765 lines
22 KiB
Fortran
765 lines
22 KiB
Fortran
!!******************************************************************************
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!!
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!! This file is part of the AMUN source code, a program to perform
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!! Newtonian or relativistic magnetohydrodynamical simulations on uniform or
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!! adaptive mesh.
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!!
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!! Copyright (C) 2008-2020 Grzegorz Kowal <grzegorz@amuncode.org>
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!!
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!! This program is free software: you can redistribute it and/or modify
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!! it under the terms of the GNU General Public License as published by
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!! the Free Software Foundation, either version 3 of the License, or
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!! (at your option) any later version.
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!!
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!! This program is distributed in the hope that it will be useful,
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!! but WITHOUT ANY WARRANTY; without even the implied warranty of
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!! MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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!! GNU General Public License for more details.
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!!
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!! You should have received a copy of the GNU General Public License
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!! along with this program. If not, see <http://www.gnu.org/licenses/>.
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!!
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!!******************************************************************************
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!!
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!! module: SOURCES
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!!
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!! This modules adds source terms.
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!!
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!!******************************************************************************
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!
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module sources
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#ifdef PROFILE
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! include external procedures
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!
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use timers, only : set_timer, start_timer, stop_timer
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#endif /* PROFILE */
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! module variables are not implicit by default
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!
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implicit none
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#ifdef PROFILE
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! timer indices
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!
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integer, save :: imi, imu
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#endif /* PROFILE */
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! GLM-MHD source terms type (1 - EGLM, 2 - HEGLM)
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!
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integer , save :: glm_type = 0
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character(len=32), save :: glm_name = "none"
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! viscosity coefficient
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!
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real(kind=8) , save :: viscosity = 0.0d+00
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! resistivity coefficient
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!
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real(kind=8) , save :: resistivity = 0.0d+00
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real(kind=8) , save :: anomalous = 0.0d+00
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real(kind=8) , save :: jcrit = 1.0d+00
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! by default everything is private
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!
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private
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! declare public subroutines
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!
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public :: initialize_sources, finalize_sources, print_sources
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public :: update_sources
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public :: viscosity, resistivity
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!- - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
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!
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contains
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!
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!===============================================================================
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!!
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!!*** PUBLIC SUBROUTINES *****************************************************
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!!
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!===============================================================================
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!
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!===============================================================================
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!
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! subroutine INITIALIZE_SOURCES:
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! -----------------------------
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!
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! Subroutine initializes module SOURCES.
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!
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! Arguments:
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!
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! verbose - a logical flag turning the information printing;
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! status - an integer flag for error return value;
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!
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!===============================================================================
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!
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subroutine initialize_sources(verbose, status)
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! include external procedures and variables
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!
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use parameters , only : get_parameter
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! local variables are not implicit by default
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!
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implicit none
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! subroutine arguments
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!
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logical, intent(in) :: verbose
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integer, intent(out) :: status
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! local variables
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!
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character(len=8) :: tglm = "none"
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!
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!-------------------------------------------------------------------------------
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!
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#ifdef PROFILE
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! set timer descriptions
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!
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call set_timer('sources:: initialize', imi)
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call set_timer('sources:: update' , imu)
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! start accounting time for module initialization/finalization
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!
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call start_timer(imi)
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#endif /* PROFILE */
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! reset the status flag
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!
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status = 0
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! get the type of the GLM source terms
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!
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call get_parameter("glm_source_terms", tglm)
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! set the glm_type variable to correct value
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!
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select case(trim(tglm))
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case("eglm", "EGLM")
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glm_type = 1
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glm_name = "EGLM"
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case("heglm", "HEGLM")
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glm_type = 2
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glm_name = "HEGLM"
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case default
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glm_type = 0
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glm_name = "none"
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end select
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! get viscosity coefficient
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!
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call get_parameter("viscosity", viscosity)
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if (viscosity < 0.0d+00) then
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if (verbose) then
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write(*,*)
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write(*,"(1x,a)") "ERROR!"
