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688 lines
32 KiB
Fortran
688 lines
32 KiB
Fortran
*DECK DDEABM
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SUBROUTINE DDEABM (DF, NEQ, T, Y, TOUT, INFO, RTOL, ATOL, IDID,
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+ RWORK, LRW, IWORK, LIW, RPAR, IPAR)
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C***BEGIN PROLOGUE DDEABM
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C***PURPOSE Solve an initial value problem in ordinary differential
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C equations using an Adams-Bashforth method.
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C***LIBRARY SLATEC (DEPAC)
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C***CATEGORY I1A1B
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C***TYPE DOUBLE PRECISION (DEABM-S, DDEABM-D)
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C***KEYWORDS ADAMS-BASHFORTH METHOD, DEPAC, INITIAL VALUE PROBLEMS,
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C ODE, ORDINARY DIFFERENTIAL EQUATIONS, PREDICTOR-CORRECTOR
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C***AUTHOR Shampine, L. F., (SNLA)
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C Watts, H. A., (SNLA)
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C***DESCRIPTION
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C
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C This is the Adams code in the package of differential equation
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C solvers DEPAC, consisting of the codes DDERKF, DDEABM, and DDEBDF.
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C Design of the package was by L. F. Shampine and H. A. Watts.
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C It is documented in
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C SAND79-2374 , DEPAC - Design of a User Oriented Package of ODE
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C Solvers.
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C DDEABM is a driver for a modification of the code ODE written by
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C L. F. Shampine and M. K. Gordon
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C Sandia Laboratories
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C Albuquerque, New Mexico 87185
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C
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C **********************************************************************
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C * ABSTRACT *
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C ************
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C
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C Subroutine DDEABM uses the Adams-Bashforth-Moulton
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C Predictor-Corrector formulas of orders one through twelve to
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C integrate a system of NEQ first order ordinary differential
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C equations of the form
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C DU/DX = DF(X,U)
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C when the vector Y(*) of initial values for U(*) at X=T is given.
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C The subroutine integrates from T to TOUT. It is easy to continue the
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C integration to get results at additional TOUT. This is the interval
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C mode of operation. It is also easy for the routine to return with
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C the solution at each intermediate step on the way to TOUT. This is
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C the intermediate-output mode of operation.
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C
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C DDEABM uses subprograms DDES, DSTEPS, DINTP, DHSTRT, DHVNRM,
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C D1MACH, and the error handling routine XERMSG. The only machine
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C dependent parameters to be assigned appear in D1MACH.
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C
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C **********************************************************************
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C * Description of The Arguments To DDEABM (An Overview) *
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C **********************************************************************
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C
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C The Parameters are
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C
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C DF -- This is the name of a subroutine which you provide to
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C define the differential equations.
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C
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C NEQ -- This is the number of (first order) differential
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C equations to be integrated.
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C
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C T -- This is a DOUBLE PRECISION value of the independent
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C variable.
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C
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C Y(*) -- This DOUBLE PRECISION array contains the solution
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C components at T.
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C
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C TOUT -- This is a DOUBLE PRECISION point at which a solution is
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C desired.
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C
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C INFO(*) -- The basic task of the code is to integrate the
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C differential equations from T to TOUT and return an
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C answer at TOUT. INFO(*) is an INTEGER array which is used
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C to communicate exactly how you want this task to be
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C carried out.
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C
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C RTOL, ATOL -- These DOUBLE PRECISION quantities represent
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C relative and absolute error tolerances which you
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C provide to indicate how accurately you wish the
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C solution to be computed. You may choose them to be
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C both scalars or else both vectors.
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C
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C IDID -- This scalar quantity is an indicator reporting what
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C the code did. You must monitor this INTEGER variable to
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C decide what action to take next.
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C
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C RWORK(*), LRW -- RWORK(*) is a DOUBLE PRECISION work array of
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C length LRW which provides the code with needed storage
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C space.
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C
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C IWORK(*), LIW -- IWORK(*) is an INTEGER work array of length LIW
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C which provides the code with needed storage space and an
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C across call flag.
