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OpenLibm/slatec/hstcrt.f
Viral B. Shah c977aa998f Add Makefile.extras to build libopenlibm-extras. 
Replace amos with slatec
2012-12-31 16:37:05 -05:00

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*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
C
C
DIMENSION F(IDIMF,*) ,BDA(*) ,BDB(*) ,BDC(*) ,
1 BDD(*) ,W(*)
C***FIRST EXECUTABLE STATEMENT HSTCRT
IERROR = 0
IF (A .GE. B) IERROR = 1
IF (MBDCND.LT.0 .OR. MBDCND.GT.4) IERROR = 2
IF (C .GE. D) IERROR = 3
IF (N .LE. 2) IERROR = 4
IF (NBDCND.LT.0 .OR. NBDCND.GT.4) IERROR = 5
IF (IDIMF .LT. M) IERROR = 7
IF (M .LE. 2) IERROR = 8
IF (IERROR .NE. 0) RETURN
NPEROD = NBDCND
MPEROD = 0
IF (MBDCND .GT. 0) MPEROD = 1
DELTAX = (B-A)/M
TWDELX = 1./DELTAX
DELXSQ = 2./DELTAX**2
DELTAY = (D-C)/N
TWDELY = 1./DELTAY
DELYSQ = DELTAY**2
TWDYSQ = 2./DELYSQ
NP = NBDCND+1
MP = MBDCND+1
C
C DEFINE THE A,B,C COEFFICIENTS IN W-ARRAY.
C
ID2 = M
ID3 = ID2+M
ID4 = ID3+M
S = (DELTAY/DELTAX)**2
ST2 = 2.*S
DO 101 I=1,M
W(I) = S
J = ID2+I
W(J) = -ST2+ELMBDA*DELYSQ
J = ID3+I
W(J) = S
101 CONTINUE
C
C ENTER BOUNDARY DATA FOR X-BOUNDARIES.
C
GO TO (111,102,102,104,104),MP
102 DO 103 J=1,N
F(1,J) = F(1,J)-BDA(J)*DELXSQ
103 CONTINUE
W(ID2+1) = W(ID2+1)-W(1)
GO TO 106
104 DO 105 J=1,N
F(1,J) = F(1,J)+BDA(J)*TWDELX
105 CONTINUE
W(ID2+1) = W(ID2+1)+W(1)
106 GO TO (111,107,109,109,107),MP
107 DO 108 J=1,N
F(M,J) = F(M,J)-BDB(J)*DELXSQ
108 CONTINUE
W(ID3) = W(ID3)-W(1)
GO TO 111
109 DO 110 J=1,N
F(M,J) = F(M,J)-BDB(J)*TWDELX
110 CONTINUE
W(ID3) = W(ID3)+W(1)
111 CONTINUE
C
C ENTER BOUNDARY DATA FOR Y-BOUNDARIES.
C
GO TO (121,112,112,114,114),NP
112 DO 113 I=1,M
F(I,1) = F(I,1)-BDC(I)*TWDYSQ
113 CONTINUE
GO TO 116
114 DO 115 I=1,M
F(I,1) = F(I,1)+BDC(I)*TWDELY
115 CONTINUE
116 GO TO (121,117,119,119,117),NP
117 DO 118 I=1,M
F(I,N) = F(I,N)-BDD(I)*TWDYSQ
118 CONTINUE
GO TO 121
119 DO 120 I=1,M
F(I,N) = F(I,N)-BDD(I)*TWDELY
120 CONTINUE
121 CONTINUE
DO 123 I=1,M
DO 122 J=1,N
F(I,J) = F(I,J)*DELYSQ
122 CONTINUE
123 CONTINUE
IF (MPEROD .EQ. 0) GO TO 124
W(1) = 0.
W(ID4) = 0.
124 CONTINUE
PERTRB = 0.
IF (ELMBDA) 133,126,125
125 IERROR = 6
GO TO 133
126 GO TO (127,133,133,127,133),MP
127 GO TO (128,133,133,128,133),NP
C
C FOR SINGULAR PROBLEMS MUST ADJUST DATA TO INSURE THAT A SOLUTION
C WILL EXIST.
C
128 CONTINUE
S = 0.
DO 130 J=1,N
DO 129 I=1,M
S = S+F(I,J)
129 CONTINUE
130 CONTINUE
PERTRB = S/(M*N)
DO 132 J=1,N
DO 131 I=1,M
F(I,J) = F(I,J)-PERTRB
131 CONTINUE
132 CONTINUE
PERTRB = PERTRB/DELYSQ
C
C SOLVE THE EQUATION.
C
133 CONTINUE
IF (NPEROD .EQ. 0) GO TO 134
CALL POISTG (NPEROD,N,MPEROD,M,W(1),W(ID2+1),W(ID3+1),IDIMF,F,
1 IERR1,W(ID4+1))
GO TO 135
134 CONTINUE
CALL GENBUN (NPEROD,N,MPEROD,M,W(1),W(ID2+1),W(ID3+1),IDIMF,F,
1 IERR1,W(ID4+1))
135 CONTINUE
W(1) = W(ID4+1)+3*M
RETURN
END
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