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The model equation to be solved is of the form:
∂T/∂t = α(∂2T/∂x2 + ∂2T/∂y2) + S(x)
*        A. Salih, Dept. of Mechanical Engg., NIT - Trichy, India.      *
*************************************************************************
*       THIS PROGRAM SOLVES TRANSIENT HEAT EQUATION IN A 2-D DOMAIN     *
*                  USING FINITE VOLUME METHOD (UNIFORM CV)              *
*                   GENERAL IMPLICIT METHOD (BETA METHOD)               *
*************************************************************************
*
      program IMPLICIT_2D
      implicit doubleprecision (a-h,o-z)
      include 'scalars/integers.inc'
      include 'scalars/parameters.inc'
      open(unit=11,file='input.dat',status='unknown')
      open(unit=21,file='output.dat',status='unknown')
      open(unit=31,file='outputs/x.dat',status='unknown')
      open(unit=32,file='outputs/y.dat',status='unknown')
      open(unit=33,file='outputs/tmp.dat',status='unknown')
      open(unit=34,file='outputs/time.dat',status='unknown')
      open(unit=35,file='outputs/time2.dat',status='unknown')
      open(unit=36,file='outputs/t_trans.dat',status='unknown')
      open(unit=37,file='outputs/iterations.dat',status='unknown')
c
      pi = 4*datan(1d0)
c
      CALL READ_IN          ! read-in data
      close (unit=11)

      CALL GRID             ! setting up the grid points in the domain

      CALL INITIAL_COND     ! setting up initial condition

      CALL BOUNDARY_COND    ! setting up boundary values

      CALL SOLVE            ! setting up system of equations
      
      CALL PRINTOUT         ! printing out the computational results

      CALL WRITE_OUT     ! write-out the basic data used for computation
c
      stop
      end
*
***SUBROUTINE: READING IN THE BASIC DATA *******************************
*
      subroutine READ_IN
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'scalars/solveparams.inc'
c
      read(11,*) alx            ! actual length of domain
      read(11,*) aly            ! actual length of domain
      read(11,*) boundary_type  ! flag for type of boundary conditions
      read(11,*) alpha          ! thermal diffusivity
      read(11,*) Fo             ! value of mean grid Fourier number for 
                                ! calculating the time step
      read(11,*) solver         ! flag for type of solver to be used
      read(11,*) tolsor         ! tolerance value for terminating the
                                ! iteration (for SOR method)
      read(11,*) wtsor          ! relaxation factor for SOR
      read(11,*) wtlsor         ! relaxation factor for Line SOR
      read(11,*) itermax        ! maximum number of iterations (for solver)

      read(11,*) tolstdy        ! convergence criterion for steady-state
      read(11,*) tfinal         ! time at which the solution is desired
      read(11,*) print_freq     !
      read(11,*) beta           ! weight factor for implicit method
                                ! 0-FTCS, 1-BTCS, 0.5-Crank-Nicolson
c
      if (beta < 5d-1) then
         Fourier = 1d0 / (4*(1-2*beta))
         write(*,*)''
         print*, 'The mean Fourier number supplied for the given value of'
         print*, 'beta =',beta, 'must be less than', Fourier
         write(*,*)''
         print*, 'Press Enter to continue'
         read(*,*)
      endif
c
c     calculation of time-step dt based on the stability condition
      dx = alx /(m-2)
      dy = aly /(n-2)
      dt = 2*Fo *(dx**2 * dy**2)/(dx**2 + dy**2) /alpha
      maxntimestp = tfinal /dt
      dt  = tfinal /maxntimestp        ! revised time-step
      Fox = alpha*dt/dx**2
      Foy = alpha*dt/dy**2
      Fo  = (Fox + Foy)/2d0            ! revised mean Fourier number
      if (tfinal < dt) then
         print*, 'Warning: final time is less than time-step!'
