D02QGF (PDF version)
D02 Chapter Contents
D02 Chapter Introduction
NAG Library Manual

NAG Library Routine Document

D02QGF

Note:  before using this routine, please read the Users' Note for your implementation to check the interpretation of bold italicised terms and other implementation-dependent details.

+ Contents

    1  Purpose
    7  Accuracy

1  Purpose

D02QGF is a reverse communication routine for integrating a non-stiff system of first-order ordinary differential equations using a variable-order variable-step Adams method. A root-finding facility is provided.

2  Specification

SUBROUTINE D02QGF ( NEQF, T, Y, TOUT, NEQG, ROOT, IREVCM, TRVCM, YRVCM, YPRVCM, GRVCM, KGRVCM, RWORK, LRWORK, IWORK, LIWORK, IFAIL)
INTEGER  NEQF, NEQG, IREVCM, YRVCM, YPRVCM, KGRVCM, LRWORK, IWORK(LIWORK), LIWORK, IFAIL
REAL (KIND=nag_wp)  T, Y(NEQF), TOUT, TRVCM, GRVCM, RWORK(LRWORK)
LOGICAL  ROOT

3  Description

Given the initial values x,y1,y2,,yNEQF D02QGF integrates a non-stiff system of first-order differential equations of the type
yi=fix,y1,y2,,yNEQF,  i=1,2,,NEQF,
from x=T to x=TOUT using a variable-order variable-step Adams method. You define the system by reverse communication, evaluating fi in terms of x and y1,y2,,yNEQF, and y1,y2,,yNEQF are supplied at x=T by D02QGF. The routine is capable of finding roots (values of x) of prescribed event functions of the form
gj x,y,y = 0 ,   j=1,2,,NEQG.
Each gj is considered to be independent of the others so that roots are sought of each gj individually. The root reported by the routine will be the first root encountered by any gj. Two techniques for determining the presence of a root in an integration step are available: the sophisticated method described in Watts (1985) and a simplified method whereby sign changes in each gj are looked for at the ends of each integration step. You also define each gj by reverse communication. In one-step mode the routine returns an approximation to the solution at each integration point. In interval mode this value is returned at the end of the integration range. If a root is detected this approximation is given at the root. You select the mode of operation, the error control, the root-finding technique and various optional inputs by a prior call to the setup routine D02QWF.
For a description of the practical implementation of an Adams formula see Shampine and Gordon (1975).

4  References

Shampine L F and Gordon M K (1975) Computer Solution of Ordinary Differential Equations – The Initial Value Problem W H Freeman & Co., San Francisco
Shampine L F and Watts H A (1979) DEPAC – design of a user oriented package of ODE solvers Report SAND79-2374 Sandia National Laboratory
Watts H A (1985) RDEAM – An Adams ODE code with root solving capability Report SAND85-1595 Sandia National Laboratory