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C
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C RPAR, IPAR -- These are DOUBLE PRECISION and INTEGER parameter
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C arrays which you can use for communication between your
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C calling program and the DF subroutine.
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C
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C Quantities which are used as input items are
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C NEQ, T, Y(*), TOUT, INFO(*),
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C RTOL, ATOL, RWORK(1), LRW and LIW.
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C
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C Quantities which may be altered by the code are
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C T, Y(*), INFO(1), RTOL, ATOL,
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C IDID, RWORK(*) and IWORK(*).
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C
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C **********************************************************************
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C * INPUT -- What To Do On The First Call To DDEABM *
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C **********************************************************************
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C
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C The first call of the code is defined to be the start of each new
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C problem. Read through the descriptions of all the following items,
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C provide sufficient storage space for designated arrays, set
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C appropriate variables for the initialization of the problem, and
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C give information about how you want the problem to be solved.
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C
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C
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C DF -- Provide a subroutine of the form
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C DF(X,U,UPRIME,RPAR,IPAR)
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C to define the system of first order differential equations
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C which is to be solved. For the given values of X and the
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C vector U(*)=(U(1),U(2),...,U(NEQ)) , the subroutine must
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C evaluate the NEQ components of the system of differential
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C equations DU/DX=DF(X,U) and store the derivatives in the
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C array UPRIME(*), that is, UPRIME(I) = * DU(I)/DX * for
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C equations I=1,...,NEQ.
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C
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C Subroutine DF must NOT alter X or U(*). You must declare
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C the name df in an external statement in your program that
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C calls DDEABM. You must dimension U and UPRIME in DF.
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C
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C RPAR and IPAR are DOUBLE PRECISION and INTEGER parameter
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C arrays which you can use for communication between your
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C calling program and subroutine DF. They are not used or
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C altered by DDEABM. If you do not need RPAR or IPAR,
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C ignore these parameters by treating them as dummy
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C arguments. If you do choose to use them, dimension them in
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C your calling program and in DF as arrays of appropriate
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C length.
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C
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C NEQ -- Set it to the number of differential equations.
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C (NEQ .GE. 1)
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C
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C T -- Set it to the initial point of the integration.
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C You must use a program variable for T because the code
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C changes its value.
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C
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C Y(*) -- Set this vector to the initial values of the NEQ solution
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C components at the initial point. You must dimension Y at
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C least NEQ in your calling program.
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C
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C TOUT -- Set it to the first point at which a solution
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C is desired. You can take TOUT = T, in which case the code
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C will evaluate the derivative of the solution at T and
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C return. Integration either forward in T (TOUT .GT. T) or
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C backward in T (TOUT .LT. T) is permitted.
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C
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C The code advances the solution from T to TOUT using
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C step sizes which are automatically selected so as to
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C achieve the desired accuracy. If you wish, the code will
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C return with the solution and its derivative following
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C each intermediate step (intermediate-output mode) so that
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C you can monitor them, but you still must provide TOUT in
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C accord with the basic aim of the code.
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C
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C The first step taken by the code is a critical one
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C because it must reflect how fast the solution changes near
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C the initial point. The code automatically selects an
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C initial step size which is practically always suitable for
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C the problem. By using the fact that the code will not step
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C past TOUT in the first step, you could, if necessary,
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C restrict the length of the initial step size.
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C
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C For some problems it may not be permissible to integrate
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C past a point TSTOP because a discontinuity occurs there
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C or the solution or its derivative is not defined beyond
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C TSTOP. When you have declared a TSTOP point (see INFO(4)
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C and RWORK(1)), you have told the code not to integrate
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C past TSTOP. In this case any TOUT beyond TSTOP is invalid
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C input.
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C
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C INFO(*) -- Use the INFO array to give the code more details about
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C how you want your problem solved. This array should be
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C dimensioned of length 15 to accommodate other members of
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C DEPAC or possible future extensions, though DDEABM uses
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C only the first four entries. You must respond to all of
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C the following items which are arranged as questions. The
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C simplest use of the code corresponds to answering all
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C questions as YES ,i.e. setting ALL entries of INFO to 0.