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write(*,"(1x,a)") "Negative viscosity coefficient!"
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end if
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status = 1
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end if
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! get resistivity coefficients
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!
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call get_parameter("resistivity", resistivity)
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if (resistivity < 0.0d+00) then
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if (verbose) then
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write(*,*)
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write(*,"(1x,a)") "ERROR!"
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write(*,"(1x,a)") "Negative resistivity coefficient!"
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end if
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status = 1
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end if
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call get_parameter("anomalous", anomalous)
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if (anomalous < 0.0d+00) then
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if (verbose) then
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write(*,*)
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write(*,"(1x,a)") "ERROR!"
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write(*,"(1x,a)") "Negative anomalous resistivity coefficient!"
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end if
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status = 1
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end if
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call get_parameter("jcrit", jcrit)
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if (jcrit <= 0.0d+00) then
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if (verbose) then
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write(*,*)
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write(*,"(1x,a)") "ERROR!"
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write(*,"(1x,a)") "Non-positive critical current density coefficient!"
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end if
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status = 1
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end if
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#ifdef PROFILE
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! stop accounting time for module initialization/finalization
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!
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call stop_timer(imi)
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#endif /* PROFILE */
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!-------------------------------------------------------------------------------
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!
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end subroutine initialize_sources
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!
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!===============================================================================
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!
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! subroutine FINALIZE_SOURCES:
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! ---------------------------
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!
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! Subroutine releases memory used by the module.
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!
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! Arguments:
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!
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! status - an integer flag for error return value;
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!
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!===============================================================================
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!
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subroutine finalize_sources(status)
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! local variables are not implicit by default
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!
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implicit none
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! subroutine arguments
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!
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integer, intent(out) :: status
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!
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!-------------------------------------------------------------------------------
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!
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#ifdef PROFILE
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! start accounting time for module initialization/finalization
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!
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call start_timer(imi)
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#endif /* PROFILE */
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! reset the status flag
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!
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status = 0
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#ifdef PROFILE
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! stop accounting time for module initialization/finalization
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!
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call stop_timer(imi)
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#endif /* PROFILE */
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!-------------------------------------------------------------------------------
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!
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end subroutine finalize_sources
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!
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!===============================================================================
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!
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! subroutine PRINT_SOURCES:
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! ------------------------
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!
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! Subroutine prints module parameters.
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!
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! Arguments:
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!
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! verbose - a logical flag turning the information printing;
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!
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!===============================================================================
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!
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subroutine print_sources(verbose)
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! include external procedures
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!
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use equations, only : magnetized
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use helpers , only : print_section, print_parameter
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! local variables are not implicit by default
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!
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implicit none
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! subroutine arguments
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!
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logical, intent(in) :: verbose
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!
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!-------------------------------------------------------------------------------
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!
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if (verbose) then
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call print_section(verbose, "Source terms")
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call print_parameter(verbose, "viscosity" , viscosity )
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if (magnetized) then
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call print_parameter(verbose, "resistivity" , resistivity)
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if (anomalous > 0.0d+00) then
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call print_parameter(verbose, "anomalous" , anomalous )
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call print_parameter(verbose, "jcrit" , jcrit )
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end if
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call print_parameter(verbose, "glm source terms", glm_name )
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end if
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end if
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!-------------------------------------------------------------------------------
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!
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end subroutine print_sources
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!
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!===============================================================================
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!
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! subroutine UPDATE_SOURCES:
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! -------------------------
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!
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! Subroutine add the source terms.
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!
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! Arguments:
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!
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! pdata - the pointer to a data block;
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! t, dt - the time and time increment;
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! du - the array of variable increment;
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!
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!===============================================================================
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!
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subroutine update_sources(pdata, t, dt, du)
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! include external variables
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!