5  Parameters

Note: this routine uses reverse communication. Its use involves an initial entry, intermediate exits and re-entries, and a final exit, as indicated by the parameter IREVCM. Between intermediate exits and re-entries, all parameters other than GRVCM and RWORK must remain unchanged.
1:     NEQF – INTEGERInput
On initial entry: the number of first-order ordinary differential equations to be solved by D02QGF. It must contain the same value as the parameter NEQF used in the prior call to D02QWF.
Constraint: NEQF1.
2:     T – REAL (KIND=nag_wp)Input/Output
On initial entry: that is after a call to D02QWF with STATEF='S', T must be set to the initial value of the independent variable x.
On final exit: the value of x at which y has been computed. This may be an intermediate output point, a root, TOUT or a point at which an error has occurred. If the integration is to be continued, possibly with a new value for TOUT, T must not be changed.
3:     Y(NEQF) – REAL (KIND=nag_wp) arrayInput/Output
On initial entry: the initial values of the solution y1,y2,,yNEQF.
On final exit: the computed values of the solution at the exit value of T. If the integration is to be continued, possibly with a new value for TOUT, these values must not be changed.
4:     TOUT – REAL (KIND=nag_wp)Input
On initial entry: the next value of x at which a computed solution is required. For the initial T, the input value of TOUT is used to determine the direction of integration. Integration is permitted in either direction. If TOUT=T on exit, TOUT must be reset beyond T in the direction of integration, before any continuation call.
5:     NEQG – INTEGERInput
On initial entry: the number of event functions which you are defining for root-finding. If root-finding is not required the value for NEQG must be 0. Otherwise it must be the same value as the parameter NEQG used in the prior call to D02QWF.
6:     ROOT – LOGICALOutput
On final exit: if root-finding was required (NEQG>0 on entry), then ROOT specifies whether or not the output value of the parameter T is a root of one of the event functions. If ROOT=.FALSE., then no root was detected, whereas ROOT=.TRUE. indicates a root and you should make a call to D02QYF for further information.
If root-finding was not required (NEQG=0 on entry), then ROOT=.FALSE..
7:     IREVCM – INTEGERInput/Output
On initial entry: must have the value 0.
On intermediate exit: specifies what action you must take before re-entering D02QGF with IREVCM unchanged.
IREVCM=1, 2, 3, 4, 5, 6 or 7
Indicates that you must supply y=fx,y, where x is given by TRVCM and yi is returned in Yi, for i=1,2,,NEQF when YRVCM=0 and RWORKYRVCM+i-1, for i=1,2,,NEQF when YRVCM0. yi should be placed in location RWORKYPRVCM+i-1, for i=1,2,,NEQF.
IREVCM=8
Indicates that the current step was not successful due to error test failure. The only information supplied to you on this return is the current value of the independent variable T, as given by TRVCM. No values must be changed before re-entering D02QGF. This facility enables you to determine the number of unsuccessful steps.
IREVCM=9, 10, 11 or 12
Indicates that you must supply gkx,y,y, where k is given by KGRVCM, x is given by TRVCM, yi is given by Yi and yi is given by RWORKYPRVCM-1+i. The result gk should be placed in the variable GRVCM.
On final exit: has the value 0, which indicates that an output point or root has been reached or an error has occurred (see IFAIL).
8:     TRVCM – REAL (KIND=nag_wp)Output
On intermediate exit: the current value of the independent variable.
9:     YRVCM – INTEGEROutput
On intermediate exit: with IREVCM=1, 2, 3, 4, 5, 6, 7, 9, 10, 11 or 12, YRVCM specifies the locations of the dependent variables y for use in evaluating the differential system or the event functions.
YRVCM=0
yi is given by Yi, for i=1,2,,NEQF.
YRVCM0
yi is given by RWORKYRVCM+i-1, for i=1,2,,NEQF.
10:   YPRVCM – INTEGEROutput
On intermediate exit: with IREVCM=1, 2, 3, 4, 5, 6 or 7, YPRVCM specifies the positions in RWORK at which you should place the derivatives y. yi should be placed in location RWORKYPRVCM+i-1, for i=1,2,,NEQF.
With IREVCM=9, 10, 11 or 12, YPRVCM specifies the locations of the derivatives y for use in evaluating the event functions. yi is given by RWORKYPRVCM+i-1, for i=1,2,,NEQF.
11:   GRVCM – REAL (KIND=nag_wp)Input
On initial entry: need not be set.
On intermediate re-entry: with IREVCM=9, 10, 11 or 12, GRVCM must contain the value of gkx,y,y, where k is given by KGRVCM.
12:   KGRVCM – INTEGERInput/Output
On intermediate re-entry: with IREVCM=9, 10, 11 or 12, KGRVCM must remain unchanged from a previous call to D02QGF.
On intermediate exit: with IREVCM=9, 10, 11 or 12, KGRVCM specifies which event function gkx,y,y you must evaluate.
13:   RWORK(LRWORK) – REAL (KIND=nag_wp) arrayCommunication Array
This must be the same parameter RWORK as supplied to D02QWF. It is used to pass information from D02QWF to D02QGF, and from D02QGF to D02QXF, D02QYF and D02QZF. Therefore the contents of this array must not be changed before the call to D02QGF or calling any of the routines D02QXF, D02QYF and D02QZF.
14:   LRWORK – INTEGERInput
On initial entry: the dimension of the array RWORK as declared in the (sub)program from which D02QGF is called.
This must be the same parameter LRWORK as supplied to D02QWF.
15:   IWORK(LIWORK) – INTEGER arrayCommunication Array
This must be the same parameter IWORK as supplied to D02QWF. It is used to pass information from D02QWF to D02QGF, and from D02QGF to D02QXF, D02QYF and D02QZF. Therefore the contents of this array must not be changed before the call to D02QGF or calling any of the routines D02QXF, D02QYF and D02QZF.
16:   LIWORK – INTEGERInput
On initial entry: the dimension of the array IWORK as declared in the (sub)program from which D02QGF is called.
This must be the same parameter LIWORK as supplied to D02QWF.
17:   IFAIL – INTEGERInput/Output
On initial entry: IFAIL must be set to 0, -1​ or ​1. If you are unfamiliar with this parameter you should refer to Section 3.3 in the Essential Introduction for details.
For environments where it might be inappropriate to halt program execution when an error is detected, the value -1​ or ​1 is recommended. If the output of error messages is undesirable, then the value 1 is recommended. Otherwise, because for this routine the values of the output parameters may be useful even if IFAIL0 on exit, the recommended value is -1. When the value -1​ or ​1 is used it is essential to test the value of IFAIL on exit.
On final exit: IFAIL=0 unless the routine detects an error or a warning has been flagged (see Section 6).