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C
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C INFO(1) -- This parameter enables the code to initialize
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C itself. You must set it to indicate the start of every
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C new problem.
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C
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C **** Is this the first call for this problem ...
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C YES -- set INFO(1) = 0
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C NO -- not applicable here.
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C See below for continuation calls. ****
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C
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C INFO(2) -- How much accuracy you want of your solution
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C is specified by the error tolerances RTOL and ATOL.
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C The simplest use is to take them both to be scalars.
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C To obtain more flexibility, they can both be vectors.
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C The code must be told your choice.
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C
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C **** Are both error tolerances RTOL, ATOL scalars ...
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C YES -- set INFO(2) = 0
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C and input scalars for both RTOL and ATOL
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C NO -- set INFO(2) = 1
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C and input arrays for both RTOL and ATOL ****
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C
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C INFO(3) -- The code integrates from T in the direction
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C of TOUT by steps. If you wish, it will return the
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C computed solution and derivative at the next
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C intermediate step (the intermediate-output mode) or
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C TOUT, whichever comes first. This is a good way to
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C proceed if you want to see the behavior of the solution.
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C If you must have solutions at a great many specific
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C TOUT points, this code will compute them efficiently.
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C
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C **** Do you want the solution only at
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C TOUT (and not at the next intermediate step) ...
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C YES -- set INFO(3) = 0
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C NO -- set INFO(3) = 1 ****
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C
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C INFO(4) -- To handle solutions at a great many specific
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C values TOUT efficiently, this code may integrate past
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C TOUT and interpolate to obtain the result at TOUT.
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C Sometimes it is not possible to integrate beyond some
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C point TSTOP because the equation changes there or it is
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C not defined past TSTOP. Then you must tell the code
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C not to go past.
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C
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C **** Can the integration be carried out without any
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C Restrictions on the independent variable T ...
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C YES -- set INFO(4)=0
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C NO -- set INFO(4)=1
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C and define the stopping point TSTOP by
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C setting RWORK(1)=TSTOP ****
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C
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C RTOL, ATOL -- You must assign relative (RTOL) and absolute (ATOL)
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C error tolerances to tell the code how accurately you want
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C the solution to be computed. They must be defined as
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C program variables because the code may change them. You
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C have two choices --
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C Both RTOL and ATOL are scalars. (INFO(2)=0)
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C Both RTOL and ATOL are vectors. (INFO(2)=1)
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C In either case all components must be non-negative.
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C
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C The tolerances are used by the code in a local error test
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C at each step which requires roughly that
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C ABS(LOCAL ERROR) .LE. RTOL*ABS(Y)+ATOL
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C for each vector component.
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C (More specifically, a Euclidean norm is used to measure
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C the size of vectors, and the error test uses the magnitude
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C of the solution at the beginning of the step.)
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C
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C The true (global) error is the difference between the true
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C solution of the initial value problem and the computed
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C approximation. Practically all present day codes,
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C including this one, control the local error at each step
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C and do not even attempt to control the global error
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C directly. Roughly speaking, they produce a solution Y(T)
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C which satisfies the differential equations with a
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C residual R(T), DY(T)/DT = DF(T,Y(T)) + R(T) ,
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C and, almost always, R(T) is bounded by the error
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C tolerances. Usually, but not always, the true accuracy of
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C the computed Y is comparable to the error tolerances. This
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C code will usually, but not always, deliver a more accurate
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C solution if you reduce the tolerances and integrate again.
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C By comparing two such solutions you can get a fairly
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C reliable idea of the true error in the solution at the
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C bigger tolerances.
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C
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C Setting ATOL=0.D0 results in a pure relative error test on
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C that component. Setting RTOL=0. results in a pure absolute
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C error test on that component. A mixed test with non-zero
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C RTOL and ATOL corresponds roughly to a relative error
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C test when the solution component is much bigger than ATOL
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C and to an absolute error test when the solution component
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C is smaller than the threshold ATOL.
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C
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C Proper selection of the absolute error control parameters
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C ATOL requires you to have some idea of the scale of the
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C solution components. To acquire this information may mean
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C that you will have to solve the problem more than once. In
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C the absence of scale information, you should ask for some
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C relative accuracy in all the components (by setting RTOL
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C values non-zero) and perhaps impose extremely small
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C absolute error tolerances to protect against the danger of
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C a solution component becoming zero.
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C
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C The code will not attempt to compute a solution at an
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C accuracy unreasonable for the machine being used. It will
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C advise you if you ask for too much accuracy and inform
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C you as to the maximum accuracy it believes possible.
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C
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C RWORK(*) -- Dimension this DOUBLE PRECISION work array of length
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C LRW in your calling program.
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C
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C RWORK(1) -- If you have set INFO(4)=0, you can ignore this
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C optional input parameter. Otherwise you must define a
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C stopping point TSTOP by setting RWORK(1) = TSTOP.
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C (for some problems it may not be permissible to integrate
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C past a point TSTOP because a discontinuity occurs there
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C or the solution or its derivative is not defined beyond
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C TSTOP.)
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C
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C LRW -- Set it to the declared length of the RWORK array.
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C You must have LRW .GE. 130+21*NEQ
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C
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C IWORK(*) -- Dimension this INTEGER work array of length LIW in
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C your calling program.
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C
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C LIW -- Set it to the declared length of the IWORK array.
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C You must have LIW .GE. 51
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C
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C RPAR, IPAR -- These are parameter arrays, of DOUBLE PRECISION and
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C INTEGER type, respectively. You can use them for
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C communication between your program that calls DDEABM and
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C the DF subroutine. They are not used or altered by
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C DDEABM. If you do not need RPAR or IPAR, ignore these
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C parameters by treating them as dummy arguments. If you do
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C choose to use them, dimension them in your calling program
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C and in DF as arrays of appropriate length.
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C
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C **********************************************************************
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C * OUTPUT -- After Any Return From DDEABM *
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C **********************************************************************
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C
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C The principal aim of the code is to return a computed solution at
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C TOUT, although it is also possible to obtain intermediate results
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C along the way. To find out whether the code achieved its goal
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C or if the integration process was interrupted before the task was
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C completed, you must check the IDID parameter.
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C
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C
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C T -- The solution was successfully advanced to the
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C output value of T.
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C
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C Y(*) -- Contains the computed solution approximation at T.
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C You may also be interested in the approximate derivative
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C of the solution at T. It is contained in
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C RWORK(21),...,RWORK(20+NEQ).
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C
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C IDID -- Reports what the code did
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C
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C *** Task Completed ***
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C Reported by positive values of IDID
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C
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C IDID = 1 -- A step was successfully taken in the
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C intermediate-output mode. The code has not
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C yet reached TOUT.
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C
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C IDID = 2 -- The integration to TOUT was successfully
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C completed (T=TOUT) by stepping exactly to TOUT.
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C
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C IDID = 3 -- The integration to TOUT was successfully
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C completed (T=TOUT) by stepping past TOUT.
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C Y(*) is obtained by interpolation.
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C
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C *** Task Interrupted ***
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C Reported by negative values of IDID
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C
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C IDID = -1 -- A large amount of work has been expended.
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C (500 steps attempted)
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C
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C IDID = -2 -- The error tolerances are too stringent.
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C
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C IDID = -3 -- The local error test cannot be satisfied
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C because you specified a zero component in ATOL
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C and the corresponding computed solution
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C component is zero. Thus, a pure relative error
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C test is impossible for this component.
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C
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C IDID = -4 -- The problem appears to be stiff.
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C
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C IDID = -5,-6,-7,..,-32 -- Not applicable for this code
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C but used by other members of DEPAC or possible
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C future extensions.
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C
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C *** Task Terminated ***
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C Reported by the value of IDID=-33
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C
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C IDID = -33 -- The code has encountered trouble from which
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C it cannot recover. A message is printed
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C explaining the trouble and control is returned
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C to the calling program. For example, this occurs
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C when invalid input is detected.
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C
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C RTOL, ATOL -- These quantities remain unchanged except when
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C IDID = -2. In this case, the error tolerances have been
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C increased by the code to values which are estimated to be
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C appropriate for continuing the integration. However, the
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C reported solution at T was obtained using the input values
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C of RTOL and ATOL.
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C
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C RWORK, IWORK -- Contain information which is usually of no
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C interest to the user but necessary for subsequent calls.
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C However, you may find use for
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C
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C RWORK(11)--which contains the step size H to be
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C attempted on the next step.
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C
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C RWORK(12)--if the tolerances have been increased by the
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C code (IDID = -2) , they were multiplied by the
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C value in RWORK(12).
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C
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C RWORK(13)--Which contains the current value of the
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C independent variable, i.e. the farthest point
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C integration has reached. This will be different
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C from T only when interpolation has been
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C performed (IDID=3).
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C
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C RWORK(20+I)--Which contains the approximate derivative
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C of the solution component Y(I). In DDEABM, it
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C is obtained by calling subroutine DF to
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C evaluate the differential equation using T and
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C Y(*) when IDID=1 or 2, and by interpolation
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C when IDID=3.
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C
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C **********************************************************************
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C * INPUT -- What To Do To Continue The Integration *
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C * (calls after the first) *
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C **********************************************************************
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C
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C This code is organized so that subsequent calls to continue the
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C integration involve little (if any) additional effort on your
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C part. You must monitor the IDID parameter in order to determine
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C what to do next.
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C
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C Recalling that the principal task of the code is to integrate
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C from T to TOUT (the interval mode), usually all you will need
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C to do is specify a new TOUT upon reaching the current TOUT.
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C
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C Do not alter any quantity not specifically permitted below,
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C in particular do not alter NEQ, T, Y(*), RWORK(*), IWORK(*) or
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C the differential equation in subroutine DF. Any such alteration
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C constitutes a new problem and must be treated as such, i.e.
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C you must start afresh.
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C
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C You cannot change from vector to scalar error control or vice
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C versa (INFO(2)) but you can change the size of the entries of
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C RTOL, ATOL. Increasing a tolerance makes the equation easier
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C to integrate. Decreasing a tolerance will make the equation
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C harder to integrate and should generally be avoided.
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C
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C You can switch from the intermediate-output mode to the
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C interval mode (INFO(3)) or vice versa at any time.
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C
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C If it has been necessary to prevent the integration from going
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C past a point TSTOP (INFO(4), RWORK(1)), keep in mind that the
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C code will not integrate to any TOUT beyond the currently
|
|
C specified TSTOP. Once TSTOP has been reached you must change
|
|
C the value of TSTOP or set INFO(4)=0. You may change INFO(4)
|
|
C or TSTOP at any time but you must supply the value of TSTOP in
|
|
C RWORK(1) whenever you set INFO(4)=1.
|
|
C
|
|
C The parameter INFO(1) is used by the code to indicate the
|
|
C beginning of a new problem and to indicate whether integration
|
|
C is to be continued. You must input the value INFO(1) = 0
|
|
C when starting a new problem. You must input the value
|
|
C INFO(1) = 1 if you wish to continue after an interrupted task.
|
|
C Do not set INFO(1) = 0 on a continuation call unless you
|
|
C want the code to restart at the current T.
|
|
C
|
|
C *** Following A Completed Task ***
|
|
C If
|
|
C IDID = 1, call the code again to continue the integration
|
|
C another step in the direction of TOUT.
|
|
C
|
|
C IDID = 2 or 3, define a new TOUT and call the code again.
|
|
C TOUT must be different from T. You cannot change
|
|
C the direction of integration without restarting.
|
|
C
|
|
C *** Following An Interrupted Task ***
|
|
C To show the code that you realize the task was
|
|
C interrupted and that you want to continue, you
|
|
C must take appropriate action and reset INFO(1) = 1
|
|
C If
|
|
C IDID = -1, the code has attempted 500 steps.
|
|
C If you want to continue, set INFO(1) = 1 and
|
|
C call the code again. An additional 500 steps
|
|
C will be allowed.
|
|
C
|
|
C IDID = -2, the error tolerances RTOL, ATOL have been
|
|
C increased to values the code estimates appropriate
|
|
C for continuing. You may want to change them
|
|
C yourself. If you are sure you want to continue
|
|
C with relaxed error tolerances, set INFO(1)=1 and
|
|
C call the code again.
|
|
C
|
|
C IDID = -3, a solution component is zero and you set the
|
|
C corresponding component of ATOL to zero. If you
|
|
C are sure you want to continue, you must first
|
|
C alter the error criterion to use positive values
|
|
C for those components of ATOL corresponding to zero
|
|
C solution components, then set INFO(1)=1 and call
|
|
C the code again.
|
|
C
|
|
C IDID = -4, the problem appears to be stiff. It is very
|
|
C inefficient to solve such problems with DDEABM.
|
|
C The code DDEBDF in DEPAC handles this task
|
|
C efficiently. If you are absolutely sure you want
|
|
C to continue with DDEABM, set INFO(1)=1 and call
|
|
C the code again.
|
|
C
|
|
C IDID = -5,-6,-7,..,-32 --- cannot occur with this code
|
|
C but used by other members of DEPAC or possible
|
|
C future extensions.
|
|
C
|
|
C *** Following A Terminated Task ***
|
|
C If
|
|
C IDID = -33, you cannot continue the solution of this
|
|
C problem. An attempt to do so will result in your
|
|
C run being terminated.
|
|
C
|
|
C **********************************************************************
|
|
C *Long Description:
|
|
C
|
|
C **********************************************************************
|
|
C * DEPAC Package Overview *
|
|
C **********************************************************************
|
|
C
|
|
C .... You have a choice of three differential equation solvers from
|
|
C .... DEPAC. The following brief descriptions are meant to aid you in
|
|
C .... choosing the most appropriate code for your problem.
|
|
C
|
|
C .... DDERKF is a fifth order Runge-Kutta code. It is the simplest of
|
|
C .... the three choices, both algorithmically and in the use of the
|
|
C .... code. DDERKF is primarily designed to solve non-stiff and
|
|
C .... mildly stiff differential equations when derivative evaluations
|
|
C .... are not expensive. It should generally not be used to get high
|
|
C .... accuracy results nor answers at a great many specific points.
|
|
C .... Because DDERKF has very low overhead costs, it will usually
|
|
C .... result in the least expensive integration when solving
|
|
C .... problems requiring a modest amount of accuracy and having
|
|
C .... equations that are not costly to evaluate. DDERKF attempts to
|
|
C .... discover when it is not suitable for the task posed.
|
|
C
|
|
C .... DDEABM is a variable order (one through twelve) Adams code.
|
|
C .... Its complexity lies somewhere between that of DDERKF and
|
|
C .... DDEBDF. DDEABM is primarily designed to solve non-stiff and
|
|
C .... mildly stiff differential equations when derivative evaluations
|
|
C .... are expensive, high accuracy results are needed or answers at
|
|
C .... many specific points are required. DDEABM attempts to discover
|
|
C .... when it is not suitable for the task posed.
|
|
C
|
|
C .... DDEBDF is a variable order (one through five) backward
|
|
C .... differentiation formula code. it is the most complicated of
|
|
C .... the three choices. DDEBDF is primarily designed to solve stiff
|
|
C .... differential equations at crude to moderate tolerances.
|
|
C .... If the problem is very stiff at all, DDERKF and DDEABM will be
|
|
C .... quite inefficient compared to DDEBDF. However, DDEBDF will be
|
|
C .... inefficient compared to DDERKF and DDEABM on non-stiff problems
|
|
C .... because it uses much more storage, has a much larger overhead,
|
|
C .... and the low order formulas will not give high accuracies
|
|
C .... efficiently.
