*DECK HSTCRT SUBROUTINE HSTCRT (A, B, M, MBDCND, BDA, BDB, C, D, N, NBDCND, + BDC, BDD, ELMBDA, F, IDIMF, PERTRB, IERROR, W) C***BEGIN PROLOGUE HSTCRT C***PURPOSE Solve the standard five-point finite difference C approximation on a staggered grid to the Helmholtz equation C in Cartesian coordinates. C***LIBRARY SLATEC (FISHPACK) C***CATEGORY I2B1A1A C***TYPE SINGLE PRECISION (HSTCRT-S) C***KEYWORDS ELLIPTIC, FISHPACK, HELMHOLTZ, PDE C***AUTHOR Adams, J., (NCAR) C Swarztrauber, P. N., (NCAR) C Sweet, R., (NCAR) C***DESCRIPTION C C HSTCRT solves the standard five-point finite difference C approximation on a staggered grid to the Helmholtz equation in C Cartesian coordinates C C (d/dX)(dU/dX) + (d/dY)(dU/dY) + LAMBDA*U = F(X,Y) C C * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * C C * * * * * * * * Parameter Description * * * * * * * * * * C C * * * * * * On Input * * * * * * C C A,B C The range of X, i.e. A .LE. X .LE. B. A must be less than B. C C M C The number of grid points in the interval (A,B). The grid points C in the X-direction are given by X(I) = A + (I-0.5)dX for C I=1,2,...,M where dX =(B-A)/M. M must be greater than 2. C C MBDCND C Indicates the type of boundary conditions at X = A and X = B. C C = 0 If the solution is periodic in X, C U(M+I,J) = U(I,J). C C = 1 If the solution is specified at X = A and X = B. C C = 2 If the solution is specified at X = A and the derivative C of the solution with respect to X is specified at X = B. C C = 3 If the derivative of the solution with respect to X is C specified at X = A and X = B. C C = 4 If the derivative of the solution with respect to X is C specified at X = A and the solution is specified at X = B. C C BDA C A one-dimensional array of length N that specifies the boundary C values (if any) of the solution at X = A. When MBDCND = 1 or 2, C C BDA(J) = U(A,Y(J)) , J=1,2,...,N. C C When MBDCND = 3 or 4, C C BDA(J) = (d/dX)U(A,Y(J)) , J=1,2,...,N. C C BDB C A one-dimensional array of length N that specifies the boundary C values of the solution at X = B. When MBDCND = 1 or 4 C C BDB(J) = U(B,Y(J)) , J=1,2,...,N. C C When MBDCND = 2 or 3 C C BDB(J) = (d/dX)U(B,Y(J)) , J=1,2,...,N. C C C,D C The range of Y, i.e. C .LE. Y .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 Y-direction are given by Y(J) = C + (J-0.5)DY, C J=1,2,...,N, where DY = (D-C)/N. N must be greater than 2. C C NBDCND C Indicates the type of boundary conditions at Y = C C and Y = D. C C = 0 If the solution is periodic in Y, i.e. C U(I,J) = U(I,N+J). C C = 1 If the solution is specified at Y = C and Y = D. C C = 2 If the solution is specified at Y = C and the derivative C of the solution with respect to Y is specified at Y = D. C C = 3 If the derivative of the solution with respect to Y is C specified at Y = C and Y = D. C C = 4 If the derivative of the solution with respect to Y is C specified at Y = C and the solution is specified at Y = D. C C BDC C A one dimensional array of length M that specifies the boundary C values of the solution at Y = C. When NBDCND = 1 or 2, C C BDC(I) = U(X(I),C) , I=1,2,...,M. C C When NBDCND = 3 or 4, C C BDC(I) = (d/dY)U(X(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 Y = D. When NBDCND = 1 or 4, C C BDD(I) = U(X(I),D) , I=1,2,...,M. C C When NBDCND = 2 or 3, C C BDD(I) = (d/dY)U(X(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 Helmholtz equation. If LAMBDA is C greater than 0, a solution may not exist. However, HSTCRT will C attempt to find a solution. C C F C A two-dimensional array that specifies the values of the right C side of the Helmholtz equation. For I=1,2,...,M and J=1,2,...,N C C F(I,J) = F(X(I),Y(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 HSTCRT. 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 HSTCRT 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 (X(I),Y(J)) for C I=1,2,...,M, J=1,2,...,N. C C PERTRB C If a combination of periodic or derivative boundary conditions is C specified for a Poisson equation (LAMBDA = 0), a solution may not C exist. PERTRB is a constant, calculated and subtracted from F, C which ensures that a solution exists. HSTCRT then computes this C solution, which is a least squares solution to the original C approximation. This solution plus any constant is also a C solution; hence, the solution is not unique. The value of PERTRB C should be small compared to the right side F. Otherwise, a C solution is obtained to an essentially different problem. This C comparison should always be made to insure that a meaningful C solution has been obtained. C C IERROR C An error flag that indicates invalid input parameters. C Except for numbers 0 and 6, a solution is not attempted. C C = 0 No error C C = 1 A .GE. B C C = 2 MBDCND .LT. 0 or MBDCND .GT. 4 C C = 3 C .GE. D C C = 4 N .LE. 2 C C = 5 NBDCND .LT. 0 or NBDCND .GT. 4 C C = 6 LAMBDA .GT. 0 C C = 7 IDIMF .LT. M C C = 8 M .LE. 2 C C Since this is the only means of indicating a possibly C incorrect call to HSTCRT, 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 HSTCRT,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 January , 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 8131(decimal) = 17703(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 HSTCRT 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 1-4 1-4 56 C 64 1-4 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 HSTCRT