SLATEC Routines --- HSTCYL ---
*DECK HSTCYL
SUBROUTINE HSTCYL (A, B, M, MBDCND, BDA, BDB, C, D, N, NBDCND,
+ BDC, BDD, ELMBDA, F, IDIMF, PERTRB, IERROR, W)
C***BEGIN PROLOGUE HSTCYL
C***PURPOSE Solve the standard five-point finite difference
C approximation on a staggered grid to the modified
C Helmholtz equation in cylindrical coordinates.
C***LIBRARY SLATEC (FISHPACK)
C***CATEGORY I2B1A1A
C***TYPE SINGLE PRECISION (HSTCYL-S)
C***KEYWORDS CYLINDRICAL, ELLIPTIC, FISHPACK, HELMHOLTZ, PDE
C***AUTHOR Adams, J., (NCAR)
C Swarztrauber, P. N., (NCAR)
C Sweet, R., (NCAR)
C***DESCRIPTION
C
C HSTCYL solves the standard five-point finite difference
C approximation on a staggered grid to the modified Helmholtz
C equation in cylindrical coordinates
C
C (1/R)(d/dR)(R(dU/dR)) + (d/dZ)(dU/dZ)C
C + LAMBDA*(1/R**2)*U = F(R,Z)
C
C This two-dimensional modified Helmholtz equation results
C from the Fourier transform of a three-dimensional Poisson
C equation.
C
C * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
C
C * * * * * * * * Parameter Description * * * * * * * * * *
C
C * * * * * * On Input * * * * * *
C
C A,B
C The range of R, i.e. A .LE. R .LE. B. A must be less than B and
C A must be non-negative.
C
C M
C The number of grid points in the interval (A,B). The grid points
C in the R-direction are given by R(I) = A + (I-0.5)DR for
C I=1,2,...,M where DR =(B-A)/M. M must be greater than 2.
C
C MBDCND
C Indicates the type of boundary conditions at R = A and R = B.
C
C = 1 If the solution is specified at R = A (see note below) and
C R = B.
C
C = 2 If the solution is specified at R = A (see note below) and
C the derivative of the solution with respect to R is
C specified at R = B.
C
C = 3 If the derivative of the solution with respect to R is
C specified at R = A (see note below) and R = B.
C
C = 4 If the derivative of the solution with respect to R is
C specified at R = A (see note below) and the solution is
C specified at R = B.
C
C = 5 If the solution is unspecified at R = A = 0 and the solution
C is specified at R = B.
C
C = 6 If the solution is unspecified at R = A = 0 and the
C derivative of the solution with respect to R is specified at
C R = B.
C
C NOTE: If A = 0, do not use MBDCND = 1,2,3, or 4, but instead
C use MBDCND = 5 or 6. The resulting approximation gives
C the only meaningful boundary condition, i.e. dU/dR = 0.
C (see D. Greenspan, 'Introductory Numerical Analysis Of
C Elliptic Boundary Value Problems,' Harper and Row, 1965,
C Chapter 5.)
C
C BDA
C A one-dimensional array of length N that specifies the boundary
C values (if any) of the solution at R = A. When MBDCND = 1 or 2,
C
C BDA(J) = U(A,Z(J)) , J=1,2,...,N.
C
C When MBDCND = 3 or 4,
C
C BDA(J) = (d/dR)U(A,Z(J)) , J=1,2,...,N.
C
C When MBDCND = 5 or 6, BDA is a dummy variable.
C
C BDB
C A one-dimensional array of length N that specifies the boundary
C values of the solution at R = B. When MBDCND = 1,4, or 5,
C
C BDB(J) = U(B,Z(J)) , J=1,2,...,N.
C
C When MBDCND = 2,3, or 6,
C
C BDB(J) = (d/dR)U(B,Z(J)) , J=1,2,...,N.
C
C C,D
C The range of Z, i.e. C .LE. Z .LE. D. C must be less
C than D.
C
C N
C The number of unknowns in the interval (C,D). The unknowns in
C the Z-direction are given by Z(J) = C + (J-0.5)DZ,
C J=1,2,...,N, where DZ = (D-C)/N. N must be greater than 2.
C
C NBDCND
C Indicates the type of boundary conditions at Z = C
C and Z = D.
C
C = 0 If the solution is periodic in Z, i.e.
C U(I,J) = U(I,N+J).
C
C = 1 If the solution is specified at Z = C and Z = D.
C
C = 2 If the solution is specified at Z = C and the derivative
C of the solution with respect to Z is specified at
C Z = D.
C
C = 3 If the derivative of the solution with respect to Z is
C specified at Z = C and Z = D.
C
C = 4 If the derivative of the solution with respect to Z is
C specified at Z = C and the solution is specified at
C Z = D.
C
C BDC
C A one dimensional array of length M that specifies the boundary
C values of the solution at Z = C. When NBDCND = 1 or 2,
C
C BDC(I) = U(R(I),C) , I=1,2,...,M.
C
C When NBDCND = 3 or 4,
C
C BDC(I) = (d/dZ)U(R(I),C), I=1,2,...,M.
C
C When NBDCND = 0, BDC is a dummy variable.
C
C BDD
C A one-dimensional array of length M that specifies the boundary
C values of the solution at Z = D. when NBDCND = 1 or 4,
C
C BDD(I) = U(R(I),D) , I=1,2,...,M.
C
C When NBDCND = 2 or 3,
C
C BDD(I) = (d/dZ)U(R(I),D) , I=1,2,...,M.
C
C When NBDCND = 0, BDD is a dummy variable.
