advection_2d.f90

An advection example using the Koren flux limiter. Time stepping is done with the explicit trapezoidal rule.

program advection_2d
  use m_a2_all

  implicit none

  integer, parameter  :: box_size   = 8
  integer, parameter  :: i_phi      = 1
  integer, parameter  :: i_phi_old  = 2
  integer, parameter  :: i_err      = 3
  integer, parameter  :: sol_type   = 1
  real(dp), parameter :: domain_len = 2 * acos(-1.0_dp)
  real(dp), parameter :: dr         = domain_len / box_size

  type(a2_t)        :: tree
  type(ref_info_t)   :: refine_info
  integer            :: ix_list(2, 1)
  integer            :: nb_list(a2_num_neighbors, 1)
  integer            :: refine_steps, time_steps, output_cnt
  integer            :: i, id, n, n_steps
  real(dp)           :: dt, time, end_time, p_err, n_err
  real(dp)           :: sum_phi, sum_phi_t0
  real(dp)           :: dt_adapt, dt_output
  real(dp)           :: velocity(2), dr_min(2)
  character(len=100) :: fname
  integer            :: count_rate, t_start, t_end

  print *, "Running advection_2d"
  print *, "Number of threads", af_get_max_threads()

  ! Initialize tree
  call a2_init(tree, & ! Tree to initialize
       box_size, &     ! A box contains box_size**DIM cells
       n_var_cell=3, & ! Number of cell-centered variables
       n_var_face=1, & ! Number of face-centered variables
       dr=dr, &        ! Distance between cells on base level
       cc_names=["phi", "old", "err"]) ! Variable names

  call a2_set_cc_methods(tree, i_phi, a2_bc_neumann_zero, a2_gc_interp_lim, &
       prolong=a2_prolong_limit)

  ! Set up geometry
  id             = 1
  ix_list(:, id) = 1            ! Set index of box
  nb_list(:, id) = id           ! Box is periodic, so its own neighbor

  ! Create the base mesh, using the box indices and their neighbor information
  call a2_set_base(tree, 1, ix_list, nb_list)

  output_cnt = 0
  time       = 0
  dt_adapt   = 0.01_dp
  dt_output  = 0.1_dp
  end_time   = 5.0_dp
  velocity(:) = 0.0_dp
  velocity(1) = 1.0_dp
  velocity(2) = -1.0_dp

  ! Set up the initial conditions
  call system_clock(t_start,count_rate)
  refine_steps=0

  do
     refine_steps=refine_steps+1
     ! We should only set the finest level, but this also works
     call a2_loop_box(tree, set_initial_condition)

     ! Fill ghost cells for variables i_phi on the sides of all boxes, using
     ! a2_gc_interp_lim on refinement boundaries: Interpolation between fine
     ! points and coarse neighbors to fill ghost cells near refinement
     ! boundaries. The ghost values are less than twice the coarse values. and
     ! a2_bc_neumann_zero physical boundaries: fill ghost cells near physical
     ! boundaries using Neumann zero
     call a2_gc_tree(tree, i_phi, a2_gc_interp_lim, a2_bc_neumann_zero)

     ! Adjust the refinement of a tree using refine_routine (see below) for grid
     ! refinement.
     ! Routine a2_adjust_refinement sets the bit af_bit_new_children for each box
     ! that is refined.  On input, the tree should be balanced. On output,
     ! the tree is still balanced, and its refinement is updated (with at most
     ! one level per call).
     call a2_adjust_refinement(tree, &           ! tree
          refine_routine, & ! Refinement function
          refine_info, &    ! Information about refinement
          1)                ! Buffer width (in cells)

     ! If no new boxes have been added, exit the loop
     if (refine_info%n_add == 0) exit
  end do
  call system_clock(t_end, count_rate)

  write(*, "(A,i0,A,Es10.3,A)") " Wall-clock time for ", &
       refine_steps, " refinement steps: ", &
       (t_end-t_start) / real(count_rate, dp), " seconds"

  call a2_print_info(tree)

  ! Restrict the initial conditions Restrict the children of a box to the box
  ! (e.g., in 2D, average the values at the four children to get the value for
  ! the parent)
  call a2_restrict_tree(tree, i_phi)