         stop
      endif
c
      return
      end
*
***SUBROUTINE: WRITING OUT THE BASIC DATA USED FOR COMPUTATION**********
*
      subroutine WRITE_OUT
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'scalars/boundaryvalues.inc'
c
      if (boundary_type == 1) then
         write(21,*) 'Dirichlet bc is specified on all boundaries'
      elseif (boundary_type == 2) then
         write(21,*) 'Dirichlet on W,E,N   Neumann on S'
      endif
      write(21,*) 'Thermal diffusivity', alpha
      write(21,*) 'Mean grid Fourier number, Fo =', Fo
      write(21,*) 'Length of the domain in x-direction', alx
      write(21,*) 'Length of the domain in y-direction', aly
      write(21,*) 'Number of control volumes:', nx, '     X', ny
      write(21,*) 'dx =', dx
      write(21,*) 'dy =', dy
      write(21,*) 'dt =', dt
      write(21,*) 'No. of Time step = ', ntimestp
      write(21,*) 'Final time = ', time
      write(21,*) 'convergence criterion for steady-state solution:',
     $tolstdy
      write(21,*) 'Weight factor for the implicit scheme = ', beta
c
      if (beta == 0d0) then
         ! nothing
      elseif (solver == 1) then
         write(21,*) 'The solver used is PSOR'
      elseif (solver == 2) then
         write(21,*) 'The solver used is LSOR'
      endif
c
      return
      end
*
****SUBROUTINE: GRID****************************************************
*
      SUBROUTINE GRID
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'arrays/grid.inc'
c
c     m-2 = number of control volumes the in x-direction
c     n-2 = number of control volumes the in y-direction
      dx   = alx /(m-2)
      x(1) = 0
      x(2) = x(1) + dx/2d0
      do i = 3, m-1
         x(i) = x(i-1) + dx
      enddo
      x(m) = x(m-1) + dx/2d0
c
      dy   = aly /(n-2)
      y(1) = 0
      y(2) = y(1) + dy/2d0
      do i = 3, n-1
         y(i) = y(i-1) + dy
      enddo
      y(n) = y(n-1) + dy/2d0
c
      return
      end
*
***SUBROUTINE: BOUNDARY CONDITIONS FOR TEMPERATURE**********************
*
      SUBROUTINE BOUNDARY_COND
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'scalars/boundaryvalues.inc'
      include 'scalars/parameters.inc'
      include 'arrays/temperature.inc'
      include 'arrays/grid.inc'
c
c     defining the boundary conditions
      include 'bc/bc.inc'
c
c     boundary_type: 1  - dirichlet: all
c     boundary_type: 2  - dirichlet: W,E,N;   neumann: S;
c
      if (boundary_type == 1) then
c        west and east
         do j = 2, n-1
            TMP(1,j) = BTW(x(1),y(j))
            TMP(m,j) = BTE(x(m),y(j))
         enddo
c        south and north
         do i = 2, m-1
            TMP(i,1) = BTS(x(i),y(1))
            TMP(i,n) = BTN(x(i),y(n))
         enddo
c        corner boundary nodes
         TMP(1,1) = BTW(x(1),y(1))
         TMP(m,1) = BTE(x(m),y(1))
         TMP(1,n) = BTW(x(1),y(n))
         TMP(m,n) = BTE(x(m),y(n))
      elseif (boundary_type == 2) then
c        west and east
         do j = 2, n-1
            TMP(1,j) = BTW(x(1),y(j))
            TMP(m,j) = BTE(x(m),y(j))
         enddo
c        south and north
         do i = 2, m-1
            qs = BQS(x(i),y(1))
            TMP(i,n) = BTN(x(i),y(n))
         enddo
c        corner boundary nodes
         TMP(1,1) = BTW(x(1),y(1))
         TMP(m,1) = BTE(x(m),y(1))
         TMP(1,n) = BTW(x(1),y(n))
         TMP(m,n) = BTE(x(m),y(n))
