methodsubcellternarymodule Module Reference

Data Types
type	methodsubcellternarytype
	Ternary triangular subcell tracking method. More...

Functions/Subroutines
subroutine, public	create_method_subcell_ternary (method)
	Create a new ternary subcell tracking method. More...
subroutine	deallocate (this)
	Deallocate the ternary subcell tracking method. More...
subroutine	apply_mst (this, particle, tmax)
	Apply the ternary subcell tracking method. More...
subroutine	track_subcell (this, subcell, particle, tmax)
	Track a particle across a triangular subcell. More...
subroutine	calculate_dt (v1, v2, dx, xL, v, dvdx, dt, status, itopbotexit)
	Do calculations related to analytical z solution. More...
subroutine	calculate_xyz_position (dt, rxx, rxy, ryx, ryy, sxx, sxy, syy, izstatus, x0, y0, az, vzi, vzbot, ztop, zbot, zi, x, y, z, exitFace)
	Calculate the particle's local unscaled xyz coordinates after dt. More...

Function/Subroutine Documentation

apply_mst()

subroutine methodsubcellternarymodule::apply_mst ( class(methodsubcellternarytype), intent(inout)  this, type(particletype), intent(inout), pointer  particle, real(dp), intent(in)  tmax  )

private

Definition at line 52 of file MethodSubcellTernary.f90.

    class(MethodSubcellTernaryType), intent(inout) :: this
    type(ParticleType), pointer, intent(inout) :: particle
    real(DP), intent(in) :: tmax
 
    select type (subcell => this%subcell)
    type is (subcelltritype)
      call this%track_subcell(subcell, particle, tmax)
    end select

calculate_dt()

subroutine methodsubcellternarymodule::calculate_dt ( real(dp)  v1, real(dp)  v2, real(dp)  dx, real(dp)  xL, real(dp)  v, real(dp)  dvdx, real(dp)  dt, integer(i4b)  status, integer(i4b)  itopbotexit  )

private

This subroutine consists partly or entirely of code written by David W. Pollock of the USGS for MODPATH 7. The authors of the present code are responsible for its appropriate application in this context and for any modifications or errors.

Definition at line 293 of file MethodSubcellTernary.f90.

    real(DP) :: v1
    real(DP) :: v2
    real(DP) :: dx
    real(DP) :: xL
    real(DP) :: v
    real(DP) :: dvdx
    real(DP) :: dt
    real(DP) :: v2a
    real(DP) :: v1a
    real(DP) :: dv
    real(DP) :: dva
    real(DP) :: vv
    real(DP) :: vvv
    real(DP) :: zro
    real(DP) :: zrom
    real(DP) :: x
    real(DP) :: tol
    real(DP) :: vr1
    real(DP) :: vr2
    real(DP) :: vr
    real(DP) :: v1v2
    integer(I4B) :: status
    integer(I4B) :: itopbotexit
    logical(LGP) :: noOutflow
 
    ! Initialize variables
    status = -1
    dt = 1.0d+20
    v2a = v2
    if (v2a .lt. dzero) v2a = -v2a
    v1a = v1
    if (v1a .lt. dzero) v1a = -v1a
    dv = v2 - v1
    dva = dv
    if (dva .lt. dzero) dva = -dva
 
    ! Check for a uniform zero velocity in this direction.
    ! If so, set status = 2 and return (dt = 1.0d+20).
    tol = 1.0d-15
    if ((v2a .lt. tol) .and. (v1a .lt. tol)) then
      v = dzero
      dvdx = dzero
      status = 2
      itopbotexit = 0
      return
    end if
 
    ! Check for uniform non-zero velocity in this direction.
    ! If so, set compute dt using the constant velocity,
    ! set status = 1 and return.
    vv = v1a
    if (v2a .gt. vv) vv = v2a
    vvv = dva / vv
    if (vvv .lt. 1.0d-4) then
      zro = tol
      zrom = -zro
      v = v1
      x = xl * dx
      if (v1 .gt. zro) then
        dt = (dx - x) / v1
        itopbotexit = -2
      end if
      if (v1 .lt. zrom) then
        dt = -x / v1
        itopbotexit = -1
      end if
      dvdx = dzero
      status = 1
      return
    end if
 
    ! Velocity has a linear variation.
    ! Compute velocity corresponding to particle position
    dvdx = dv / dx
    v = (done - xl) * v1 + xl * v2
 
