strot_dirac_global.C

/*
 *  Methods for computing global quantities within the class Star_rot_Dirac
 *
 *    (see file star.h for documentation).
 *
 */

/*
 *   Copyright (c) 2005 Lap-Ming Lin & Jerome Novak
 *
 *   This file is part of LORENE.
 *
 *   LORENE is free software; you can redistribute it and/or modify
 *   it under the terms of the GNU General Public License version 2
 *   as published by the Free Software Foundation.
 *
 *   LORENE is distributed in the hope that it will be useful,
 *   but WITHOUT ANY WARRANTY; without even the implied warranty of
 *   MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
 *   GNU General Public License for more details.
 *
 *   You should have received a copy of the GNU General Public License
 *   along with LORENE; if not, write to the Free Software
 *   Foundation, Inc., 59 Temple Place, Suite 330, Boston, MA  02111-1307  USA
 *
 */

 

/*
 * $Id: strot_dirac_global.C,v 1.14 2016/12/05 16:18:15 j_novak Exp $
 * $Log: strot_dirac_global.C,v $
 * Revision 1.14  2016/12/05 16:18:15  j_novak
 * Suppression of some global variables (file names, loch, ...) to prevent redefinitions
 *
 * Revision 1.13  2014/10/13 08:53:40  j_novak
 * Lorene classes and functions now belong to the namespace Lorene.
 *
 * Revision 1.12  2014/10/06 15:13:18  j_novak
 * Modified #include directives to use c++ syntax.
 *
 * Revision 1.11  2010/11/17 11:21:52  j_novak
 * Corrected minor problems in the case nz=1 and nt=1.
 *
 * Revision 1.10  2010/10/22 08:08:40  j_novak
 * Removal of the method Star_rot_dirac::lambda_grv2() and call to the C++ version of integrale2d.
 *
 * Revision 1.9  2009/10/26 10:54:33  j_novak
 * Added the case of a NONSYM base in theta.
 *
 * Revision 1.8  2008/05/30 08:27:38  j_novak
 * New global quantities rp_circ and ellipt (circumferential polar coordinate and
 * ellipticity).
 *
 * Revision 1.7  2008/02/18 13:51:20  j_novak
 * Change of a dzpuis
 *
 * Revision 1.6  2005/03/25 14:11:49  j_novak
 * In the 1D case, GRV2 returns -1 (because of a problem in integral2d).
 *
 * Revision 1.5  2005/02/17 17:30:42  f_limousin
 * Change the name of some quantities to be consistent with other classes
 * (for instance nnn is changed to nn, shift to beta, beta to lnq...)
 *
 * Revision 1.4  2005/02/09 13:36:01  lm_lin
 *
 * Add the calculations of GRV2, T/W, R_circ, and flattening.
 *
 * Revision 1.3  2005/02/02 10:11:24  j_novak
 * Better calculation of the GRV3 identity.
 *
 *
 *
 * $Header: /cvsroot/Lorene/C++/Source/Star/strot_dirac_global.C,v 1.14 2016/12/05 16:18:15 j_novak Exp $
 *
 */


// C headers
#include <cmath>
#include <cassert>

// Lorene headers
#include "star_rot_dirac.h"
#include "unites.h"
#include "utilitaires.h" 
#include "proto.h"

        //-------------------------------------------------------//
        //                Baryonic mass                          //
        //                                                       //
        //  Note: In Lorene units, mean particle mass is unity   //
        //-------------------------------------------------------//


namespace Lorene {
double Star_rot_Dirac::mass_b() const {

  if (p_mass_b == 0x0) {    // a new computation is required

    Scalar dens = sqrt( gamma.determinant() ) * gam_euler * nbar ;

    dens.std_spectral_base() ;

    p_mass_b = new double( dens.integrale() ) ;

  }

  return *p_mass_b ;

}

          //---------------------------------------------------------//
          //            Gravitational mass                           //   
          //                                                         //
          // Note: This is the Komar mass for stationary and         //
          //       asymptotically flat spacetime (see, eg, Wald)     //
          //---------------------------------------------------------//

double Star_rot_Dirac::mass_g() const {

  if (p_mass_g == 0x0) {    // a new computation is required

    Scalar j_source = 2.* contract(contract(gamma.cov(), 0, j_euler, 0), 
                   0, beta, 0) ;
           
    Scalar dens = sqrt( gamma.determinant() ) *  
          ( nn * (ener_euler + s_euler) - j_source ) ;

    dens.std_spectral_base() ;

    p_mass_g = new double( dens.integrale() ) ;

  }

  return *p_mass_g ;