  ! Fill ghost cells for variables i_phi on the sides of all boxes, using
  ! a2_gc_interp_lim on refinement boundaries and a2_bc_neumann_zero on
  ! physical boundaries
  call a2_gc_tree(tree, i_phi, a2_gc_interp_lim, a2_bc_neumann_zero)

  call system_clock(t_start, count_rate)
  time_steps = 0

  call a2_tree_sum_cc(tree, i_phi, sum_phi_t0)

  ! Starting simulation
  do
     time_steps = time_steps + 1
     dr_min  = a2_min_dr(tree)
     dt      = 0.5_dp / (sum(abs(velocity/dr_min)) + epsilon(1.0_dp))

     n_steps = ceiling(dt_adapt/dt)
     dt      = dt_adapt / n_steps

     if (output_cnt * dt_output <= time) then
        output_cnt = output_cnt + 1
        write(fname, "(A,I0)") "advection_2d_", output_cnt

        ! Call procedure set_error (see below) for each box in tree, with argument time
        call a2_loop_box_arg(tree, set_error, [time])

        ! Write the cell centered data of tree to a vtk unstructured file fname.
        ! Only the leaves of the tree are used
        call a2_write_silo(tree, trim(fname), output_cnt, time, dir="output")

        ! Find maximum and minimum values of cc(..., i_err) and cc(..., i_phi).
        ! By default, only loop over leaves, and ghost cells are not used.
        call a2_tree_max_cc(tree, i_err, p_err)
        call a2_tree_min_cc(tree, i_err, n_err)
        call a2_tree_sum_cc(tree, i_phi, sum_phi)
        write(*,"(2(A,1x,Es12.4,2x))")  &
             " max error:", max(p_err, abs(n_err)), &
             "conservation error:  ", (sum_phi - sum_phi_t0) / sum_phi_t0
     end if

     if (time > end_time) exit

     do n = 1, n_steps
        ! Copy previous solution
        call a2_tree_copy_cc(tree, i_phi, i_phi_old)

        ! Two forward Euler steps over dt
        do i = 1, 2
           ! Call procedure fluxes_koren for each id in tree, giving the list of boxes
           call a2_loop_boxes(tree, fluxes_koren)

           ! Restrict fluxes from children to parents on refinement boundaries.
           call a2_consistent_fluxes(tree, [i_phi])

           ! Call procedure update_solution (see below) for each box in tree, with argument dt
           call a2_loop_box_arg(tree, update_solution, [dt])

           ! Restrict variables i_phi to all parent boxes
           call a2_restrict_tree(tree, i_phi)
        end do

        ! Take average of phi_old and phi
        call a2_loop_box(tree, average_phi)
        time = time + dt
     end do

     ! Fill ghost cells for variable i_phi
     call a2_gc_tree(tree, i_phi, a2_gc_interp_lim, a2_bc_neumann_zero)

     ! Adjust the refinement of a tree using refine_routine (see below) for grid
     ! refinement. On input, the tree should be balanced. On output, the tree is
     ! still balanced, and its refinement is updated (with at most one level per
     ! call).
     call a2_adjust_refinement(tree, refine_routine, refine_info, 1)
  end do

  call system_clock(t_end,count_rate)
  write(*, "(A,I0,A,Es10.3,A)") &
       " Wall-clock time after ",time_steps, &
       " time steps: ", (t_end-t_start) / real(count_rate, dp), &
       " seconds"

  ! This call is not really necessary here, but cleaning up the data in a tree
  ! is important if your program continues with other tasks.
  call a2_destroy(tree)

contains

  subroutine refine_routine(box, cell_flags)
    type(box2_t), intent(in) :: box
    integer, intent(out)      :: cell_flags(box%n_cell, box%n_cell)
    real(dp)                  :: diff
    integer                   :: i, j, nc

    nc   = box%n_cell

    do j = 1, nc; do i = 1, nc
       diff = abs(box%cc(i+1, j, i_phi) + &
            box%cc(i-1, j, i_phi) + &
            box%cc(i, j+1, i_phi) + &
            box%cc(i, j-1, i_phi) - &
            4 * box%cc(i, j, i_phi)) * box%dr

