SLATEC Routines --- HWSCYL ---
*DECK HWSCYL
SUBROUTINE HWSCYL (A, B, M, MBDCND, BDA, BDB, C, D, N, NBDCND,
+ BDC, BDD, ELMBDA, F, IDIMF, PERTRB, IERROR, W)
C***BEGIN PROLOGUE HWSCYL
C***PURPOSE Solve a standard finite difference approximation
C to the Helmholtz equation in cylindrical coordinates.
C***LIBRARY SLATEC (FISHPACK)
C***CATEGORY I2B1A1A
C***TYPE SINGLE PRECISION (HWSCYL-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 Subroutine HWSCYL solves a finite difference approximation to the
C Helmholtz equation in cylindrical coordinates:
C
C (1/R)(d/dR)(R(dU/dR)) + (d/dZ)(dU/dZ)
C
C + (LAMBDA/R**2)U = F(R,Z)
C
C This modified Helmholtz equation results from the Fourier
C transform of the three-dimensional Poisson equation.
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
C and A must be non-negative.
C
C M
C The number of panels into which the interval (A,B) is
C subdivided. Hence, there will be M+1 grid points in the
C R-direction given by R(I) = A+(I-1)DR, for I = 1,2,...,M+1,
C where DR = (B-A)/M is the panel width. M must be greater than 3.
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 and R = B.
C = 2 If the solution is specified at R = A and the derivative of
C the solution with respect to R is specified at R = B.
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 = 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 = 5 If the solution is unspecified at R = A = 0 and the
C solution is specified at R = B.
C = 6 If the solution is unspecified at R = A = 0 and the
C derivative of the solution with respect to R is specified
C at R = B.
C
C NOTE: If A = 0, do not use MBDCND = 3 or 4, but instead use
C MBDCND = 1,2,5, or 6 .
C
C BDA
C A one-dimensional array of length N+1 that specifies the values
C of the derivative of the solution with respect to R at R = A.
C When MBDCND = 3 or 4,
C
C BDA(J) = (d/dR)U(A,Z(J)), J = 1,2,...,N+1 .
C
C When MBDCND has any other value, BDA is a dummy variable.
C
C BDB
C A one-dimensional array of length N+1 that specifies the values
C of the derivative of the solution with respect to R at R = B.
C When MBDCND = 2,3, or 6,
C
C BDB(J) = (d/dR)U(B,Z(J)), J = 1,2,...,N+1 .
C
C When MBDCND has any other value, BDB is a dummy variable.
C
C C,D
C The range of Z, i.e., C .LE. Z .LE. D. C must be less than D.
C
C N
C The number of panels into which the interval (C,D) is
C subdivided. Hence, there will be N+1 grid points in the
C Z-direction given by Z(J) = C+(J-1)DZ, for J = 1,2,...,N+1,
C where DZ = (D-C)/N is the panel width. N must be greater than 3.
C
C NBDCND
C Indicates the type of boundary conditions at Z = C and Z = D.
C
C = 0 If the solution is periodic in Z, i.e., U(I,1) = U(I,N+1).
C = 1 If the solution is specified at Z = C and Z = D.
C = 2 If the solution is specified at Z = C and the derivative of
C the solution with respect to Z is specified at Z = D.
C = 3 If the derivative of the solution with respect to Z is
C specified at Z = C and Z = D.
C = 4 If the derivative of the solution with respect to Z is
C specified at Z = C and the solution is specified at Z = D.
C
C BDC
C A one-dimensional array of length M+1 that specifies the values
C of the derivative of the solution with respect to Z at Z = C.
C When NBDCND = 3 or 4,
C
C BDC(I) = (d/dZ)U(R(I),C), I = 1,2,...,M+1 .
C
C When NBDCND has any other value, BDC is a dummy variable.
C
C BDD
C A one-dimensional array of length M+1 that specifies the values
C of the derivative of the solution with respect to Z at Z = D.
C When NBDCND = 2 or 3,
C
C BDD(I) = (d/dZ)U(R(I),D), I = 1,2,...,M+1 .
C
C When NBDCND has any other value, BDD is a dummy variable.
C
C ELMBDA
C The constant LAMBDA in the Helmholtz equation. If
C LAMBDA .GT. 0, a solution may not exist. However, HWSCYL will
C attempt to find a solution. LAMBDA must be zero when
C MBDCND = 5 or 6 .
C
C F
C A two-dimensional array that specifies the values of the right
C side of the Helmholtz equation and boundary data (if any). For
C I = 2,3,...,M and J = 2,3,...,N
C
C F(I,J) = F(R(I),Z(J)).