}

                //--------------------------------------//
                //    Angular momentum                  //
                //                                      // 
                // Komar-type integral (see, eg, Wald)  //
                //--------------------------------------// 

double Star_rot_Dirac::angu_mom() const {

  if (p_angu_mom == 0x0) {    // a new computation is required

    // phi_kill = axial killing vector 

    Vector phi_kill(mp, CON, mp.get_bvect_spher()) ;

    phi_kill.set(1).set_etat_zero() ;
    phi_kill.set(2).set_etat_zero() ;
    phi_kill.set(3) = 1. ;
    phi_kill.set(3).std_spectral_base() ;
    phi_kill.set(3).mult_rsint() ;

    Scalar j_source = contract(contract(gamma.cov(), 0, j_euler, 0),
                   0, phi_kill, 0) ;

    Scalar dens = sqrt( gamma.determinant() ) * j_source  ;

    dens.std_spectral_base() ;

    p_angu_mom = new double( dens.integrale() ) ;


  }

  return *p_angu_mom ;

}

                     //---------------------//
                     //        T/W          //
                     //---------------------//

double Star_rot_Dirac::tsw() const {

  if (p_tsw == 0x0) {    // a new computation is required

    double tcin = 0.5 * omega * angu_mom() ;

    Scalar dens = sqrt( gamma.determinant() ) * gam_euler * ener ;
    
    dens.std_spectral_base() ;
    
    double mass_p = dens.integrale() ;

    p_tsw = new double( tcin / ( mass_p + tcin - mass_g() ) ) ;

  }

  return *p_tsw ;

}


      //--------------------------------------------------------------//
      //                        GRV2                                  //   
      // cf. Eq. (28) of Bonazzola & Gourgoulhon CQG, 11, 1775 (1994) // 
      //                                                              //
      //--------------------------------------------------------------//

double Star_rot_Dirac::grv2() const {

  using namespace Unites ;

  if (p_grv2 == 0x0) {    // a new computation is required

      // determinant of the 2-metric k_{ab}
      
      Scalar k_det = gamma.cov()(1,1)*gamma.cov()(2,2) - 
      gamma.cov()(1,2)*gamma.cov()(1,2) ;
      
      
      //**
      // sou_m = 8\pi T_{\mu\nu} m^{\mu}m^{\nu}
      // => sou_m = 8\pi [ (E+P) U^2 + P ], where v^2 = v_i v^i 
      //
      //**
      
      Scalar sou_m = 2 * qpig * ( (ener_euler + press)*v2 + press ) ;
      
      sou_m = sqrt( k_det )*sou_m ;
      
      sou_m.std_spectral_base() ;
      
      
      // This is the term 3k_a k^a. 
      
      Scalar sou_q = 3 *( taa(1,3) * aa(1,3) + taa(2,3)*aa(2,3) )  ;
      
      
      // This is the term \nu_{|| a}\nu^{|| a}. 
      //
      
      Scalar sou_tmp = gamma.con()(1,1) * logn.dsdr() * logn.dsdr() ;
      
      Scalar term_2 = 2 * gamma.con()(1,2) * logn.dsdr() * logn.dsdt() ;
      
      term_2.div_r_dzpuis(4) ;
      
      Scalar term_3 = gamma.con()(2,2) * logn.dsdt() * logn.dsdt() ;
      
      term_3.div_r_dzpuis(2) ;
      term_3.div_r_dzpuis(4) ;
      
      sou_tmp += term_2 + term_3 ;
      
      
      // Source of the gravitational part
      
      sou_q -= sou_tmp ;
      
      sou_q = sqrt( k_det )*sou_q ;
      
      sou_q.std_spectral_base() ;
      
      p_grv2 = new double( double(1) + integrale2d(sou_m)/integrale2d(sou_q) ) ;

  }

  return *p_grv2 ;

}


     //-------------------------------------------------------------//
     //                 GRV3                                        //
     // cf. Eq. (29) of Gourgoulhon & Bonazzola CQG, 11, 443 (1994) //
     //-------------------------------------------------------------//

double Star_rot_Dirac::grv3() const {

  using namespace Unites ;

  if (p_grv3 == 0x0) {    // a new computation is required

    // Gravitational term 
    // -------------------

    Scalar sou_q = 0.75*aa_quad - contract(logn.derive_cov(gamma), 0,
                       logn.derive_con(gamma), 0) ;


    Tensor t_tmp = contract(gamma.connect().get_delta(), 2, 
                gamma.connect().get_delta(), 0) ;

    Scalar tmp_1 = 0.25* contract( gamma.con(), 0, 1, 
        contract(t_tmp, 0, 3), 0, 1 ) ;