       if (box%lvl < 2 .or. diff > 0.5e-3_dp .and. box%lvl < 5) then
          cell_flags(i, j) = af_do_ref
       else if (diff < 0.1_dp * 0.1e-3_dp) then
          cell_flags(i, j) = af_rm_ref
       else
          cell_flags(i, j) = af_keep_ref
       end if
    end do; end do
  end subroutine refine_routine

  subroutine set_initial_condition(box)
    type(box2_t), intent(inout) :: box
    integer                      :: i, j, nc
    real(dp)                     :: rr(2)

    nc = box%n_cell
    do j = 0, nc+1; do i = 0, nc+1
       rr = a2_r_cc(box, [i, j])
       box%cc(i, j, i_phi) = solution(rr, 0.0_dp)
    end do; end do
  end subroutine set_initial_condition

  subroutine set_error(box, time)
    type(box2_t), intent(inout) :: box
    real(dp), intent(in)         :: time(:)
    integer                      :: i, j, nc
    real(dp)                     :: rr(2)

    nc = box%n_cell
    do j = 1, nc; do i = 1, nc
       rr = a2_r_cc(box, [i, j])
       box%cc(i, j, i_err) = &
            box%cc(i, j, i_phi) - solution(rr, time(1))
    end do; end do
  end subroutine set_error

  function solution(rr, t) result(sol)
    real(dp), intent(in) :: rr(2), t
    real(dp)             :: sol, rr_t(2)

    rr_t = rr - velocity * t

    select case (sol_type)
    case (1)
       sol = sin(rr_t(1))**4 * cos(rr_t(2))**4
    case (2)
       rr_t = modulo(rr_t, domain_len) / domain_len
       if (norm2(rr_t - 0.5_dp) < 0.1_dp) then
          sol = 1.0_dp
       else
          sol = 0.0_dp
       end if
    end select
  end function solution

  subroutine fluxes_koren(boxes, id)
    use m_flux_schemes
    type(box2_t), intent(inout) :: boxes(:)
    integer, intent(in)          :: id
    integer                      :: nc
    real(dp), allocatable        :: cc(:, :)
    real(dp), allocatable        :: v(:, :, :)

    nc     = boxes(id)%n_cell
    allocate(cc(-1:nc+2, -1:nc+2))
    allocate(v(1:nc+1, 1:nc+1, 2))

    call a2_gc_box(boxes, id, i_phi, a2_gc_interp_lim, a2_bc_neumann_zero)

    ! Get a second layer of ghost cell data (the 'normal' routines give just one
    ! layer of ghost cells). Use a2_gc2_prolong_linear on refinement boundaries and
    ! a2_bc2_neumann_zero on physical boundaries.
    call a2_gc2_box(boxes, &      ! List of all the boxes
         id, &                     ! Id of box for which we set ghost cells
         i_phi, &                  ! Variable for which ghost cells are set
         a2_gc2_prolong_linear, & ! Procedure called at refinement boundaries
         a2_bc2_neumann_zero, &   ! Procedure called at physical boundaries
         cc, &                  ! The enlarged box with ghost cells
         nc)                       ! box%n_cell

    v(:, :, 1) = velocity(1)
    v(:, :, 2) = velocity(2)

    call flux_koren_2d(cc, v, nc, 2)
    boxes(id)%fc(:, :, :, i_phi) = v

  end subroutine fluxes_koren

  subroutine update_solution(box, dt)
    type(box2_t), intent(inout) :: box
    real(dp), intent(in)         :: dt(:)
    real(dp)                     :: inv_dr
    integer                      :: i, j, nc

    nc     = box%n_cell
    inv_dr = 1/box%dr

    forall (i = 1:nc, j = 1:nc)
       box%cc(i, j, i_phi) = box%cc(i, j, i_phi) + dt(1) * inv_dr * ( &
            box%fc(i, j, 1, i_phi) - box%fc(i+1, j, 1, i_phi) + &
            box%fc(i, j, 2, i_phi) - box%fc(i, j+1, 2, i_phi))
    end forall
  end subroutine update_solution

  subroutine average_phi(box)
    type(box2_t), intent(inout) :: box

    box%cc(:, :, i_phi) = 0.5_dp * (box%cc(:, :, i_phi) + &
         box%cc(:, :, i_phi_old))
  end subroutine average_phi

end program advection_2d