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use blocks , only : block_data
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use coordinates , only : nn => bcells
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use coordinates , only : ax, ay, az, adx, ady, adz
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use equations , only : inx, iny, inz
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use equations , only : idn, ivx, ivy, ivz, imx, imy, imz, ien
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use equations , only : ibx, iby, ibz, ibp
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use gravity , only : gravity_enabled, gravitational_acceleration
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use operators , only : divergence, gradient, laplace, curl
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use user_problem , only : update_sources_user
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! local variables are not implicit by default
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!
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implicit none
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! subroutine arguments
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!
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type(block_data), pointer , intent(inout) :: pdata
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real(kind=8) , intent(in) :: t, dt
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real(kind=8), dimension(:,:,:,:), intent(inout) :: du
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! local variables
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!
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integer :: i, j, k = 1
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real(kind=8) :: fc, gc
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real(kind=8) :: gx, gy, gz
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real(kind=8) :: dvxdx, dvxdy, dvxdz, divv
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real(kind=8) :: dvydx, dvydy, dvydz
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real(kind=8) :: dvzdx, dvzdy, dvzdz
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! local arrays
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!
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real(kind=8), dimension(3) :: ga, dh
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real(kind=8), dimension(nn) :: x, y
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#if NDIMS == 3
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real(kind=8), dimension(nn) :: z
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real(kind=8), dimension(nn,nn,nn) :: db
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real(kind=8), dimension(3,3,nn,nn,nn) :: tmp
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#else /* NDIMS == 3 */
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real(kind=8), dimension( 1) :: z
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real(kind=8), dimension(nn,nn, 1) :: db
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real(kind=8), dimension(3,3,nn,nn, 1) :: tmp
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#endif /* NDIMS == 3 */
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!
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!-------------------------------------------------------------------------------
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!
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#ifdef PROFILE
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! start accounting time for source terms
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!
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call start_timer(imu)
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#endif /* PROFILE */
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! proceed only if the gravitational term is enabled
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!
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if (gravity_enabled) then
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! prepare block coordinates
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!
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x(:) = pdata%meta%xmin + ax(pdata%meta%level,:)
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y(:) = pdata%meta%ymin + ay(pdata%meta%level,:)
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#if NDIMS == 3
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z(:) = pdata%meta%zmin + az(pdata%meta%level,:)
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#endif /* NDIMS == 3 */
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! iterate over all positions in the YZ plane
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!
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#if NDIMS == 3
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do k = 1, nn
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#endif /* NDIMS == 3 */
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do j = 1, nn
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do i = 1, nn
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! get gravitational acceleration components
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!
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call gravitational_acceleration(t, dt, x(i), y(j), z(k), ga(1:3))
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! calculate the gravitational source terms
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!
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gx = pdata%q(idn,i,j,k) * ga(1)
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gy = pdata%q(idn,i,j,k) * ga(2)
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#if NDIMS == 3
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gz = pdata%q(idn,i,j,k) * ga(3)
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#endif /* NDIMS == 3 */
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! add source terms to momentum equations
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!
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du(imx,i,j,k) = du(imx,i,j,k) + gx
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du(imy,i,j,k) = du(imy,i,j,k) + gy
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#if NDIMS == 3
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du(imz,i,j,k) = du(imz,i,j,k) + gz
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#endif /* NDIMS == 3 */
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! add source terms to total energy equation
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!
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if (ien > 0) then
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#if NDIMS == 2
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du(ien,i,j,k) = du(ien,i,j,k) + gx * pdata%q(ivx,i,j,k) &
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+ gy * pdata%q(ivy,i,j,k)
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#endif /* NDIMS == 2 */
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#if NDIMS == 3
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du(ien,i,j,k) = du(ien,i,j,k) + gx * pdata%q(ivx,i,j,k) &
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+ gy * pdata%q(ivy,i,j,k) &
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+ gz * pdata%q(ivz,i,j,k)
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#endif /* NDIMS == 3 */
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end if
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end do ! i = 1, nn
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end do ! j = 1, nn
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#if NDIMS == 3
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end do ! k = 1, nn
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#endif /* NDIMS == 3 */
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end if ! gravity enabled
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! proceed only if the viscosity coefficient is not zero
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!