    Scalar tmp_2 = 0.25* contract( gamma.con(), 0, 1, 
          contract( contract( gamma.connect().get_delta(), 0, 1), 
                       0, gamma.connect().get_delta(), 0), 0, 1)  ;

    sou_q = sou_q + tmp_1 - tmp_2 ;

    sou_q = sqrt( gamma.determinant() ) * sou_q ; 

    sou_q.std_spectral_base() ;

    double int_grav = sou_q.integrale() ;


    // Matter term 
    // --------------

    Scalar sou_m = qpig*s_euler ;

    sou_m = sqrt( gamma.determinant() ) * sou_m ;

    sou_m.std_spectral_base() ;

    double int_mat = sou_m.integrale() ;

    p_grv3 = new double( (int_grav + int_mat) / int_mat ) ;
    


  }

  return *p_grv3 ;

}


                //--------------------//
                //     R_circ         //
                //--------------------//

double Star_rot_Dirac::r_circ() const {

  if (p_r_circ ==0x0) {  // a new computation is required

    // Index of the point at phi=0, theta=pi/2 at the surface of the star:
    const Mg3d* mg = mp.get_mg() ;
    int l_b = nzet - 1 ; 
    int i_b = mg->get_nr(l_b) - 1 ; 
    int j_b = (mg->get_type_t() == SYM ? mg->get_nt(l_b) - 1 : mg->get_nt(l_b) / 2) ; 
    int k_b = 0 ;

    double gamma_phi = gamma.cov()(3,3).val_grid_point(l_b, k_b, j_b, i_b) ;

    p_r_circ = new double( sqrt( gamma_phi ) * ray_eq() ) ;

  }

  return *p_r_circ ;

}


                //--------------------//
                //     R_circ         //
                //--------------------//

double Star_rot_Dirac::rp_circ() const {

    if (p_rp_circ ==0x0) {  // a new computation is required
    const Mg3d& mg = *mp.get_mg() ;
    int nz = mg.get_nzone() ;
    assert(nz>2) ;
    int np = mg.get_np(0) ;
    if (np != 1) {
        cout << "The polar circumferential radius is only well defined\n"
         << "with np = 1!" << endl ;
        abort() ;
    }
    int nt = mg.get_nt(0) ;
    Sym_tensor gam = gamma.cov() ;
    const Coord& tet = mp.tet ;
    Scalar rrr(mp) ;
    rrr.annule_hard() ;
    rrr.annule(nzet,nz-1) ;
    double phi = 0 ;
    for (int j=0; j<nt; j++) {
        double theta = (+tet)(0, 0, j, 0) ;
        double erre = 
        mp.val_r(l_surf()(0,j), xi_surf()(0, j), theta, phi) ;
        for (int lz=0; lz<nzet; lz++) {
        int nrz = mg.get_nr(lz) ;
        for (int i=0; i<nrz; i++) {
            rrr.set_grid_point(lz, 0, j, i) = erre ; 
        }
        }
    }
    rrr.std_spectral_base() ;
    Scalar drrr = rrr.dsdt() ;

    Scalar fff(mp) ;
    fff.annule_hard() ;
    fff.annule(nzet,nz-1) ;
    for (int j=0; j<nt; j++) {
        double theta = (+tet)(0, 0, j, 0) ;
        int ls = l_surf()(0, j) ;
        double xs = xi_surf()(0, j) ;
        double grr = gam(1,1).get_spectral_va().val_point_jk(ls, xs, j, 0) ;
        double grt = gam(1,2).get_spectral_va().val_point_jk(ls, xs, j, 0) ;
        double gtt = gam(2,2).get_spectral_va().val_point_jk(ls, xs, j, 0) ;
        double rr = mp.val_r(ls, xs, theta, phi) ;
        double dr = drrr.get_spectral_va().val_point_jk(ls, xs, j, 0) ;
        for (int i=0; i< mg.get_nr(nzet-1); i++) {
        fff.set_grid_point(nzet-1, 0, j, i) 
            = sqrt(grr*dr*dr + 2*grt*rr*dr + gtt*rr*rr) ;
        }
    }
    fff.std_spectral_base() ;
    fff.set_spectral_va().coef() ;
    p_rp_circ = new double((*fff.get_spectral_va().c_cf)(nzet-1, 0, 0, 0)) ;      
    }
    return *p_rp_circ ;
}

                //--------------------------//
                //       Flattening         //
                //--------------------------//

double Star_rot_Dirac::aplat() const {

  return ray_pole() / ray_eq() ;

}

                //--------------------------//
                //       Ellipticity        //
                //--------------------------//

double Star_rot_Dirac::ellipt() const {

  return sqrt(1. - (rp_circ()*rp_circ())/(r_circ()*r_circ())) ;

}
}