    ! If flow is into the cell from both sides there is no outflow.
    ! In that case, set status = 3 and return
    nooutflow = .true.
    if (v1 .lt. dzero) nooutflow = .false.
    if (v2 .gt. dzero) nooutflow = .false.
    if (nooutflow) then
      status = 3
      itopbotexit = 0
      return
    end if
 
    ! If there is a divide in the cell for this flow direction, check to see if the
    ! particle is located exactly on the divide. If it is, move it very slightly to
    ! get it off the divide. This avoids possible numerical problems related to
    ! stagnation points.
    if ((v1 .le. dzero) .and. (v2 .ge. dzero)) then
      if (abs(v) .le. dzero) then
        v = 1.0d-20
        if (v2 .le. dzero) v = -v
      end if
    end if
 
    ! If there is a flow divide, find out what side of the divide the particle
    ! is on and set the value of vr appropriately to reflect that location.
    vr1 = v1 / v
    vr2 = v2 / v
    vr = vr1
    itopbotexit = -1
    if (vr .le. dzero) then
      vr = vr2
      itopbotexit = -2
    end if
 
    ! Check if velocity is in the same direction throughout cell (i.e. no flow divide).
    ! Check if product v1*v2 > 0 then the velocity is in the same direction throughout
    ! the cell (i.e. no flow divide). If so, set vr to reflect appropriate direction.
    v1v2 = v1 * v2
    if (v1v2 .gt. dzero) then
      if (v .gt. dzero) then
        vr = vr2
        itopbotexit = -2
      end if
      if (v .lt. dzero) then
        vr = vr1
        itopbotexit = -1
      end if
    end if
 
    ! Compute travel time to exit face. Return with status = 0
    dt = log(vr) / dvdx
    status = 0

Here is the caller graph for this function:

calculate_xyz_position()

subroutine methodsubcellternarymodule::calculate_xyz_position ( real(dp)  dt, real(dp)  rxx, real(dp)  rxy, real(dp)  ryx, real(dp)  ryy, real(dp)  sxx, real(dp)  sxy, real(dp)  syy, integer(i4b)  izstatus, real(dp)  x0, real(dp)  y0, real(dp)  az, real(dp)  vzi, real(dp)  vzbot, real(dp)  ztop, real(dp)  zbot, real(dp)  zi, real(dp)  x, real(dp)  y, real(dp)  z, integer(i4b), optional  exitFace  )

private

Definition at line 425 of file MethodSubcellTernary.f90.

    ! dummy
    real(DP) :: dt
    real(DP) :: rxx
    real(DP) :: rxy
    real(DP) :: ryx
    real(DP) :: ryy
    real(DP) :: sxx
    real(DP) :: sxy
    real(DP) :: syy
    integer(I4B) :: izstatus
    real(DP) :: x0
    real(DP) :: y0
    real(DP) :: az
    real(DP) :: vzi
    real(DP) :: vzbot
    real(DP) :: ztop
    real(DP) :: zbot
    real(DP) :: zi
    real(DP) :: x
    real(DP) :: y
    real(DP) :: z
    integer(I4B), optional :: exitFace
    ! local
    integer(I4B) :: lexitface
    real(DP) :: rot(2, 2), res(2), loc(2)
    real(DP) :: alp
    real(DP) :: bet
 
    ! process optional exit face argument
    if (present(exitface)) then
      lexitface = exitface
    else
      lexitface = 0
    end if
 
    ! calculate alpha and beta
    call step_analytical(dt, alp, bet)
 
    ! if exit face is known, set alpha or beta coordinate
    ! corresponding to the exit face exactly.
    if (lexitface .eq. 1) then
      bet = dzero
    else if (lexitface .eq. 2) then
      alp = done - bet
    else if (lexitface .eq. 3) then
      alp = dzero
    end if
 
    ! if exit face is top or bottom, set z coordinate exactly.
    if (lexitface .eq. 4) then
      z = zbot
    else if (lexitface .eq. 5) then
      z = ztop
    else
      ! otherwise calculate z.
      if (izstatus .eq. 2) then
        ! -- vz uniformly zero
        z = zi
      else if (izstatus .eq. 1) then
        ! -- vz uniform, nonzero
        z = zi + vzi * dt
      else
        ! -- vz nonuniform
        z = zbot + (vzi * dexp(az * dt) - vzbot) / az
      end if
    end if
 
    ! transform (alp, beta) to (x, y)
    loc = (/alp, bet/)
    loc = skew(loc, (/sxx, sxy, syy/), invert=.true.)
    rot = reshape((/rxx, rxy, ryx, ryy/), shape(rot))
    res = matmul(rot, loc) ! rotate vector
    x = res(1) + x0
    y = res(2) + y0
 

Here is the call graph for this function:

Here is the caller graph for this function:

create_method_subcell_ternary()

subroutine, public methodsubcellternarymodule::create_method_subcell_ternary

(

type(methodsubcellternarytype), pointer

method

)

Definition at line 32 of file MethodSubcellTernary.f90.