      endif
c
      return
      end
*
***SUBROUTINE: INITIAL CONDITIONS FOR TEMPERATURE**********************
*
      SUBROUTINE INITIAL_COND
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'scalars/parameters.inc'
      include 'arrays/temperature.inc'
      include 'arrays/grid.inc'
c
c     defining the initial conditions
      TINIT(x,y,t) = 0   ! dsin(pi*x/alx)
c
      do j = 2, n-1
      do i = 2, m-1
         TMP(i,j) = TINIT(x(i),y(j),0)
      enddo
      enddo
c
      return
      end
*
***SUBROUTINE: CONSTRUCTION OF SYSTEM OF EQUATION AND ITS SOLUTION******
*
      subroutine SOLVE
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'scalars/boundaryvalues.inc'
      include 'scalars/parameters.inc'
      include 'arrays/grid.inc'
      include 'arrays/temperature.inc'
      include 'arrays/coeff.inc'
      doubleprecision TN(0:m1,0:n1), maxdif
c
      include 'arithmeticfunctions/source.inc'    ! source.inc file
                           ! contains the definition of source term
c
c     storing the values of temperature at nth time level
      TN = TMP
c
      ntimestp = 0
      maxdif = 1d9
      time = 0d0
      write(34,101) time        ! continuous time
      write(35,101) time        ! periodic time
      monitorx = nx/4
      monitory = ny/4
      write(36,*) TMP(monitorx,monitory)
c
      write(37,*) 'Number of iterations by solver at each time step'
c
10    if ((maxdif > tolstdy).and.(ntimestp < maxntimestp)) then
c        construction of coefficient matrix
         do j = 3, n-2
         do i = 3, m-2
            AS(i,j) = -beta *Foy
            AW(i,j) = -beta *Fox
            AE(i,j) = -beta *Fox
            AN(i,j) = -beta *Foy
            AP(i,j) = 1d0 - (AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
         enddo
         enddo
c        construction of RHS vector
         do j = 3, n-2
         do i = 3, m-2
            C(i,j) = TN(i,j) + (1d0 - beta)* (
     $      Fox*(TN(i-1,j) - 2*TN(i,j) + TN(i+1,j)) +
     $      Foy*(TN(i,j-1) - 2*TN(i,j) + TN(i,j+1)) ) + S(x(i),y(j))*dt
         enddo
         enddo
c
c        incorporation of boundary conditions:
c
c        boundary_type: 1  - dirichlet: all
c        boundary_type: 2  - dirichlet: W,E,N;   neumann: S;
c
         if (boundary_type == 1) then
c           west
            i = 2
            do j = 3, n-2
               AS(i,j) = -beta *Foy
               AW(i,j) = -8d0/3d0 *beta *Fox
               AE(i,j) = -4d0/3d0 *beta *Fox
               AN(i,j) = -beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(8*TN(i-1,j) - 12*TN(i,j) + 4*TN(i+1,j))/3d0 +
     $          Foy*(TN(i,j-1) - 2*TN(i,j) + TN(i,j+1)) ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AW(i,j)*TMP(i-1,j)
               AW(i,j) = 0
            enddo
c           east
            i = m-1
            do j = 3, n-2
               AS(i,j) = -beta *Foy
               AW(i,j) = -4d0/3d0 *beta *Fox
               AE(i,j) = -8d0/3d0 *beta *Fox
               AN(i,j) = -beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(4*TN(i-1,j) - 12*TN(i,j) + 8*TN(i+1,j))/3d0 +
     $          Foy*(TN(i,j-1) - 2*TN(i,j) + TN(i,j+1)) ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AE(i,j)*TMP(i+1,j)
               AE(i,j) = 0
            enddo
c           south
            j = 2
            do i = 3, m-2