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if (viscosity > 0.0d+00) then
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! prepare coordinate increments
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!
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dh(1) = adx(pdata%meta%level)
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dh(2) = ady(pdata%meta%level)
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dh(3) = adz(pdata%meta%level)
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! calculate the velocity Jacobian
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!
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call gradient(dh(:), pdata%q(ivx,:,:,:), tmp(inx,inx:inz,:,:,:))
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call gradient(dh(:), pdata%q(ivy,:,:,:), tmp(iny,inx:inz,:,:,:))
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call gradient(dh(:), pdata%q(ivz,:,:,:), tmp(inz,inx:inz,:,:,:))
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! iterate over all cells
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!
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#if NDIMS == 3
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do k = 1, nn
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#endif /* NDIMS == 3 */
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do j = 1, nn
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do i = 1, nn
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! prepare the νρ factor
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!
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gc = viscosity * pdata%q(idn,i,j,k)
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fc = 2.0d+00 * gc
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! get the velocity Jacobian elements
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!
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dvxdx = tmp(inx,inx,i,j,k)
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dvxdy = tmp(inx,iny,i,j,k)
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dvxdz = tmp(inx,inz,i,j,k)
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dvydx = tmp(iny,inx,i,j,k)
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dvydy = tmp(iny,iny,i,j,k)
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dvydz = tmp(iny,inz,i,j,k)
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dvzdx = tmp(inz,inx,i,j,k)
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dvzdy = tmp(inz,iny,i,j,k)
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dvzdz = tmp(inz,inz,i,j,k)
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divv = (dvxdx + dvydy + dvzdz) / 3.0d+00
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! calculate elements of the viscous stress tensor
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!
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tmp(inx,inx,i,j,k) = fc * (dvxdx - divv)
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tmp(iny,iny,i,j,k) = fc * (dvydy - divv)
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tmp(inz,inz,i,j,k) = fc * (dvzdz - divv)
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tmp(inx,iny,i,j,k) = gc * (dvxdy + dvydx)
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tmp(inx,inz,i,j,k) = gc * (dvxdz + dvzdx)
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tmp(iny,inz,i,j,k) = gc * (dvydz + dvzdy)
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tmp(iny,inx,i,j,k) = tmp(inx,iny,i,j,k)
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tmp(inz,inx,i,j,k) = tmp(inx,inz,i,j,k)
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tmp(inz,iny,i,j,k) = tmp(iny,inz,i,j,k)
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end do ! i = 1, nn
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end do ! j = 1, nn
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#if NDIMS == 3
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end do ! k = 1, nn
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#endif /* NDIMS == 3 */
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! calculate the divergence of the first tensor row
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!
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call divergence(dh(:), tmp(inx,inx:inz,:,:,:), db(:,:,:))
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! add viscous source terms to the X momentum equation
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!
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du(imx,:,:,:) = du(imx,:,:,:) + db(:,:,:)
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! calculate the divergence of the second tensor row
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!
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call divergence(dh(:), tmp(iny,inx:inz,:,:,:), db(:,:,:))
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! add viscous source terms to the Y momentum equation
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!
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du(imy,:,:,:) = du(imy,:,:,:) + db(:,:,:)
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! calculate the divergence of the third tensor row
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!
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call divergence(dh(:), tmp(inz,inx:inz,:,:,:), db(:,:,:))
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! add viscous source terms to the Z momentum equation
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!
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du(imz,:,:,:) = du(imz,:,:,:) + db(:,:,:)
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! add viscous source term to total energy equation
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!
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if (ien > 0) then
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! iterate over all cells
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!
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#if NDIMS == 3
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do k = 1, nn
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#endif /* NDIMS == 3 */
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do j = 1, nn
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do i = 1, nn
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! calculate scalar product of v and viscous stress tensor τ
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!
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gx = pdata%q(ivx,i,j,k) * tmp(inx,inx,i,j,k) &
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+ pdata%q(ivy,i,j,k) * tmp(inx,iny,i,j,k) &
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+ pdata%q(ivz,i,j,k) * tmp(inx,inz,i,j,k)
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gy = pdata%q(ivx,i,j,k) * tmp(iny,inx,i,j,k) &
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+ pdata%q(ivy,i,j,k) * tmp(iny,iny,i,j,k) &
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+ pdata%q(ivz,i,j,k) * tmp(iny,inz,i,j,k)
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gz = pdata%q(ivx,i,j,k) * tmp(inz,inx,i,j,k) &
|
||
+ pdata%q(ivy,i,j,k) * tmp(inz,iny,i,j,k) &
|
||
+ pdata%q(ivz,i,j,k) * tmp(inz,inz,i,j,k)
|
||
|
||
! update (v.τ), use the first row of the tensor tmp
|
||
!
|
||
tmp(inx,inx,i,j,k) = gx
|
||
tmp(inx,iny,i,j,k) = gy
|
||
tmp(inx,inz,i,j,k) = gz
|
||
|
||
end do ! i = 1, nn
|
||
end do ! j = 1, nn
|
||
#if NDIMS == 3
|
||
end do ! k = 1, nn
|
||
#endif /* NDIMS == 3 */
|
||
|
||
! calculate the divergence of (v.τ)
|
||
!
|
||
call divergence(dh(:), tmp(inx,inx:inz,:,:,:), db(:,:,:))
|
||
|
||
! update the energy increment
|
||
!
|
||
du(ien,:,:,:) = du(ien,:,:,:) + db(:,:,:)
|
||
|
||
end if ! ien > 0
|
||
|
||
end if ! viscosity is not zero
|
||
|
||
!=== add magnetic field related source terms ===
|
||
!
|
||
if (ibx > 0) then
|
||
|
||
! prepare coordinate increments
|
||
!
|
||
dh(1) = adx(pdata%meta%level)
|
||
dh(2) = ady(pdata%meta%level)
|
||
dh(3) = adz(pdata%meta%level)
|
||
|
||
! add the EGLM-MHD source terms
|
||
!
|
||
if (glm_type > 0) then
|
||
|
||
! calculate the magnetic field divergence
|
||
!
|
||
call divergence(dh(:), pdata%q(ibx:ibz,:,:,:), db(:,:,:))
|
||
|
||
! update the momentum component increments, i.e.
|
||
! d/dt (ρv) + ∇.F = - (∇.B)B
|
||
!
|
||
du(imx,:,:,:) = du(imx,:,:,:) - db(:,:,:) * pdata%q(ibx,:,:,:)
|
||
du(imy,:,:,:) = du(imy,:,:,:) - db(:,:,:) * pdata%q(iby,:,:,:)
|
||
du(imz,:,:,:) = du(imz,:,:,:) - db(:,:,:) * pdata%q(ibz,:,:,:)
|
||
|
||
! update the energy equation
|
||
!
|
||
if (ien > 0 .and. ibp > 0) then
|
||
|
||
! calculate the gradient of divergence potential
|
||
!
|
||
call gradient(dh(:), pdata%q(ibp,:,:,:), tmp(inx:inz,inx,:,:,:))
|
||
|
||
! add the divergence potential source term to the energy equation, i.e.
|
||
! d/dt E + ∇.F = - B.(∇ψ)
|
||
!
|
||
du(ien,:,:,:) = du(ien,:,:,:) &
|
||
- sum(pdata%q(ibx:ibz,:,:,:) * tmp(inx:inz,inx,:,:,:), 1)
|
||
|
||
end if ! ien > 0
|
||
|
||
! add the HEGLM-MHD source terms
|
||
!
|
||
if (glm_type > 1) then
|
||
|
||
! update magnetic field component increments, i.e.