C
C On the boundaries F is defined by
C
C MBDCND F(1,J) F(M+1,J)
C ------ --------- ---------
C
C 1 U(A,Z(J)) U(B,Z(J))
C 2 U(A,Z(J)) F(B,Z(J))
C 3 F(A,Z(J)) F(B,Z(J)) J = 1,2,...,N+1
C 4 F(A,Z(J)) U(B,Z(J))
C 5 F(0,Z(J)) U(B,Z(J))
C 6 F(0,Z(J)) F(B,Z(J))
C
C NBDCND F(I,1) F(I,N+1)
C ------ --------- ---------
C
C 0 F(R(I),C) F(R(I),C)
C 1 U(R(I),C) U(R(I),D)
C 2 U(R(I),C) F(R(I),D) I = 1,2,...,M+1
C 3 F(R(I),C) F(R(I),D)
C 4 F(R(I),C) U(R(I),D)
C
C F must be dimensioned at least (M+1)*(N+1).
C
C NOTE
C
C If the table calls for both the solution U and the right side F
C at a corner then the solution must be specified.
C
C IDIMF
C The row (or first) dimension of the array F as it appears in the
C program calling HWSCYL. This parameter is used to specify the
C variable dimension of F. IDIMF must be at least M+1 .
C
C W
C A one-dimensional array that must be provided by the user for
C work space. W may require up to 4*(N+1) +
C (13 + INT(log2(N+1)))*(M+1) locations. The actual number of
C locations used is computed by HWSCYL and is returned in location
C 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)), I = 1,2,...,M+1,
C J = 1,2,...,N+1 .
C
C PERTRB
C If one specifies a combination of periodic, derivative, and
C unspecified boundary conditions for a Poisson equation
C (LAMBDA = 0), a solution may not exist. PERTRB is a constant,
C calculated and subtracted from F, which ensures that a solution
C exists. HWSCYL then computes this solution, which is a least
C squares solution to the original approximation. This solution
C plus any constant is also a solution. Hence, the solution is
C not unique. The value of PERTRB should be small compared to the
C right side F. Otherwise, a solution is obtained to an
C essentially different problem. This comparison should always
C be made to insure that a meaningful solution has been obtained.
C
C IERROR
C An error flag which indicates invalid input parameters. Except
C for numbers 0 and 11, a solution is not attempted.
C
C = 0 No error.
C = 1 A .LT. 0 .
C = 2 A .GE. B.
C = 3 MBDCND .LT. 1 or MBDCND .GT. 6 .
C = 4 C .GE. D.
C = 5 N .LE. 3
C = 6 NBDCND .LT. 0 or NBDCND .GT. 4 .
C = 7 A = 0, MBDCND = 3 or 4 .
C = 8 A .GT. 0, MBDCND .GE. 5 .
C = 9 A = 0, LAMBDA .NE. 0, MBDCND .GE. 5 .
C = 10 IDIMF .LT. M+1 .
C = 11 LAMBDA .GT. 0 .
C = 12 M .LE. 3
C
C Since this is the only means of indicating a possibly incorrect
C call to HWSCYL, the user should test IERROR after 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+1),BDB(N+1),BDC(M+1),BDD(M+1),F(IDIMF,N+1),
C Arguments W(see argument list)
C
C Latest June 1, 1976
C Revision
C
C Subprograms HWSCYL,GENBUN,POISD2,POISN2,POISP2,COSGEN,MERGE,
C Required 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 Standardized September 1, 1973
C Revised April 1, 1976
C
C Algorithm The routine defines the finite difference
C equations, incorporates boundary data, and adjusts
C the right side of singular systems and then calls
C GENBUN to solve the system.
C
C Space 5818(decimal) = 13272(octal) locations on the NCAR
C Required Control Data 7600
C
C Timing and The execution time T on the NCAR Control Data
C Accuracy 7600 for subroutine HWSCYL is roughly proportional
C to M*N*log2(N), but also depends on the input
C parameters NBDCND and MBDCND. Some typical values
C are listed in the table below.
C The solution process employed results in a loss
C of no more than three significant digits for N and
C M as large as 64. More detailed information about
C accuracy can be found in the documentation for
C subroutine GENBUN which is the routine that
C solves the finite difference equations.
C
C
C M(=N) MBDCND NBDCND T(MSECS)
C ----- ------ ------ --------
C
C 32 1 0 31
C 32 1 1 23
C 32 3 3 36
C 64 1 0 128
C 64 1 1 96
C 64 3 3 142
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 Swarztrauber, P. and R. Sweet, 'Efficient FORTRAN
C Subprograms for the Solution of Elliptic Equations'
C NCAR TN/IA-109, July, 1975, 138 pp.
C
C * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
C
C***REFERENCES P. N. Swarztrauber and R. Sweet, Efficient Fortran
C subprograms for the solution of elliptic equations,
C NCAR TN/IA-109, July 1975, 138 pp.
C***ROUTINES CALLED GENBUN
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 HWSCYL