               AS(i,j) = -8d0/3d0 *beta *Foy
               AW(i,j) = -beta *Fox
               AE(i,j) = -beta *Fox
               AN(i,j) = -4d0/3d0 *beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(TN(i-1,j) - 2*TN(i,j) + TN(i+1,j)) +
     $          Foy*(8*TN(i,j-1) - 12*TN(i,j) + 4*TN(i,j+1))/3d0 ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AS(i,j)*TMP(i,j-1)
               AS(i,j) = 0
            enddo
c           north
            j = n-1
            do i = 3, m-2
               AS(i,j) = -4d0/3d0 *beta *Foy
               AW(i,j) = -beta *Fox
               AE(i,j) = -beta *Fox
               AN(i,j) = -8d0/3d0 *beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(TN(i-1,j) - 2*TN(i,j) + TN(i+1,j)) +
     $          Foy*(4*TN(i,j-1) - 12*TN(i,j) + 8*TN(i,j+1))/3d0 ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AN(i,j)*TMP(i,j+1)
               AN(i,j) = 0
            enddo
c           south-west
            i = 2
            j = 2
            AS(i,j) = -8d0/3d0 *beta *Foy
            AW(i,j) = -8d0/3d0 *beta *Fox
            AE(i,j) = -4d0/3d0 *beta *Fox
            AN(i,j) = -4d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(8*TN(i-1,j) - 12*TN(i,j) + 4*TN(i+1,j))/3d0 +
     $       Foy*(8*TN(i,j-1) - 12*TN(i,j) + 4*TN(i,j+1))/3d0 ) +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AS(i,j)*TMP(i,j-1) - AW(i,j)*TMP(i-1,j)
            AS(i,j) = 0
            AW(i,j) = 0
c           south-east
            i = m-1
            j = 2
            AS(i,j) = -8d0/3d0 *beta *Foy
            AW(i,j) = -4d0/3d0 *beta *Fox
            AE(i,j) = -8d0/3d0 *beta *Fox
            AN(i,j) = -4d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(4*TN(i-1,j) - 12*TN(i,j) + 8*TN(i+1,j))/3d0 +
     $       Foy*(8*TN(i,j-1) - 12*TN(i,j) + 4*TN(i,j+1))/3d0 ) +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AS(i,j)*TMP(i,j-1) - AE(i,j)*TMP(i+1,j)
            AS(i,j) = 0
            AE(i,j) = 0
c           north-west
            i = 2
            j = n-1
            AS(i,j) = -4d0/3d0 *beta *Foy
            AW(i,j) = -8d0/3d0 *beta *Fox
            AE(i,j) = -4d0/3d0 *beta *Fox
            AN(i,j) = -8d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(8*TN(i-1,j) - 12*TN(i,j) + 4*TN(i+1,j))/3d0 +
     $       Foy*(4*TN(i,j-1) - 12*TN(i,j) + 8*TN(i,j+1))/3d0 ) +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AW(i,j)*TMP(i-1,j) - AN(i,j)*TMP(i,j+1)
            AW(i,j) = 0
            AN(i,j) = 0
c           north-east
            i = m-1
            j = n-1
            AS(i,j) = -4d0/3d0 *beta *Foy
            AW(i,j) = -4d0/3d0 *beta *Fox
            AE(i,j) = -8d0/3d0 *beta *Fox
            AN(i,j) = -8d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(4*TN(i-1,j) - 12*TN(i,j) + 8*TN(i+1,j))/3d0 +
     $       Foy*(4*TN(i,j-1) - 12*TN(i,j) + 8*TN(i,j+1))/3d0 ) +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AE(i,j)*TMP(i+1,j) - AN(i,j)*TMP(i,j+1)
            AE(i,j) = 0
            AN(i,j) = 0
         elseif (boundary_type == 2) then
c           west
            i = 2
            do j = 3, n-2
               AS(i,j) = -beta *Foy
               AW(i,j) = -8d0/3d0 *beta *Fox
               AE(i,j) = -4d0/3d0 *beta *Fox
               AN(i,j) = -beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(8*TN(i-1,j) - 12*TN(i,j) + 4*TN(i+1,j))/3d0 +