C
C ELMBDA
C The constant LAMBDA in the modified Helmholtz equation. If
C LAMBDA is greater than 0, a solution may not exist. However,
C HSTCYL will attempt to find a solution. LAMBDA must be zero
C when MBDCND = 5 or 6.
C
C F
C A two-dimensional array that specifies the values of the right
C side of the modified Helmholtz equation. For I=1,2,...,M
C and J=1,2,...,N
C
C F(I,J) = F(R(I),Z(J)) .
C
C F must be dimensioned at least M X N.
C
C IDIMF
C The row (or first) dimension of the array F as it appears in the
C program calling HSTCYL. This parameter is used to specify the
C variable dimension of F. IDIMF must be at least M.
C
C W
C A one-dimensional array that must be provided by the user for
C work space. W may require up to 13M + 4N + M*INT(log2(N))
C locations. The actual number of locations used is computed by
C HSTCYL and is returned in the location W(1).
C
C
C * * * * * * On Output * * * * * *
C
C F
C Contains the solution U(I,J) of the finite difference
C approximation for the grid point (R(I),Z(J)) for
C I=1,2,...,M, J=1,2,...,N.
C
C PERTRB
C If a combination of periodic, derivative, or unspecified
C boundary conditions is specified for a Poisson equation
C (LAMBDA = 0), a solution may not exist. PERTRB is a con-
C stant, calculated and subtracted from F, which ensures
C that a solution exists. HSTCYL then computes this
C solution, which is a least squares solution to the
C original approximation. This solution plus any constant is also
C a solution; hence, the solution is not unique. The value of
C PERTRB should be small compared to the right side F.
C Otherwise, a solution is obtained to an essentially different
C problem. This comparison should always be made to insure that
C a meaningful solution has been obtained.
C
C IERROR
C An error flag that indicates invalid input parameters.
C Except for numbers 0 and 11, a solution is not attempted.
C
C = 0 No error
C
C = 1 A .LT. 0
C
C = 2 A .GE. B
C
C = 3 MBDCND .LT. 1 or MBDCND .GT. 6
C
C = 4 C .GE. D
C
C = 5 N .LE. 2
C
C = 6 NBDCND .LT. 0 or NBDCND .GT. 4
C
C = 7 A = 0 and MBDCND = 1,2,3, or 4
C
C = 8 A .GT. 0 and MBDCND .GE. 5
C
C = 9 M .LE. 2
C
C = 10 IDIMF .LT. M
C
C = 11 LAMBDA .GT. 0
C
C = 12 A=0, MBDCND .GE. 5, ELMBDA .NE. 0
C
C Since this is the only means of indicating a possibly
C incorrect call to HSTCYL, the user should test IERROR after
C the call.
C
C W
C W(1) contains the required length of W.
C
C *Long Description:
C
C * * * * * * * Program Specifications * * * * * * * * * * * *
C
C Dimension OF BDA(N),BDB(N),BDC(M),BDD(M),F(IDIMF,N),
C Arguments W(see argument list)
C
C Latest June 1, 1977
C Revision
C
C Subprograms HSTCYL,POISTG,POSTG2,GENBUN,POISD2,POISN2,POISP2,
C Required COSGEN,MERGE,TRIX,TRI3,PIMACH
C
C Special NONE
C Conditions
C
C Common NONE
C Blocks
C
C I/O NONE
C
C Precision Single
C
C Specialist Roland Sweet
C
C Language FORTRAN
C
C History Written by Roland Sweet at NCAR in March, 1977
C
C Algorithm This subroutine defines the finite-difference
C equations, incorporates boundary data, adjusts the
C right side when the system is singular and calls
C either POISTG or GENBUN which solves the linear
C system of equations.
C
C Space 8228(decimal) = 20044(octal) locations on the
C Required NCAR Control Data 7600
C
C Timing and The execution time T on the NCAR Control Data
C Accuracy 7600 for subroutine HSTCYL is roughly proportional
C to M*N*log2(N). Some typical values are listed in
C the table below.
C The solution process employed results in a loss
C of no more than four significant digits for N and M
C as large as 64. More detailed information about
C accuracy can be found in the documentation for
C subroutine POISTG which is the routine that
C actually solves the finite difference equations.
C
C
C M(=N) MBDCND NBDCND T(MSECS)
C ----- ------ ------ --------
C
C 32 1-6 1-4 56
C 64 1-6 1-4 230
C
C Portability American National Standards Institute Fortran.
C The machine dependent constant PI is defined in
C function PIMACH.
C
C Required COS
C Resident
C Routines
C
C Reference Schumann, U. and R. Sweet,'A Direct Method For
C The Solution of Poisson's Equation With Neumann
C Boundary Conditions On A Staggered Grid Of
C Arbitrary Size,' J. Comp. Phys. 20(1976),
C pp. 171-182.
C
C * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
C
C***REFERENCES U. Schumann and R. Sweet, A direct method for the
C solution of Poisson's equation with Neumann boundary
C conditions on a staggered grid of arbitrary size,
C Journal of Computational Physics 20, (1976),
C pp. 171-182.
C***ROUTINES CALLED GENBUN, POISTG
C***REVISION HISTORY (YYMMDD)
C 801001 DATE WRITTEN
C 890531 Changed all specific intrinsics to generic. (WRB)
C 890531 REVISION DATE from Version 3.2
C 891214 Prologue converted to Version 4.0 format. (BAB)
C 920501 Reformatted the REFERENCES section. (WRB)
C***END PROLOGUE HSTCYL