|
|
C
|
|
C .... The concept of stiffness cannot be described in a few words.
|
|
C .... If you do not know the problem to be stiff, try either DDERKF
|
|
C .... or DDEABM. Both of these codes will inform you of stiffness
|
|
C .... when the cost of solving such problems becomes important.
|
|
C
|
|
C *********************************************************************
|
|
C
|
|
C***REFERENCES L. F. Shampine and H. A. Watts, DEPAC - design of a user
|
|
C oriented package of ODE solvers, Report SAND79-2374,
|
|
C Sandia Laboratories, 1979.
|
|
C***ROUTINES CALLED DDES, XERMSG
|
|
C***REVISION HISTORY (YYMMDD)
|
|
C 820301 DATE WRITTEN
|
|
C 890531 Changed all specific intrinsics to generic. (WRB)
|
|
C 890831 Modified array declarations. (WRB)
|
|
C 891006 Cosmetic changes to prologue. (WRB)
|
|
C 891024 Changed references from DVNORM to DHVNRM. (WRB)
|
|
C 891024 REVISION DATE from Version 3.2
|
|
C 891214 Prologue converted to Version 4.0 format. (BAB)
|
|
C 900510 Convert XERRWV calls to XERMSG calls. (RWC)
|
|
C 920501 Reformatted the REFERENCES section. (WRB)
|
|
C***END PROLOGUE DDEABM
|
|
C
|
|
INTEGER IALPHA, IBETA, IDELSN, IDID, IFOURU, IG, IHOLD,
|
|
1 INFO, IP, IPAR, IPHI, IPSI, ISIG, ITOLD, ITSTAR, ITWOU,
|
|
2 IV, IW, IWORK, IWT, IYP, IYPOUT, IYY, LIW, LRW, NEQ
|
|
DOUBLE PRECISION ATOL, RPAR, RTOL, RWORK, T, TOUT, Y
|
|
LOGICAL START,PHASE1,NORND,STIFF,INTOUT
|
|
C
|
|
DIMENSION Y(*),INFO(15),RTOL(*),ATOL(*),RWORK(*),IWORK(*),
|
|
1 RPAR(*),IPAR(*)
|
|
C
|
|
CHARACTER*8 XERN1
|
|
CHARACTER*16 XERN3
|
|
C
|
|
EXTERNAL DF
|
|
C
|
|
C CHECK FOR AN APPARENT INFINITE LOOP
|
|
C
|
|
C***FIRST EXECUTABLE STATEMENT DDEABM
|
|
IF ( INFO(1) .EQ. 0 ) IWORK(LIW) = 0
|
|
IF (IWORK(LIW) .GE. 5) THEN
|
|
IF (T .EQ. RWORK(21 + NEQ)) THEN
|
|
WRITE (XERN3, '(1PE15.6)') T
|
|
CALL XERMSG ('SLATEC', 'DDEABM',
|
|
* 'AN APPARENT INFINITE LOOP HAS BEEN DETECTED.$$' //
|
|
* 'YOU HAVE MADE REPEATED CALLS AT T = ' // XERN3 //
|
|
* ' AND THE INTEGRATION HAS NOT ADVANCED. CHECK THE ' //
|
|
* 'WAY YOU HAVE SET PARAMETERS FOR THE CALL TO THE ' //
|
|
* 'CODE, PARTICULARLY INFO(1).', 13, 2)
|
|
RETURN
|
|
ENDIF
|
|
ENDIF
|
|
C
|
|
C CHECK LRW AND LIW FOR SUFFICIENT STORAGE ALLOCATION