    ! -- dummy
    type(MethodSubcellTernaryType), pointer :: method
    ! -- local
    type(SubcellTriType), pointer :: subcell
 
    allocate (method)
    call create_subcell_tri(subcell)
    method%subcell => subcell
    method%type => method%subcell%type
    method%delegates = .false.

Here is the call graph for this function:

Here is the caller graph for this function:

deallocate()

subroutine methodsubcellternarymodule::deallocate ( class(methodsubcellternarytype), intent(inout)  this )

private

Definition at line 46 of file MethodSubcellTernary.f90.

    class(MethodSubcellTernaryType), intent(inout) :: this
    deallocate (this%type)

track_subcell()

subroutine methodsubcellternarymodule::track_subcell ( class(methodsubcellternarytype), intent(inout)  this, class(subcelltritype), intent(in)  subcell, type(particletype), intent(inout), pointer  particle, real(dp), intent(in)  tmax  )

private

Definition at line 64 of file MethodSubcellTernary.f90.

    ! dummy
    class(MethodSubcellTernaryType), intent(inout) :: this
    class(SubcellTriType), intent(in) :: subcell
    type(ParticleType), pointer, intent(inout) :: particle
    real(DP), intent(in) :: tmax
    ! local
    integer(I4B) :: exitFace
    real(DP) :: x0
    real(DP) :: y0
    real(DP) :: x1
    real(DP) :: y1
    real(DP) :: x2
    real(DP) :: y2
    real(DP) :: v0x
    real(DP) :: v0y
    real(DP) :: v1x
    real(DP) :: v1y
    real(DP) :: v2x
    real(DP) :: v2y
    real(DP) :: xi
    real(DP) :: yi
    real(DP) :: zi
    real(DP) :: zirel
    real(DP) :: ztop
    real(DP) :: zbot
    real(DP) :: dz
    real(DP) :: rxx
    real(DP) :: rxy
    real(DP) :: ryx
    real(DP) :: ryy
    real(DP) :: sxx
    real(DP) :: sxy
    real(DP) :: syy
    real(DP) :: alp0
    real(DP) :: bet0
    real(DP) :: alp1
    real(DP) :: bet1
    real(DP) :: alp2
    real(DP) :: bet2
    real(DP) :: alpi
    real(DP) :: beti
    real(DP) :: gami
    real(DP) :: vzbot
    real(DP) :: vztop
    real(DP) :: vzi
    real(DP) :: vziodz
    real(DP) :: az
    real(DP) :: dtexitz
    real(DP) :: dt
    real(DP) :: t
    real(DP) :: t0
    real(DP) :: dtexitxy
    real(DP) :: texit
    real(DP) :: x
    real(DP) :: y
    real(DP) :: z
    integer(I4B) :: izstatus
    integer(I4B) :: itopbotexit
    integer(I4B) :: ntmax
    integer(I4B) :: isolv
    integer(I4B) :: itrifaceenter
    integer(I4B) :: itrifaceexit
    real(DP) :: tol
    real(DP) :: dtexit
    real(DP) :: alpexit
    real(DP) :: betexit
    integer(I4B) :: reason
    integer(I4B) :: i
 
    ! Set solution method
    if (particle%iexmeth == 0) then
      isolv = 1 ! default to Brent's
    else
      isolv = particle%iexmeth
    end if
 
    ntmax = 10000
    tol = particle%extol
    reason = -1
 
    ! Set some local variables for convenience.
    xi = particle%x
    yi = particle%y
    zi = particle%z
    x0 = subcell%x0
    y0 = subcell%y0
    x1 = subcell%x1
    y1 = subcell%y1
    x2 = subcell%x2
    y2 = subcell%y2
    v0x = subcell%v0x
    v0y = subcell%v0y
    v1x = subcell%v1x
    v1y = subcell%v1y
    v2x = subcell%v2x
    v2y = subcell%v2y
    zbot = subcell%zbot
    ztop = subcell%ztop
    dz = subcell%dz
    vzbot = subcell%vzbot
    vztop = subcell%vztop
 