6  Error Indicators and Warnings

If on entry IFAIL=0 or -1, explanatory error messages are output on the current error message unit (as defined by X04AAF).
Errors or warnings detected by the routine:
IFAIL=1
On entry, the integrator detected an illegal input, or D02QWF has not been called before the call to the integrator.
This error may be caused by overwriting elements of RWORK and IWORK.
IFAIL=2
The maximum number of steps has been attempted (at a cost of about 2 derivative evaluations per step). (See parameter MAXSTP in D02QWF.) If integration is to be continued then you need only reset IFAIL and call the routine again and a further MAXSTP steps will be attempted.
IFAIL=3
The step size needed to satisfy the error requirements is too small for the machine precision being used. (See parameter TOLFAC in D02QXF.)
IFAIL=4
Some error weight wi became zero during the integration (see parameters VECTOL, RTOL and ATOL in D02QWF.) Pure relative error control (ATOL=0.0) was requested on a variable (the ith) which has now become zero. (See parameter BADCMP in D02QXF.) The integration was successful as far as T.
IFAIL=5
The problem appears to be stiff (see the D02 Chapter Introduction for a discussion of the term ‘stiff’). Although it is inefficient to use this integrator to solve stiff problems, integration may be continued by resetting IFAIL and calling the routine again.
IFAIL=6
A change in sign of an event function has been detected but the root-finding process appears to have converged to a singular point T rather than a root. Integration may be continued by resetting IFAIL and calling the routine again.
IFAIL=7
The code has detected two successive error exits at the current value of T and cannot proceed. Check all input variables.

7  Accuracy

The accuracy of integration is determined by the parameters VECTOL, RTOL and ATOL in a prior call to D02QWF. Note that only the local error at each step is controlled by these parameters. The error estimates obtained are not strict bounds but are usually reliable over one step. Over a number of steps the overall error may accumulate in various ways, depending on the properties of the differential equation system. The code is designed so that a reduction in the tolerances should lead to an approximately proportional reduction in the error. You are strongly recommended to call D02QGF with more than one set of tolerances and to compare the results obtained to estimate their accuracy.
The accuracy obtained depends on the type of error test used. If the solution oscillates around zero a relative error test should be avoided, whereas if the solution is exponentially increasing an absolute error test should not be used. If different accuracies are required for different components of the solution then a component-wise error test should be used. For a description of the error test see the specifications of the parameters VECTOL, RTOL and ATOL in the routine document for D02QWF.
The accuracy of any roots located will depend on the accuracy of integration and may also be restricted by the numerical properties of gx,y,y. When evaluating g you should try to write the code so that unnecessary cancellation errors will be avoided.

8  Further Comments

If D02QGF fails with IFAIL=3 then the combination of ATOL and RTOL may be so small that a solution cannot be obtained, in which case the routine should be called again with larger values for RTOL and/or ATOL (see D02QWF). If the accuracy requested is really needed then you should consider whether there is a more fundamental difficulty. For example:
(a) in the region of a singularity the solution components will usually be of a large magnitude. D02QGF could be used in one-step mode to monitor the size of the solution with the aim of trapping the solution before the singularity. In any case numerical integration cannot be continued through a singularity, and analytical treatment may be necessary;
(b) for ‘stiff’ equations, where the solution contains rapidly decaying components, the routine will require a very small step size to preserve stability. This will usually be exhibited by excessive computing time and sometimes an error exit with IFAIL=3, but usually an error exit with IFAIL=2 or 5. The Adams methods are not efficient in such cases and you should consider using a routine from the sub-chapter D02M–N. A high proportion of failed steps (see parameter NFAIL in D02QXF) may indicate stiffness but there may be other reasons for this phenomenon.
D02QGF can be used for producing results at short intervals (for example, for graph plotting); you should set CRIT=.TRUE. and TCRIT to the last output point required in a prior call to D02QWF and then set TOUT appropriately for each output point in turn in the call to D02QGF.

9  Example

This example solves the following system (for a projectile)
y=tanϕ v= -0.032 tanϕ v - 0.02v cosϕ ϕ= -0.032 v2
over an interval 0.0,10.0 starting with values y=0.5, v=0.5 and ϕ=π/5 using scalar error control (VECTOL=.FALSE.) until the first point where y=0.0 is encountered.
Also, D02QGF is used to produce output at intervals of 2.0.

9.1  Program Text

Program Text (d02qgfe.f90)

9.2  Program Data

Program Data (d02qgfe.d)

9.3  Program Results

Program Results (d02qgfe.r)

Produced by GNUPLOT 4.4 patchlevel 0 -1 -0.5 0 0.5 1 1.5 2 0 1 2 3 4 5 6 7 8 Solution x Example Program ODE Solution using Adams Method with Root-finding height velocity angle

D02QGF (PDF version)
D02 Chapter Contents
D02 Chapter Introduction
NAG Library Manual

© The Numerical Algorithms Group Ltd, Oxford, UK. 2012