     $          Foy*(TN(i,j-1) - 2*TN(i,j) + TN(i,j+1)) ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AW(i,j)*TMP(i-1,j)
               AW(i,j) = 0
            enddo
c           east
            i = m-1
            do j = 3, n-2
               AS(i,j) = -beta *Foy
               AW(i,j) = -4d0/3d0 *beta *Fox
               AE(i,j) = -8d0/3d0 *beta *Fox
               AN(i,j) = -beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(4*TN(i-1,j) - 12*TN(i,j) + 8*TN(i+1,j))/3d0 +
     $          Foy*(TN(i,j-1) - 2*TN(i,j) + TN(i,j+1)) ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AE(i,j)*TMP(i+1,j)
               AE(i,j) = 0
            enddo
c           south
            j = 2
            do i = 3, m-2
               AS(i,j) = 0
               AW(i,j) = -beta *Fox
               AE(i,j) = -beta *Fox
               AN(i,j) = -beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(TN(i-1,j) - 2*TN(i,j) + TN(i+1,j)) +
     $          Foy*(TN(i,j+1) - TN(i,j)) ) - qs*Foy*dy +
     $          S(x(i),y(j))*dt
            enddo
c           north
            j = n-1
            do i = 3, m-2
               AS(i,j) = -4d0/3d0 *beta *Foy
               AW(i,j) = -beta *Fox
               AE(i,j) = -beta *Fox
               AN(i,j) = -8d0/3d0 *beta *Foy
               AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
               C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $          Fox*(TN(i-1,j) - 2*TN(i,j) + TN(i+1,j)) +
     $          Foy*(4*TN(i,j-1) - 12*TN(i,j) + 8*TN(i,j+1))/3d0 ) +
     $          S(x(i),y(j))*dt
               C(i,j)  = C(i,j) - AN(i,j)*TMP(i,j+1)
               AN(i,j) = 0
            enddo
c           south-west
            i = 2
            j = 2
            AS(i,j) = 0
            AW(i,j) = -8d0/3d0 *beta *Fox
            AE(i,j) = -4d0/3d0 *beta *Fox
            AN(i,j) = -4d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(8*TN(i-1,j) - 12*TN(i,j) + 4*TN(i+1,j))/3d0 +
     $       Foy*(TN(i,j+1) - TN(i,j)) ) - qs*Foy*dy +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AW(i,j)*TMP(i-1,j)
            AW(i,j) = 0
c           south-east
            i = m-1
            j = 2
            AS(i,j) = 0
            AW(i,j) = -4d0/3d0 *beta *Fox
            AE(i,j) = -8d0/3d0 *beta *Fox
            AN(i,j) = -4d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(4*TN(i-1,j) - 12*TN(i,j) + 8*TN(i+1,j))/3d0 +
     $       Foy*(TN(i,j+1) - TN(i,j)) ) - qs*Foy*dy +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AE(i,j)*TMP(i+1,j)
            AE(i,j) = 0
c           north-west
            i = 2
            j = n-1
            AS(i,j) = -4d0/3d0 *beta *Foy
            AW(i,j) = -8d0/3d0 *beta *Fox
            AE(i,j) = -4d0/3d0 *beta *Fox
            AN(i,j) = -8d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(8*TN(i-1,j) - 12*TN(i,j) + 4*TN(i+1,j))/3d0 +
     $       Foy*(4*TN(i,j-1) - 12*TN(i,j) + 8*TN(i,j+1))/3d0 ) +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AW(i,j)*TMP(i-1,j) - AN(i,j)*TMP(i,j+1)
            AW(i,j) = 0
            AN(i,j) = 0
c           north-east
            i = m-1
            j = n-1
            AS(i,j) = -4d0/3d0 *beta *Foy
            AW(i,j) = -4d0/3d0 *beta *Fox
            AE(i,j) = -8d0/3d0 *beta *Fox
            AN(i,j) = -8d0/3d0 *beta *Foy
            AP(i,j) = 1d0 -(AS(i,j) + AW(i,j) + AE(i,j) + AN(i,j))