|
|
C
|
|
IDID=0
|
|
IF (LRW .LT. 130+21*NEQ) THEN
|
|
WRITE (XERN1, '(I8)') LRW
|
|
CALL XERMSG ('SLATEC', 'DDEABM', 'THE LENGTH OF THE RWORK ' //
|
|
* 'ARRAY MUST BE AT LEAST 130 + 21*NEQ.$$' //
|
|
* 'YOU HAVE CALLED THE CODE WITH LRW = ' // XERN1, 1, 1)
|
|
IDID=-33
|
|
ENDIF
|
|
C
|
|
IF (LIW .LT. 51) THEN
|
|
WRITE (XERN1, '(I8)') LIW
|
|
CALL XERMSG ('SLATEC', 'DDEABM', 'THE LENGTH OF THE IWORK ' //
|
|
* 'ARRAY MUST BE AT LEAST 51.$$YOU HAVE CALLED THE CODE ' //
|
|
* 'WITH LIW = ' // XERN1, 2, 1)
|
|
IDID=-33
|
|
ENDIF
|
|
C
|
|
C COMPUTE THE INDICES FOR THE ARRAYS TO BE STORED IN THE WORK ARRAY
|
|
C
|
|
IYPOUT = 21
|
|
ITSTAR = NEQ + 21
|
|
IYP = 1 + ITSTAR
|
|
IYY = NEQ + IYP
|
|
IWT = NEQ + IYY
|
|
IP = NEQ + IWT
|
|
IPHI = NEQ + IP
|
|
IALPHA = (NEQ*16) + IPHI
|
|
IBETA = 12 + IALPHA
|
|
IPSI = 12 + IBETA
|
|
IV = 12 + IPSI
|
|
IW = 12 + IV
|
|
ISIG = 12 + IW
|
|
IG = 13 + ISIG
|
|
IGI = 13 + IG
|
|
IXOLD = 11 + IGI
|
|
IHOLD = 1 + IXOLD
|
|
ITOLD = 1 + IHOLD
|
|
IDELSN = 1 + ITOLD
|
|
ITWOU = 1 + IDELSN
|
|
IFOURU = 1 + ITWOU
|
|
C
|
|
RWORK(ITSTAR) = T
|
|
IF (INFO(1) .EQ. 0) GO TO 50
|
|
START = IWORK(21) .NE. (-1)
|
|
PHASE1 = IWORK(22) .NE. (-1)
|
|
NORND = IWORK(23) .NE. (-1)
|
|
STIFF = IWORK(24) .NE. (-1)
|
|
INTOUT = IWORK(25) .NE. (-1)
|
|
C
|
|
50 CALL DDES(DF,NEQ,T,Y,TOUT,INFO,RTOL,ATOL,IDID,RWORK(IYPOUT),
|
|
1 RWORK(IYP),RWORK(IYY),RWORK(IWT),RWORK(IP),RWORK(IPHI),
|
|
2 RWORK(IALPHA),RWORK(IBETA),RWORK(IPSI),RWORK(IV),
|
|
3 RWORK(IW),RWORK(ISIG),RWORK(IG),RWORK(IGI),RWORK(11),
|
|
4 RWORK(12),RWORK(13),RWORK(IXOLD),RWORK(IHOLD),
|
|
5 RWORK(ITOLD),RWORK(IDELSN),RWORK(1),RWORK(ITWOU),
|
|
5 RWORK(IFOURU),START,PHASE1,NORND,STIFF,INTOUT,IWORK(26),
|
|
6 IWORK(27),IWORK(28),IWORK(29),IWORK(30),IWORK(31),
|
|
7 IWORK(32),IWORK(33),IWORK(34),IWORK(35),IWORK(45),
|
|
8 RPAR,IPAR)
|
|
C
|
|
IWORK(21) = -1
|
|
IF (START) IWORK(21) = 1
|
|
IWORK(22) = -1
|
|
IF (PHASE1) IWORK(22) = 1
|
|
IWORK(23) = -1
|
|
IF (NORND) IWORK(23) = 1
|
|
IWORK(24) = -1
|
|
IF (STIFF) IWORK(24) = 1
|
|
IWORK(25) = -1
|
|
IF (INTOUT) IWORK(25) = 1
|
|
C
|
|
IF (IDID .NE. (-2)) IWORK(LIW) = IWORK(LIW) + 1
|
|
IF (T .NE. RWORK(ITSTAR)) IWORK(LIW) = 0
|
|
C
|
|
RETURN
|
|
END
|