|
||
! d/dt B + ∇.F = - (∇.B)v
|
||
!
|
||
du(ibx,:,:,:) = du(ibx,:,:,:) - db(:,:,:) * pdata%q(ivx,:,:,:)
|
||
du(iby,:,:,:) = du(iby,:,:,:) - db(:,:,:) * pdata%q(ivy,:,:,:)
|
||
du(ibz,:,:,:) = du(ibz,:,:,:) - db(:,:,:) * pdata%q(ivz,:,:,:)
|
||
|
||
! update the energy equation
|
||
!
|
||
if (ien > 0) then
|
||
|
||
! calculate scalar product of velocity and magnetic field
|
||
!
|
||
tmp(inx,inx,:,:,:) = sum(pdata%q(ivx:ivz,:,:,:) &
|
||
* pdata%q(ibx:ibz,:,:,:), 1)
|
||
|
||
! add the divergence potential source term to the energy equation, i.e.
|
||
! d/dt E + ∇.F = - (∇.B) (v.B)
|
||
!
|
||
du(ien,:,:,:) = du(ien,:,:,:) - db(:,:,:) * tmp(inx,inx,:,:,:)
|
||
|
||
end if ! ien > 0
|
||
|
||
end if ! glm_type > 1
|
||
|
||
end if ! glmtype > 0
|
||
|
||
! if anomalous resistivity is enabled
|
||
!
|
||
if (anomalous > 0.0d+00) then
|
||
|
||
! calculate current density (J = ∇xB)
|
||
!
|
||
call curl(dh(:), pdata%q(ibx:ibz,:,:,:), tmp(inx:inz,inx,:,:,:))
|
||
|
||
! calculate the normalized absolute value of current density (|J|/Jcrit)
|
||
!
|
||
tmp(inx,iny,:,:,:) = sqrt(sum(tmp(inx:inz,inx,:,:,:)**2, 1)) / jcrit
|
||
|
||
! calculate the local resistivity [ηu + ηa (|J|/Jcrit - 1) H(|J|/Jcrit)]
|
||
!
|
||
tmp(iny,iny,:,:,:) = resistivity + &
|
||
anomalous * max(0.0d+00, (tmp(inx,iny,:,:,:) - 1.0d+00))
|
||
|
||
! multiply the current density vector by the local resistivity (ηJ)
|
||
!
|
||
tmp(inx,inz,:,:,:) = tmp(iny,iny,:,:,:) * tmp(inx,inx,:,:,:)
|
||
tmp(iny,inz,:,:,:) = tmp(iny,iny,:,:,:) * tmp(iny,inx,:,:,:)
|
||
tmp(inz,inz,:,:,:) = tmp(iny,iny,:,:,:) * tmp(inz,inx,:,:,:)
|
||
|
||
! calculate the curl of (ηJ)
|
||
!
|
||
call curl(dh(:), tmp(inx:inz,inz,:,:,:), tmp(inx:inz,iny,:,:,:))
|
||
|
||
! update magnetic field component increments
|
||
!
|
||
du(ibx,:,:,:) = du(ibx,:,:,:) - tmp(inx,iny,:,:,:)
|
||
du(iby,:,:,:) = du(iby,:,:,:) - tmp(iny,iny,:,:,:)
|
||
du(ibz,:,:,:) = du(ibz,:,:,:) - tmp(inz,iny,:,:,:)
|
||
|
||
! update energy equation
|
||
!
|
||
if (ien > 0) then
|
||
|
||
! calculate the vector product Bx(η ∇xB)
|
||
!