            C(i,j)  = TN(i,j) + (1d0 - beta)* (
     $       Fox*(4*TN(i-1,j) - 12*TN(i,j) + 8*TN(i+1,j))/3d0 +
     $       Foy*(4*TN(i,j-1) - 12*TN(i,j) + 8*TN(i,j+1))/3d0 ) +
     $       S(x(i),y(j))*dt
            C(i,j)  = C(i,j) - AE(i,j)*TMP(i+1,j) - AN(i,j)*TMP(i,j+1)
            AE(i,j) = 0
            AN(i,j) = 0
         endif
c
c        solution of system of algebraic equation
         if (beta == 0d0) then   ! no system of eqns to be solved
            do j = 2, n-1
            do i = 2, m-1
               TMP(i,j) = C(i,j)
            enddo
            enddo
         elseif (solver == 1) then
            CALL SOR(TMP)             ! point SOR
         elseif (solver == 2) then
            CALL LSOR(TMP)            ! line SOR
         endif
c
         time     = time + dt
         ntimestp = ntimestp + 1
c
         maxdif = 0
         do j = 2, n-1
         do i = 2, m-1
              dif = TMP(i,j) - TN(i,j)
              if (dabs(dif) > maxdif) then
                   maxdif = dabs(dif)
              endif
         enddo
         enddo
c
c        updating the temperature
         TN = TMP
c
         write(34,101) time              ! continuous time
         write(6,102) ntimestp, maxdif
c
c        printing out transient temperature at selected point of domain
         j = jcounter + 1
         jcounter = mod(j,print_freq)
         if (jcounter == 0) then
            write(35,101) (time + dt)    ! periodic time
            write(36,*) TMP(monitorx,monitory)
         endif
         go to 10
      endif
c
101   format(e14.7)
102   format(i7,5x,e14.7)
c
c     calculation of boundary temperatures where Neumann BC is specified
      if (boundary_type == 1) then
            !
      elseif (boundary_type == 2) then
c        south
         j = 1
         do i = 1, m
            TMP(i,j) = (9*TMP(i,j+1) - TMP(i,j+2) - 3*qs*dy) /8d0
         enddo
      endif
c
      return
      end
*
**SUBROUTINE: POINT SOR FOR TRIDIAGONAL MATRIX**************************
*
      SUBROUTINE SOR(X)
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/solveparams.inc'
      include 'arrays/coeff.inc'
      doubleprecision X(0:m1,0:n1)
c
      mm   = m-1
      nn   = n-1
      iter = 1
      wt   = wtsor
      relresidual = 1d9            ! maximum norm of relative residual
c
c     calculation of maximum norm of rhs vector
      rhsnorm = 0
      do j = 2, nn
      do i = 2, mm
         rhsnorm = max(rhsnorm, dabs(C(i,j)))
      enddo
      enddo
      rhsnorm = rhsnorm + 1d-30     ! avoid overflow if rhsnorm is zero
c
10    if ((relresidual > tolsor).and.(iter < itermax)) then
         do j = 2, nn
         do i = 2, mm
            xold = X(i,j)
            xnew = (C(i,j)- AS(i,j)*X(i,j-1) - AW(i,j)*X(i-1,j) 
     $                    - AE(i,j)*X(i+1,j) - AN(i,j)*X(i,j+1))/AP(i,j)
            X(i,j) = wt*xnew + (1d0 - wt)*xold
         enddo
         enddo
c
c        compute new max-norm of residual vector
         residnorm = 0
         do j = 2, nn
         do i = 2, mm
            res = C(i,j) -(AS(i,j)*X(i,j-1) + AW(i,j)*X(i-1,j) + AP(i,j)
     $                    *X(i,j) + AE(i,j)*X(i+1,j) + AN(i,j)*X(i,j+1))
            residnorm = max(residnorm, dabs(res))
         enddo
         enddo
         relresidual = residnorm /rhsnorm
*        write(333,101) iter, relresidual
         iter = iter + 1
