOLOUT_FILE_ASCII);
if(p->verbose)
fprintf(stderr,"%s: writing spherical harmonics solution to %s\n",
argv[0],filename);
out = hc_fopen(filename,"w","main",p->main_program_name);
hc_print_spectral_solution(model,sol_spectral,out,
p->solution_mode,
p->sol_binary_out,p->verbose);
fclose(out);
/* */
if(p->print_density_field){
/*
print the density field
*/
sprintf(file_prefix,"dscaled");
if(p->sol_binary_out)
sprintf(filename,"%s.%s",file_prefix,HC_SOLOUT_FILE_BINARY);
else
sprintf(filename,"%s.%s",file_prefix,HC_SOLOUT_FILE_ASCII);
if(p->verbose)
fprintf(stderr,"%s: writing scaled density anomaly field to %s\n",
argv[0],filename);
out = hc_fopen(filename,"w","main",p->main_program_name);
hc_print_dens_anom(model,out,p->sol_binary_out,p->verbose);
fclose(out);
}
if(p->print_spatial){
/*
we wish to use the spatial solution
expand velocities to spatial base, compute spatial
representation
*/
hc_compute_sol_spatial(model,sol_spectral,&sol_spatial,
p->verbose);
/*
output of spatial solution
*/
sprintf(filename,"%s.%s",file_prefix,HC_SPATIAL_SOLOUT_FILE);
/* print lon lat z v_r v_theta v_phi */
hc_print_spatial_solution(model,sol_spectral,sol_spatial,
filename,HC_LAYER_OUT_FILE,
p->solution_mode,p->sol_binary_out,
p->verbose);
}
} /* end non-kernel branch */
/* compute the geoid? */
if(p->compute_geoid){
/*
print geoid solution
*/
if(p->print_kernel_only)
sprintf(filename,"%s",HC_GEOID_KERNEL_FILE);
else
sprintf(filename,"%s",HC_GEOID_FILE);
if(p->verbose)
fprintf(stderr,"%s: writing geoid %sto %s, %s\n",argv[0],
((p->print_kernel_only)?("kernels "):("")),filename,
(p->compute_geoid == 1)?("at surface"):("all layers"));
out = hc_fopen(filename,"w","main",p->main_program_name);
if(p->print_kernel_only){
hc_print_geoid_kernel(geoid,model->r,model->nradp2,out,p->verbose);
}else{ /* geoid solutions */
if(p->compute_geoid == 1) /* surface layer */
hc_print_sh_scalar_field(geoid,out,FALSE,geoid_binary,p->verbose);
else{ /* all layers */
for(i=0;i < model->nradp2;i++){
sh_print_parameters_to_stream((geoid+i),1,i,model->nradp2,
HC_Z_DEPTH(model->r[i]),out,
FALSE,geoid_binary,p->verbose);
sh_print_coefficients_to_stream((geoid+i),1,out,
unitya,geoid_binary,p->verbose);
}
}
}
fclose(out);
}
/*
free memory
*/
sh_free_expansion(sol_spectral,nsol);
/* local copies of plate velocities */
sh_free_expansion(pvel,2);
/* */
if(p->compute_geoid == 1) /* only one layer */
sh_free_expansion(geoid,1);
else if(p->compute_geoid == 2) /* all layers */
sh_free_expansion(geoid,model->nradp2);
free(sol_spatial);
if(p->verbose)
fprintf(stderr,"%s: done\n",argv[0]);
hc_struc_free(&model);
return 0;
}