|
||
tmp(inx,iny,:,:,:) = pdata%q(iby,:,:,:) * tmp(inz,inz,:,:,:) &
|
||
- pdata%q(ibz,:,:,:) * tmp(iny,inz,:,:,:)
|
||
tmp(iny,iny,:,:,:) = pdata%q(ibz,:,:,:) * tmp(inx,inz,:,:,:) &
|
||
- pdata%q(ibx,:,:,:) * tmp(inz,inz,:,:,:)
|
||
tmp(inz,iny,:,:,:) = pdata%q(ibx,:,:,:) * tmp(iny,inz,:,:,:) &
|
||
- pdata%q(iby,:,:,:) * tmp(inx,inz,:,:,:)
|
||
|
||
! calculate the divergence ∇.[Bx(η ∇xB)]
|
||
!
|
||
call divergence(dh(:), tmp(inx:inz,iny,:,:,:), db(:,:,:))
|
||
|
||
! add the second resistive source term to the energy equation, i.e.
|
||
! d/dt E + ∇.F = η J²
|
||
!
|
||
du(ien,:,:,:) = du(ien,:,:,:) + db(:,:,:)
|
||
|
||
end if ! energy equation present
|
||
|
||
else if (resistivity > 0.0d+00) then
|
||
|
||
! calculate the Laplace operator of B, i.e. Δ(B)
|
||
!
|
||
call laplace(dh(:), pdata%q(ibx,:,:,:), tmp(inx,inx,:,:,:))
|
||
call laplace(dh(:), pdata%q(iby,:,:,:), tmp(inx,iny,:,:,:))
|
||
call laplace(dh(:), pdata%q(ibz,:,:,:), tmp(inx,inz,:,:,:))
|
||
|
||
! multiply by the resistivity coefficient
|
||
!
|
||
tmp(iny,inx:inz,:,:,:) = resistivity * tmp(inx,inx:inz,:,:,:)
|
||
|
||
! update magnetic field component increments
|
||
!
|
||
du(ibx,:,:,:) = du(ibx,:,:,:) + tmp(iny,inx,:,:,:)
|
||
du(iby,:,:,:) = du(iby,:,:,:) + tmp(iny,iny,:,:,:)
|
||
du(ibz,:,:,:) = du(ibz,:,:,:) + tmp(iny,inz,:,:,:)
|
||
|
||
! update energy equation
|
||
!
|
||
if (ien > 0) then
|
||
|
||
! add the first resistive source term to the energy equation, i.e.
|
||
! d/dt E + ∇.F = η B.[Δ(B)]
|
||
!
|
||
du(ien,:,:,:) = du(ien,:,:,:) &
|
||
+ (pdata%q(ibx,:,:,:) * tmp(iny,inx,:,:,:) &
|
||
+ pdata%q(iby,:,:,:) * tmp(iny,iny,:,:,:) &
|
||
+ pdata%q(ibz,:,:,:) * tmp(iny,inz,:,:,:))
|
||
|
||
! calculate current density J = ∇xB
|
||
!
|
||
call curl(dh(:), pdata%q(ibx:ibz,:,:,:), tmp(inz,inx:inz,:,:,:))
|
||
|
||
! calculate J²
|
||
!
|
||
db(:,:,:) = tmp(inz,inx,:,:,:)**2 + tmp(inz,iny,:,:,:)**2 &
|
||
+ tmp(inz,inz,:,:,:)**2
|
||
|
||
! add the second resistive source term to the energy equation, i.e.
|
||
! d/dt E + ∇.F = η J²
|
||
!
|
||
du(ien,:,:,:) = du(ien,:,:,:) + resistivity * db(:,:,:)
|
||
|
||
end if ! energy equation present
|
||
|
||
end if ! resistivity is not zero
|
||
|
||
end if ! ibx > 0
|
||
|
||
! add user defined source terms
|
||
!
|
||
call update_sources_user(pdata, t, dt, du(:,:,:,:))
|
||
|
||
#ifdef PROFILE
|
||
! stop accounting time for source terms
|
||
!
|
||
call stop_timer(imu)
|
||
#endif /* PROFILE */
|
||
|
||
!-------------------------------------------------------------------------------
|
||
!
|
||
end subroutine update_sources
|
||
|
||
!===============================================================================
|
||
!
|
||
end module sources
|