         go to 10
      endif
c
      if (relresidual > tolsor) then
         write(21,*) 'Tolerance condition for SOR is not met'
      endif
      write(37,*) iter
*101  format('',3x,i4,4x,e10.3)
c
      return
      end
*
***SUBROUTINE: LINE SOR FOR NONADJACENT PENTADIAGONAL MATRIX************
*
      subroutine LSOR(X)
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/solveparams.inc'
      include 'arrays/coeff.inc'
      doubleprecision X(0:m1,0:n1)
      parameter( mn = max(m,n)+1 )
      doubleprecision LO(0:mn),DI(0:mn),UP(0:mn),CO(0:mn),XX(0:mn)
c
      mm   = m-1
      nn   = n-1
      iter = 1
      wt   = wtlsor
      relresidual = 1d9            ! maximum norm of relative residual
c
c     calculation of maximum norm of rhs vector
      rhsnorm = 0
      do j = 2, nn
      do i = 2, mm
         rhsnorm = max(rhsnorm, dabs(C(i,j)))
      enddo
      enddo
      rhsnorm = rhsnorm + 1d-30     ! avoid overflow if rhsnorm is zero
c
10    if ((relresidual > tolsor).and.(iter < itermax)) then
         do j = 2, nn
            do i = 2, mm
               LO(i) = wt*AW(i,j)
               DI(i) = AP(i,j)
               UP(i) = wt*AE(i,j)
               CO(i) = wt*(C(i,j) - AS(i,j)*X(i,j-1) - AN(i,j)*X(i,j+1))
     $                                         + (1 - wt)*AP(i,j)*X(i,j)
*     write(333,*) AS(i,j), AN(i,j)
            enddo
            CALL TDMA(LO,DI,UP,CO,XX)
            do i = 2, mm
               X(i,j) = XX(i)
            enddo
         enddo
c
c        compute new max-norm of residual vector
         residnorm = 0
         do j = 2, nn
         do i = 2, mm
            res = C(i,j) -(AS(i,j)*X(i,j-1) + AW(i,j)*X(i-1,j) + AP(i,j)
     $                    *X(i,j) + AE(i,j)*X(i+1,j) + AN(i,j)*X(i,j+1))
            residnorm = max(residnorm, dabs(res))
         enddo
         enddo
         relresidual = residnorm /rhsnorm
*        write(333,101) iter, relresidual
         iter = iter + 1
         go to 10
      endif
c
      if (relresidual > tolsor) then
         write(21,*) 'Tolerance condition for LSOR is not met'
      endif
      write(37,*) iter
*101  format('',3x,i4,4x,e10.3)
c
      return
      end
*
***SUBROUTINE: TDMA*****************************************************
*
      subroutine TDMA(L,D,U,C,X)
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      parameter( mn = max(m,n)+1 )
      doubleprecision L(0:mn),D(0:mn),U(0:mn),C(0:mn),X(0:mn)
      doubleprecision P(-1:mn),Q(-1:mn)
c
      P(1) = 0d0
      Q(1) = 0d0
c
c     forward elimination
      do i = 2, m-1
         denom =  D(i) + L(i)*P(i-1)
         P(i)  = -U(i) /denom
         Q(i)  = (C(i) - L(i)*Q(i-1)) /denom
      enddo
c
c     back substitution
      do i = m-1, 2, -1
         X(i) = P(i)*X(i+1) + Q(i)
      enddo
*
      return
      end
*
***SUBROUTINE: Printing-out the output data*****************************
*
      SUBROUTINE PRINTOUT
      implicit doubleprecision (a-h,o-z)
      include 'array_dimension.inc'
      include 'scalars/integers.inc'
      include 'scalars/reals.inc'
      include 'arrays/temperature.inc'
      include 'arrays/grid.inc'
c
      write(31,101) (x(i), i=1,m)
      write(32,101) (y(i), i=1,n)   
      write(33,102) ((TMP(i,j), i=1,m), j=1,n)
101   format(e13.6)
102   format(34(e13.6,1x))! format number = no. of CV in x-direction + 2
c
      return
      end