    ! Transform coordinates to the "canonical" configuration:
    ! barycentric in two dimensions with alpha, beta & gamma
    ! such that at f2 alpha = 0, f0 beta = 0, f1 gamma = 0.
    !
    !     v2
    !     |\
    !   f2| \f1
    !     |__\
    !   v0 f0 v1
    !
    call canonical(x0, y0, x1, y1, x2, y2, &
                   v0x, v0y, v1x, v1y, v2x, v2y, &
                   xi, yi, &
                   rxx, rxy, ryx, ryy, &
                   sxx, sxy, syy, &
                   alp0, bet0, alp1, bet1, alp2, bet2, alpi, beti)
 
    ! Clamp particle coordinates to the canonical triangular
    ! subcell and nudge it ever so slightly inside if needed.
    call clamp_bary(alpi, beti, gami, pad=dsame * dep3)
 
    ! Do calculations related to the analytical z solution.
    ! todo: just once for each cell? store at cell-level?
    zirel = (zi - zbot) / dz
    call calculate_dt(vzbot, vztop, dz, zirel, vzi, &
                      az, dtexitz, izstatus, &
                      itopbotexit)
    vziodz = vzi / dz
 
    ! If possible, track the particle across the subcell.
    itrifaceenter = particle%iboundary(3) - 1
    if (itrifaceenter == -1) itrifaceenter = 999
    call traverse_triangle(isolv, tol, &
                           dtexitxy, alpexit, betexit, &
                           itrifaceenter, itrifaceexit, &
                           alp1, bet1, alp2, bet2, alpi, beti)
 
    ! If the subcell has no exit face, terminate the particle.
    ! todo: after initial release, consider ramifications
    if (itopbotexit == 0 .and. itrifaceexit == 0) then
      particle%istatus = 9
      particle%advancing = .false.
      call this%save(particle, reason=3)
      return
    end if
 
    ! Determine the particle's exit face and travel time to exit.
    ! The exit face is the face through which it would exit first,
    ! considering only the velocity component in the direction of
    ! the face. Then compute the particle's exit time.
    if (itrifaceexit /= 0) then
      ! Exit through lateral subcell face
      exitface = itrifaceexit
      dtexit = dtexitxy
    else if (dtexitz < dtexitxy) then
      ! Exit through top or bottom
      if (itopbotexit == -1) then
        exitface = 4
      else
        exitface = 5
      end if
      dtexit = dtexitz
    end if
    texit = particle%ttrack + dtexit
    t0 = particle%ttrack
 
    ! Select user tracking times to solve. If this is the first time step
    ! of the simulation, include all times before it begins; if it is the
    ! last time step include all times after it ends only if the 'extend'
    ! option is on, otherwise times in this period and time step only.
    call this%tracktimes%advance()
    if (this%tracktimes%any()) then
      do i = this%tracktimes%selection(1), this%tracktimes%selection(2)
        t = this%tracktimes%times(i)
        if (t < particle%ttrack) cycle
        if (t >= texit .or. t >= tmax) exit
        dt = t - t0
        call calculate_xyz_position(dt, rxx, rxy, ryx, ryy, sxx, sxy, syy, &
                                    izstatus, x0, y0, az, vzi, vzbot, &
                                    ztop, zbot, zi, x, y, z)
        particle%x = x
        particle%y = y
        particle%z = z
        particle%ttrack = t
        particle%istatus = 1
        call this%save(particle, reason=5)
      end do
    end if
 
    ! Compute exit time and face and update the particle's coordinates
    ! (local, unscaled) and other properties. The particle may at this
    ! point lie on a boundary of the subcell or may still be within it.
    if (texit .gt. tmax) then
      ! -- The computed exit time is greater than the maximum time, so set
      ! -- final time for particle trajectory equal to maximum time.
      t = tmax
      dt = t - t0
      exitface = 0
      particle%istatus = 1
      particle%advancing = .false.
      reason = 2 ! timestep end
    else
      ! -- The computed exit time is less than or equal to the maximum time,
      ! -- so set final time for particle trajectory equal to exit time.
      t = texit
      dt = dtexit
      reason = 1 ! (sub)cell transition
    end if
    call calculate_xyz_position(dt, rxx, rxy, ryx, ryy, sxx, sxy, syy, &
                                izstatus, x0, y0, az, vzi, vzbot, &
                                ztop, zbot, zi, x, y, z, exitface)
    particle%x = x
    particle%y = y
    particle%z = z
    particle%ttrack = t
    particle%iboundary(3) = exitface
    call this%save(particle, reason=reason)

Here is the call graph for this function: