NAG FL Interface
d03pkf (dim1_​parab_​dae_​keller)

1 Purpose

d03pkf integrates a system of linear or nonlinear, first-order, time-dependent partial differential equations (PDEs) in one space variable, with scope for coupled ordinary differential equations (ODEs). The spatial discretization is performed using the Keller box scheme and the method of lines is employed to reduce the PDEs to a system of ODEs. The resulting system is solved using a Backward Differentiation Formula (BDF) method or a Theta method (switching between Newton's method and functional iteration).

2 Specification

Fortran Interface
Subroutine d03pkf ( npde, ts, tout, pdedef, bndary, u, npts, x, nleft, nv, odedef, nxi, xi, neqn, rtol, atol, itol, norm, laopt, algopt, rsave, lrsave, isave, lisave, itask, itrace, ind, ifail)
Integer, Intent (In) :: npde, npts, nleft, nv, nxi, neqn, itol, lrsave, lisave, itask, itrace
Integer, Intent (Inout) :: isave(lisave), ind, ifail
Real (Kind=nag_wp), Intent (In) :: tout, x(npts), xi(nxi), rtol(*), atol(*), algopt(30)
Real (Kind=nag_wp), Intent (Inout) :: ts, u(neqn), rsave(lrsave)
Character (1), Intent (In) :: norm, laopt
External :: pdedef, bndary, odedef
C Header Interface
#include <nag.h>
void  d03pkf_ (const Integer *npde, double *ts, const double *tout,
void (NAG_CALL *pdedef)(const Integer *npde, const double *t, const double *x, const double u[], const double ut[], const double ux[], const Integer *nv, const double v[], const double vdot[], double res[], Integer *ires),
void (NAG_CALL *bndary)(const Integer *npde, const double *t, const Integer *ibnd, const Integer *nobc, const double u[], const double ut[], const Integer *nv, const double v[], const double vdot[], double res[], Integer *ires),
double u[], const Integer *npts, const double x[], const Integer *nleft, const Integer *nv,
void (NAG_CALL *odedef)(const Integer *npde, const double *t, const Integer *nv, const double v[], const double vdot[], const Integer *nxi, const double xi[], const double ucp[], const double ucpx[], const double ucpt[], double r[], Integer *ires),
const Integer *nxi, const double xi[], const Integer *neqn, const double rtol[], const double atol[], const Integer *itol, const char *norm, const char *laopt, const double algopt[], double rsave[], const Integer *lrsave, Integer isave[], const Integer *lisave, const Integer *itask, const Integer *itrace, Integer *ind, Integer *ifail, const Charlen length_norm, const Charlen length_laopt)
The routine may be called by the names d03pkf or nagf_pde_dim1_parab_dae_keller.

3 Description

d03pkf integrates the system of first-order PDEs and coupled ODEs
Gi x,t,U,Ux,Ut,V,V. = 0 ,   i=1,2,,npde ,   axb,tt0 , (1)
Ri t,V,V.,ξ,U*,Ux*,Ut* = 0 ,   i=1,2,,nv . (2)
In the PDE part of the problem given by (1), the functions Gi must have the general form
Gi = j=1 npde Pi,j Uj t + j=1 nv Qi,j V.j + Si = 0 ,   i=1,2,,npde , (3)
where Pi,j, Qi,j and Si depend on x,t,U,Ux and V.
The vector U is the set of PDE solution values
U x,t = U 1 x,t ,, U npde x,t T ,  
and the vector Ux is the partial derivative with respect to x. The vector V is the set of ODE solution values
Vt=V1t,,VnvtT,  
and V. denotes its derivative with respect to time.
In the ODE part given by (2), ξ represents a vector of nξ spatial coupling points at which the ODEs are coupled to the PDEs. These points may or may not be equal to some of the PDE spatial mesh points. U*, Ux* and Ut* are the functions U, Ux and Ut evaluated at these coupling points. Each Ri may only depend linearly on time derivatives. Hence equation (2) may be written more precisely as
R=A-BV.-CUt*, (4)
where R=R1,,RnvT, A is a vector of length nv, B is an nv by nv matrix, C is an nv by nξ×npde matrix. The entries in A, B and C may depend on t, ξ, U*, Ux* and V. In practice you only need to supply a vector of information to define the ODEs and not the matrices B and C. (See Section 5 for the specification of odedef.)
The integration in time is from t0 to tout, over the space interval axb, where a=x1 and b=xnpts are the leftmost and rightmost points of a user-defined mesh x1,x2,,xnpts.
The PDE system which is defined by the functions Gi must be specified in pdedef.
The initial values of the functions Ux,t and Vt must be given at t=t0.
For a first-order system of PDEs, only one boundary condition is required for each PDE component Ui. The npde boundary conditions are separated into na at the left-hand boundary x=a, and nb at the right-hand boundary x=b, such that na+nb=npde. The position of the boundary condition for each component should be chosen with care; the general rule is that if the characteristic direction of Ui at the left-hand boundary (say) points into the interior of the solution domain, then the boundary condition for Ui should be specified at the left-hand boundary. Incorrect positioning of boundary conditions generally results in initialization or integration difficulties in the underlying time integration routines.
The boundary conditions have the form:
G i L x,t,U, U t ,V, V . = 0   at ​ x = a ,   i=1,2,,na , (5)
at the left-hand boundary, and
G i R x,t,U, U t ,V, V . = 0   at ​ x = b,   i=1,2,,nb, (6)
at the right-hand boundary.
Note that the functions GiL and GiR must not depend on Ux, since spatial derivatives are not determined explicitly in the Keller box scheme. If the problem involves derivative (Neumann) boundary conditions then it is generally possible to restate such boundary conditions in terms of permissible variables. Also note that GiL and GiR must be linear with respect to time derivatives, so that the boundary conditions have the general form:
j=1npdeEi,jL Uj t +j=1nvHi,jLV.j+KiL=0,   i=1,2,,na, (7)
at the left-hand boundary, and
j=1npdeEi,jR Uj t +j=1nvHi,jRV.j+KiR=0,   i=1,2,,nb, (8)
at the right-hand boundary, where Ei,jL, Ei,jR, Hi,jL, Hi,jR, KiL and KiR depend on x,t,U and V only.
The boundary conditions must be specified in bndary.
The problem is subject to the following restrictions:
  1. (i)Pi,j, Qi,j and Si must not depend on any time derivatives;
  2. (ii)t0<tout, so that integration is in the forward direction;
  3. (iii)The evaluation of the function Gi is done approximately at the mid-points of the mesh xi, for i=1,2,,npts, by calling the pdedef for each mid-point in turn. Any discontinuities in the function must therefore be at one or more of the mesh points x1,x2,,xnpts;
  4. (iv)At least one of the functions Pi,j must be nonzero so that there is a time derivative present in the PDE problem.
The algebraic-differential equation system which is defined by the functions Ri must be specified in odedef. You must also specify the coupling points ξ in the array xi.
The parabolic equations are approximated by a system of ODEs in time for the values of Ui at mesh points. In this method of lines approach the Keller box scheme (see Keller (1970)) is applied to each PDE in the space variable only, resulting in a system of ODEs in time for the values of Ui at each mesh point. In total there are npde×npts+nv ODEs in time direction. This system is then integrated forwards in time using a Backward Differentiation Formula (BDF) or a Theta method.

4 References

Berzins M (1990) Developments in the NAG Library software for parabolic equations Scientific Software Systems (eds J C Mason and M G Cox) 59–72 Chapman and Hall
Berzins M, Dew P M and Furzeland R M (1989) Developing software for time-dependent problems using the method of lines and differential-algebraic integrators Appl. Numer. Math. 5 375–397
Berzins M and Furzeland R M (1992) An adaptive theta method for the solution of stiff and nonstiff differential equations Appl. Numer. Math. 9 1–19
Keller H B (1970) A new difference scheme for parabolic problems Numerical Solutions of Partial Differential Equations (ed J Bramble) 2 327–350 Academic Press
Pennington S V and Berzins M (1994) New NAG Library software for first-order partial differential equations ACM Trans. Math. Softw. 20 63–99

5 Arguments

1: npde Integer Input
On entry: the number of PDEs to be solved.
Constraint: npde1.
2: ts Real (Kind=nag_wp) Input/Output
On entry: the initial value of the independent variable t.
Constraint: ts<tout.
On exit: the value of t corresponding to the solution in u. Normally ts=tout.
3: tout Real (Kind=nag_wp) Input
On entry: the final value of t to which the integration is to be carried out.
4: pdedef Subroutine, supplied by the user. External Procedure
pdedef must evaluate the functions Gi which define the system of PDEs. pdedef is called approximately midway between each pair of mesh points in turn by d03pkf.
The specification of pdedef is:
Fortran Interface
Subroutine pdedef ( npde, t, x, u, ut, ux, nv, v, vdot, res, ires)
Integer, Intent (In) :: npde, nv
Integer, Intent (Inout) :: ires
Real (Kind=nag_wp), Intent (In) :: t, x, u(npde), ut(npde), ux(npde), v(nv), vdot(nv)
Real (Kind=nag_wp), Intent (Out) :: res(npde)
C Header Interface
void  pdedef_ (const Integer *npde, const double *t, const double *x, const double u[], const double ut[], const double ux[], const Integer *nv, const double v[], const double vdot[], double res[], Integer *ires)
1: npde Integer Input
On entry: the number of PDEs in the system.
2: t Real (Kind=nag_wp) Input
On entry: the current value of the independent variable t.
3: x Real (Kind=nag_wp) Input
On entry: the current value of the space variable x.
4: unpde Real (Kind=nag_wp) array Input
On entry: ui contains the value of the component Uix,t, for i=1,2,,npde.
5: utnpde Real (Kind=nag_wp) array Input
On entry: uti contains the value of the component Uix,t t , for i=1,2,,npde.
6: uxnpde Real (Kind=nag_wp) array Input
On entry: uxi contains the value of the component Uix,t x , for i=1,2,,npde.
7: nv Integer Input
On entry: the number of coupled ODEs in the system.
8: vnv Real (Kind=nag_wp) array Input
On entry: if nv>0, vi contains the value of the component Vit, for i=1,2,,nv.
9: vdotnv Real (Kind=nag_wp) array Input
On entry: if nv>0, vdoti contains the value of component V.it, for i=1,2,,nv.
10: resnpde Real (Kind=nag_wp) array Output
On exit: resi must contain the ith component of G, for i=1,2,,npde, where G is defined as
Gi=j=1npdePi,j Uj t +j=1nvQi,jV.j, (9)
i.e., only terms depending explicitly on time derivatives, or
Gi=j=1npdePi,j Uj t +j=1nvQi,jV.j+Si, (10)
i.e., all terms in equation (3).
The definition of G is determined by the input value of ires.
11: ires Integer Input/Output
On entry: the form of Gi that must be returned in the array res.
ires=-1
Equation (9) must be used.
ires=1
Equation (10) must be used.
On exit: should usually remain unchanged. However, you may set ires to force the integration routine to take certain actions, as described below:
ires=2
Indicates to the integrator that control should be passed back immediately to the calling (sub)routine with the error indicator set to ifail=6.
ires=3
Indicates to the integrator that the current time step should be abandoned and a smaller time step used instead. You may wish to set ires=3 when a physically meaningless input or output value has been generated. If you consecutively set ires=3, d03pkf returns to the calling subroutine with the error indicator set to ifail=4.
pdedef must either be a module subprogram USEd by, or declared as EXTERNAL in, the (sub)program from which d03pkf is called. Arguments denoted as Input must not be changed by this procedure.
Note: pdedef should not return floating-point NaN (Not a Number) or infinity values, since these are not handled by d03pkf. If your code inadvertently does return any NaNs or infinities, d03pkf is likely to produce unexpected results.
5: bndary Subroutine, supplied by the user. External Procedure
bndary must evaluate the functions GiL and GiR which describe the boundary conditions, as given in (5) and (6).
The specification of bndary is:
Fortran Interface
Subroutine bndary ( npde, t, ibnd, nobc, u, ut, nv, v, vdot, res, ires)
Integer, Intent (In) :: npde, ibnd, nobc, nv
Integer, Intent (Inout) :: ires
Real (Kind=nag_wp), Intent (In) :: t, u(npde), ut(npde), v(nv), vdot(nv)
Real (Kind=nag_wp), Intent (Out) :: res(nobc)
C Header Interface
void  bndary_ (const Integer *npde, const double *t, const Integer *ibnd, const Integer *nobc, const double u[], const double ut[], const Integer *nv, const double v[], const double vdot[], double res[], Integer *ires)
1: npde Integer Input
On entry: the dimension of the array u and the dimension of the array ut as declared in the (sub)program from which d03pkf is called. The number of PDEs in the system.
2: t Real (Kind=nag_wp) Input
On entry: the current value of the independent variable t.
3: ibnd Integer Input
On entry: specifies which boundary conditions are to be evaluated.
ibnd=0
bndary must compute the left-hand boundary condition at x=a.
ibnd0
bndary must compute the right-hand boundary condition at x=b.
4: nobc Integer Input
On entry: specifies the number of boundary conditions at the boundary specified by ibnd.
5: unpde Real (Kind=nag_wp) array Input
On entry: ui contains the value of the component Uix,t at the boundary specified by ibnd, for i=1,2,,npde.
6: utnpde Real (Kind=nag_wp) array Input
On entry: uti contains the value of the component Uix,t t at the boundary specified by ibnd, for i=1,2,,npde.
7: nv Integer Input
On entry: the number of coupled ODEs in the system.
8: vnv Real (Kind=nag_wp) array Input
On entry: if nv>0, vi contains the value of the component Vit, for i=1,2,,nv.
9: vdotnv Real (Kind=nag_wp) array Input
On entry: if nv>0, vdoti contains the value of component V.it, for i=1,2,,nv.
Note: vdoti, for i=1,2,,nv, may only appear linearly as in (7) and (8).
10: resnobc Real (Kind=nag_wp) array Output
On exit: resi must contain the ith component of GL or GR, depending on the value of ibnd, for i=1,2,,nobc, where GL is defined as
GiL=j=1npdeEi,jL Uj t +j=1nvHi,jLV.j, (11)
i.e., only terms depending explicitly on time derivatives, or
GiL=j=1npdeEi,jL Uj t +j=1nvHi,jLV.j+KiL, (12)
i.e., all terms in equation (7), and similarly for GiR.
The definitions of GL and GR are determined by the input value of ires.
11: ires Integer Input/Output
On entry: the form of GiL (or GiR) that must be returned in the array res.
ires=-1
Equation (11) must be used.
ires=1
Equation (12) must be used.
On exit: should usually remain unchanged. However, you may set ires to force the integration routine to take certain actions as described below:
ires=2
Indicates to the integrator that control should be passed back immediately to the calling (sub)routine with the error indicator set to ifail=6.
ires=3
Indicates to the integrator that the current time step should be abandoned and a smaller time step used instead. You may wish to set ires=3 when a physically meaningless input or output value has been generated. If you consecutively set ires=3, d03pkf returns to the calling subroutine with the error indicator set to ifail=4.
bndary must either be a module subprogram USEd by, or declared as EXTERNAL in, the (sub)program from which d03pkf is called. Arguments denoted as Input must not be changed by this procedure.
Note: bndary should not return floating-point NaN (Not a Number) or infinity values, since these are not handled by d03pkf. If your code inadvertently does return any NaNs or infinities, d03pkf is likely to produce unexpected results.
6: uneqn Real (Kind=nag_wp) array Input/Output
On entry: the initial values of the dependent variables defined as follows:
  • unpde×j-1+i contain Uixj,t0, for i=1,2,,npde and j=1,2,,npts, and
  • unpts×npde+i contain Vit0, for i=1,2,,nv.
On exit: the computed solution Uixj,t, for i=1,2,,npde and j=1,2,,npts, and Vkt, for k=1,2,,nv, evaluated at t=ts, as follows:
  • unpde×j-1+i contain Uixj,t, for i=1,2,,npde and j=1,2,,npts, and
  • unpts×npde+i contain Vit, for i=1,2,,nv.
7: npts Integer Input
On entry: the number of mesh points in the interval a,b.
Constraint: npts3.
8: xnpts Real (Kind=nag_wp) array Input
On entry: the mesh points in the space direction. x1 must specify the left-hand boundary, a, and xnpts must specify the right-hand boundary, b.
Constraint: x1<x2<<xnpts.
9: nleft Integer Input
On entry: the number na of boundary conditions at the left-hand mesh point x1.
Constraint: 0nleftnpde.
10: nv Integer Input
On entry: the number of coupled ODE components.
Constraint: nv0.
11: odedef Subroutine, supplied by the NAG Library or the user. External Procedure
odedef must evaluate the functions R, which define the system of ODEs, as given in (4).
If you wish to compute the solution of a system of PDEs only (i.e., nv=0), odedef must be the dummy routine d03pek. (d03pek is included in the NAG Library.)
The specification of odedef is:
Fortran Interface
Subroutine odedef ( npde, t, nv, v, vdot, nxi, xi, ucp, ucpx, ucpt, r, ires)
Integer, Intent (In) :: npde, nv, nxi
Integer, Intent (Inout) :: ires
Real (Kind=nag_wp), Intent (In) :: t, v(nv), vdot(nv), xi(nxi), ucp(npde,nxi), ucpx(npde,nxi), ucpt(npde,nxi)
Real (Kind=nag_wp), Intent (Out) :: r(nv)
C Header Interface
void  odedef_ (const Integer *npde, const double *t, const Integer *nv, const double v[], const double vdot[], const Integer *nxi, const double xi[], const double ucp[], const double ucpx[], const double ucpt[], double r[], Integer *ires)
1: npde Integer Input
On entry: the number of PDEs in the system.
2: t Real (Kind=nag_wp) Input
On entry: the current value of the independent variable t.
3: nv Integer Input
On entry: the number of coupled ODEs in the system.
4: vnv Real (Kind=nag_wp) array Input
On entry: if nv>0, vi contains the value of the component Vit, for i=1,2,,nv.
5: vdotnv Real (Kind=nag_wp) array Input
On entry: if nv>0, vdoti contains the value of component V.it, for i=1,2,,nv.
6: nxi Integer Input
On entry: the number of ODE/PDE coupling points.
7: xinxi Real (Kind=nag_wp) array Input
On entry: if nxi>0, xii contains the ODE/PDE coupling points, ξi, for i=1,2,,nxi.
8: ucpnpdenxi Real (Kind=nag_wp) array Input
On entry: if nxi>0, ucpij contains the value of Uix,t at the coupling point x=ξj, for i=1,2,,npde and j=1,2,,nxi.
9: ucpxnpdenxi Real (Kind=nag_wp) array Input
On entry: if nxi>0, ucpxij contains the value of Uix,t x at the coupling point x=ξj, for i=1,2,,npde and j=1,2,,nxi.
10: ucptnpdenxi Real (Kind=nag_wp) array Input
On entry: if nxi>0, ucptij contains the value of Ui t at the coupling point x=ξj, for i=1,2,,npde and j=1,2,,nxi.
11: rnv Real (Kind=nag_wp) array Output
On exit: if nv>0, ri must contain the ith component of R, for i=1,2,,nv, where R is defined as
R=-BV.-CUt*, (13)
i.e., only terms depending explicitly on time derivatives, or
R=A-BV.-CUt*, (14)
i.e., all terms in equation (4). The definition of R is determined by the input value of ires.
12: ires Integer Input/Output
On entry: the form of R that must be returned in the array r.
ires=-1
Equation (13) must be used.
ires=1
Equation (14) must be used.
On exit: should usually remain unchanged. However, you may reset ires to force the integration routine to take certain actions, as described below:
ires=2
Indicates to the integrator that control should be passed back immediately to the calling (sub)routine with the error indicator set to ifail=6.
ires=3
Indicates to the integrator that the current time step should be abandoned and a smaller time step used instead. You may wish to set ires=3 when a physically meaningless input or output value has been generated. If you consecutively set ires=3, d03pkf returns to the calling subroutine with the error indicator set to ifail=4.
odedef must either be a module subprogram USEd by, or declared as EXTERNAL in, the (sub)program from which d03pkf is called. Arguments denoted as Input must not be changed by this procedure.
Note: odedef should not return floating-point NaN (Not a Number) or infinity values, since these are not handled by d03pkf. If your code inadvertently does return any NaNs or infinities, d03pkf is likely to produce unexpected results.
12: nxi Integer Input
On entry: the number of ODE/PDE coupling points.
Constraints:
  • if nv=0, nxi=0;
  • if nv>0, nxi0.
13: xinxi Real (Kind=nag_wp) array Input
On entry: xii, for i=1,2,,nxi, must be set to the ODE/PDE coupling points, ξi.
Constraint: x1xi1<xi2<<xinxixnpts.
14: neqn Integer Input
On entry: the number of ODEs in the time direction.
Constraint: neqn=npde×npts+nv.
15: rtol* Real (Kind=nag_wp) array Input
Note: the dimension of the array rtol must be at least 1 if itol=1 or 2 and at least neqn if itol=3 or 4.
On entry: the relative local error tolerance.
Constraint: rtoli0.0 for all relevant i.
16: atol* Real (Kind=nag_wp) array Input
Note: the dimension of the array atol must be at least 1 if itol=1 or 3 and at least neqn if itol=2 or 4.
On entry: the absolute local error tolerance.
Constraint: atoli0.0 for all relevant i.
Note: corresponding elements of rtol and atol cannot both be 0.0.
17: itol Integer Input
On entry: a value to indicate the form of the local error test. itol indicates to d03pkf whether to interpret either or both of rtol or atol as a vector or scalar. The error test to be satisfied is ei/wi<1.0, where wi is defined as follows:
itol rtol atol wi
1 scalar scalar rtol1×ui+atol1
2 scalar vector rtol1×ui+atoli
3 vector scalar rtoli×ui+atol1
4 vector vector rtoli×ui+atoli
In the above, ei denotes the estimated local error for the ith component of the coupled PDE/ODE system in time, ui, for i=1,2,,neqn.
The choice of norm used is defined by the argument norm.
Constraint: 1itol4.
18: norm Character(1) Input
On entry: the type of norm to be used.
norm='M'
Maximum norm.
norm='A'
Averaged L2 norm.
If unorm denotes the norm of the vector u of length neqn, then for the averaged L2 norm
unorm=1neqni=1neqnui/wi2,  
while for the maximum norm
u norm = maxi ui / wi .  
See the description of itol for the formulation of the weight vector w.
Constraint: norm='M' or 'A'.
19: laopt Character(1) Input
On entry: the type of matrix algebra required.
laopt='F'
Full matrix methods to be used.
laopt='B'
Banded matrix methods to be used.
laopt='S'
Sparse matrix methods to be used.
Constraint: laopt='F', 'B' or 'S'.
Note: you are recommended to use the banded option when no coupled ODEs are present (i.e., nv=0).
20: algopt30 Real (Kind=nag_wp) array Input
On entry: may be set to control various options available in the integrator. If you wish to employ all the default options, algopt1 should be set to 0.0. Default values will also be used for any other elements of algopt set to zero. The permissible values, default values, and meanings are as follows:
algopt1
Selects the ODE integration method to be used. If algopt1=1.0, a BDF method is used and if algopt1=2.0, a Theta method is used. The default value is algopt1=1.0.
If algopt1=2.0, then algopti, for i=2,3,4, are not used.
algopt2
Specifies the maximum order of the BDF integration formula to be used. algopt2 may be 1.0, 2.0, 3.0, 4.0 or 5.0. The default value is algopt2=5.0.
algopt3
Specifies what method is to be used to solve the system of nonlinear equations arising on each step of the BDF method. If algopt3=1.0 a modified Newton iteration is used and if algopt3=2.0 a functional iteration method is used. If functional iteration is selected and the integrator encounters difficulty, there is an automatic switch to the modified Newton iteration. The default value is algopt3=1.0.
algopt4
Specifies whether or not the Petzold error test is to be employed. The Petzold error test results in extra overhead but is more suitable when algebraic equations are present, such as Pi,j=0.0, for j=1,2,,npde, for some i or when there is no V.it dependence in the coupled ODE system. If algopt4=1.0, the Petzold test is used. If algopt4=2.0, the Petzold test is not used. The default value is algopt4=1.0.
If algopt1=1.0, algopti, for i=5,6,7, are not used.
algopt5
Specifies the value of Theta to be used in the Theta integration method. 0.51algopt50.99. The default value is algopt5=0.55.
algopt6
Specifies what method is to be used to solve the system of nonlinear equations arising on each step of the Theta method. If algopt6=1.0, a modified Newton iteration is used and if algopt6=2.0, a functional iteration method is used. The default value is algopt6=1.0.
algopt7
Specifies whether or not the integrator is allowed to switch automatically between modified Newton and functional iteration methods in order to be more efficient. If algopt7=1.0, switching is allowed and if algopt7=2.0, switching is not allowed. The default value is algopt7=1.0.
algopt11
Specifies a point in the time direction, tcrit, beyond which integration must not be attempted. The use of tcrit is described under the argument itask. If algopt10.0, a value of 0.0, for algopt11, say, should be specified even if itask subsequently specifies that tcrit will not be used.
algopt12
Specifies the minimum absolute step size to be allowed in the time integration. If this option is not required, algopt12 should be set to 0.0.
algopt13
Specifies the maximum absolute step size to be allowed in the time integration. If this option is not required, algopt13 should be set to 0.0.
algopt14
Specifies the initial step size to be attempted by the integrator. If algopt14=0.0, the initial step size is calculated internally.
algopt15
Specifies the maximum number of steps to be attempted by the integrator in any one call. If algopt15=0.0, no limit is imposed.
algopt23
Specifies what method is to be used to solve the nonlinear equations at the initial point to initialize the values of U, Ut, V and V.. If algopt23=1.0, a modified Newton iteration is used and if algopt23=2.0, functional iteration is used. The default value is algopt23=1.0.
algopt29 and algopt30 are used only for the sparse matrix algebra option, i.e., laopt='S'.
algopt29
Governs the choice of pivots during the decomposition of the first Jacobian matrix. It should lie in the range 0.0<algopt29<1.0, with smaller values biasing the algorithm towards maintaining sparsity at the expense of numerical stability. If algopt29 lies outside this range then the default value is used. If the routines regard the Jacobian matrix as numerically singular then increasing algopt29 towards 1.0 may help, but at the cost of increased fill-in. The default value is algopt29=0.1.
algopt30
Used as a relative pivot threshold during subsequent Jacobian decompositions (see algopt29) below which an internal error is invoked. algopt30 must be greater than zero, otherwise the default value is used. If algopt30 is greater than 1.0 no check is made on the pivot size, and this may be a necessary option if the Jacobian is found to be numerically singular (see algopt29). The default value is algopt30=0.0001.
21: rsavelrsave Real (Kind=nag_wp) array Communication Array
If ind=0, rsave need not be set on entry.
If ind=1, rsave must be unchanged from the previous call to the routine because it contains required information about the iteration.
22: lrsave Integer Input
On entry: the dimension of the array rsave as declared in the (sub)program from which d03pkf is called. Its size depends on the type of matrix algebra selected.
If laopt='F', lrsaveneqn×neqn+neqn+nwkres+lenode.
If laopt='B', lrsave2ml+mu+2×neqn+nwkres+lenode.
If laopt='S', lrsave4neqn+11neqn/2+1+nwkres+lenode.
Where ml and mu are the lower and upper half bandwidths given by ml=npde+nleft-1 such that
for problems involving PDEs only,
mu=2npde-nleft-1;
for coupled PDE/ODE problems,
ml=mu=neqn-1.
Where nwkres is defined by
if nv>0​ and ​nxi>0,
nwkres=npde3npde+6nxi+npts+15+nxi+nv+7npts+2;
if nv>0​ and ​nxi=0,
nwkres=npde3npde+npts+21+nv+7npts+3;
if nv=0,
nwkres=npde3npde+npts+21+7npts+4.
Where lenode is defined by
if the BDF method is used,
lenode=6+intalgopt2×neqn+50;
if the Theta method is used,
lenode=9neqn+50.
Note: when using the sparse option, the value of lrsave may be too small when supplied to the integrator. An estimate of the minimum size of lrsave is printed on the current error message unit if itrace>0 and the routine returns with ifail=15.
23: isavelisave Integer array Communication Array
If ind=0, isave need not be set.
If ind=1, isave must be unchanged from the previous call to the routine because it contains required information about the iteration. In particular the following components of the array isave concern the efficiency of the integration:
isave1
Contains the number of steps taken in time.
isave2
Contains the number of residual evaluations of the resulting ODE system used. One such evaluation involves evaluating the PDE functions at all the mesh points, as well as one evaluation of the functions in the boundary conditions.
isave3
Contains the number of Jacobian evaluations performed by the time integrator.
isave4
Contains the order of the ODE method last used in the time integration.
isave5
Contains the number of Newton iterations performed by the time integrator. Each iteration involves residual evaluation of the resulting ODE system followed by a back-substitution using the LU decomposition of the Jacobian matrix.
24: lisave Integer Input
On entry: the dimension of the array isave as declared in the (sub)program from which d03pkf is called. Its size depends on the type of matrix algebra selected:
  • if laopt='F', lisave24;
  • if laopt='B', lisaveneqn+24;
  • if laopt='S', lisave25×neqn+24.
Note: when using the sparse option, the value of lisave may be too small when supplied to the integrator. An estimate of the minimum size of lisave is printed on the current error message unit if itrace>0 and the routine returns with ifail=15.
25: itask Integer Input
On entry: the task to be performed by the ODE integrator.
itask=1
Normal computation of output values u at t=tout (by overshooting and interpolating).
itask=2
Take one step in the time direction and return.
itask=3
Stop at first internal integration point at or beyond t=tout.
itask=4
Normal computation of output values u at t=tout but without overshooting t=tcrit where tcrit is described under the argument algopt.
itask=5
Take one step in the time direction and return, without passing tcrit, where tcrit is described under the argument algopt.
Constraint: itask=1, 2, 3, 4 or 5.
26: itrace Integer Input
On entry: the level of trace information required from d03pkf and the underlying ODE solver as follows:
itrace-1
No output is generated.
itrace=0
Only warning messages from the PDE solver are printed on the current error message unit (see x04aaf).
itrace=1
Output from the underlying ODE solver is printed on the current advisory message unit (see x04abf). This output contains details of Jacobian entries, the nonlinear iteration and the time integration during the computation of the ODE system.
itrace=2
Output from the underlying ODE solver is similar to that produced when itrace=1, except that the advisory messages are given in greater detail.
itrace3
Output from the underlying ODE solver is similar to that produced when itrace=2, except that the advisory messages are given in greater detail.
You advised to set itrace=0, unless you are experienced with Sub-chapter D02MN.
27: ind Integer Input/Output
On entry: indicates whether this is a continuation call or a new integration.
ind=0
Starts or restarts the integration in time.
ind=1
Continues the integration after an earlier exit from the routine. In this case, only the arguments tout and ifail should be reset between calls to d03pkf.
Constraint: ind=0 or 1.
On exit: ind=1.
28: ifail Integer Input/Output
On entry: ifail must be set to 0, -1 or 1. If you are unfamiliar with this argument you should refer to Section 4 in the Introduction to the NAG Library FL Interface 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, if you are not familiar with this argument, the recommended value is 0. When the value -1 or 1 is used it is essential to test the value of ifail on exit.
On 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, at least one point in xi lies outside x1,xnpts: x1=value and xnpts=value.
On entry, i=value, xi=value, j=value and xj=value.
Constraint: x1<x2<<xnpts.
On entry, i=value, xii+1=value and xii=value.
Constraint: xii+1>xii.
On entry, i=value and atoli=value.
Constraint: atoli0.0.
On entry, i=value and j=value.
Constraint: corresponding elements atoli and rtolj cannot both be 0.0.
On entry, i=value and rtoli=value.
Constraint: rtoli0.0.
On entry, ind=value.
Constraint: ind=0 or 1.
On entry, itask=value.
Constraint: itask=1, 2, 3, 4 or 5.
On entry, itol=value.
Constraint: itol=1, 2, 3 or 4.
On entry, laopt=value.
Constraint: laopt='F', 'B' or 'S'.
On entry, lisave=value.
Constraint: lisavevalue.
On entry, lrsave=value.
Constraint: lrsavevalue.
On entry, neqn=value, npde=value, npts=value and nv=value.
Constraint: neqn=npde×npts+nv.
On entry, nleft=value, npde=value.
Constraint: nleftnpde.
On entry, nleft=value.
Constraint: nleft0.
On entry, norm=value.
Constraint: norm='A' or 'M'.
On entry, npde=value.
Constraint: npde1.
On entry, npts=value.
Constraint: npts3.
On entry, nv=value.
Constraint: nv0.
On entry, nv=value and nxi=value.
Constraint: nxi=0 when nv=0.
On entry, nv=value and nxi=value.
Constraint: nxi0 when nv>0.
On entry, on initial entry ind=1.
Constraint: on initial entry ind=0.
On entry, tout=value and ts=value.
Constraint: tout>ts.
On entry, tout-ts is too small: tout=value and ts=value.
ifail=2
Underlying ODE solver cannot make further progress from the point ts with the supplied values of atol and rtol. ts=value.
ifail=3
Repeated errors in an attempted step of underlying ODE solver. Integration was successful as far as ts: ts=value.
In the underlying ODE solver, there were repeated error test failures on an attempted step, before completing the requested task, but the integration was successful as far as t=ts. The problem may have a singularity, or the error requirement may be inappropriate. Incorrect positioning of boundary conditions may also result in this error.
ifail=4
In setting up the ODE system an internal auxiliary was unable to initialize the derivative. This could be due to your setting ires=3 in pdedef or bndary.
ifail=5
Singular Jacobian of ODE system. Check problem formulation.
ifail=6
In evaluating residual of ODE system, ires=2 has been set in pdedef, bndary, or odedef. Integration is successful as far as ts: ts=value.
ifail=7
atol and rtol were too small to start integration.
ifail=8
ires set to an invalid value in call to pdedef, bndary, or odedef.
ifail=9
Serious error in internal call to an auxiliary. Increase itrace for further details.
ifail=10
Integration completed, but small changes in atol or rtol are unlikely to result in a changed solution.
The required task has been completed, but it is estimated that a small change in atol and rtol is unlikely to produce any change in the computed solution. (Only applies when you are not operating in one step mode, that is when itask2 or 5.)
ifail=11
Error during Jacobian formulation for ODE system. Increase itrace for further details.
ifail=12
In solving ODE system, the maximum number of steps algopt15 has been exceeded. algopt15=value.
ifail=13
Zero error weights encountered during time integration.
Some error weights wi became zero during the time integration (see the description of itol). Pure relative error control atoli=0.0 was requested on a variable (the ith) which has become zero. The integration was successful as far as t=ts.
ifail=15
When using the sparse option lisave or lrsave is too small: lisave=value, lrsave=value.
ifail=-99
An unexpected error has been triggered by this routine. Please contact NAG.
See Section 7 in the Introduction to the NAG Library FL Interface for further information.
ifail=-399
Your licence key may have expired or may not have been installed correctly.
See Section 8 in the Introduction to the NAG Library FL Interface for further information.
ifail=-999
Dynamic memory allocation failed.
See Section 9 in the Introduction to the NAG Library FL Interface for further information.

7 Accuracy

d03pkf controls the accuracy of the integration in the time direction but not the accuracy of the approximation in space. The spatial accuracy depends on both the number of mesh points and on their distribution in space. In the time integration only the local error over a single step is controlled and so the accuracy over a number of steps cannot be guaranteed. You should therefore test the effect of varying the accuracy arguments, atol and rtol.

8 Parallelism and Performance

d03pkf is not thread safe and should not be called from a multithreaded user program. Please see Section 1 in FL Interface Multithreading for more information on thread safety.
d03pkf is threaded by NAG for parallel execution in multithreaded implementations of the NAG Library.
d03pkf makes calls to BLAS and/or LAPACK routines, which may be threaded within the vendor library used by this implementation. Consult the documentation for the vendor library for further information.
Please consult the X06 Chapter Introduction for information on how to control and interrogate the OpenMP environment used within this routine. Please also consult the Users' Note for your implementation for any additional implementation-specific information.

9 Further Comments

The Keller box scheme can be used to solve higher-order problems which have been reduced to first-order by the introduction of new variables (see the example in Section 10). In general, a second-order problem can be solved with slightly greater accuracy using the Keller box scheme instead of a finite difference scheme (see d03pcf/​d03pca or d03phf/​d03pha for example), but at the expense of increased CPU time due to the larger number of function evaluations required.
It should be noted that the Keller box scheme, in common with other central-difference schemes, may be unsuitable for some hyperbolic first-order problems such as the apparently simple linear advection equation Ut+aUx=0, where a is a constant, resulting in spurious oscillations due to the lack of dissipation. This type of problem requires a discretization scheme with upwind weighting (d03plf for example), or the addition of a second-order artificial dissipation term.
The time taken depends on the complexity of the system and on the accuracy requested. For a given system and a fixed accuracy it is approximately proportional to neqn.

10 Example

This example provides a simple coupled system of two PDEs and one ODE.
V1 2 U1 t -xV1V.1U2- U2 x =0, U2- U1 x =0, V.1-V1U1-U2-1-t=0,  
for t10-4,0.1×2i, for i=1,2,,5,x0,1. The left boundary condition at x=0 is
U2=-V1expt,  
and the right boundary condition at x=1 is
U2=-V1V.1.  
The initial conditions at t=10-4 are defined by the exact solution:
V1 = t , U1 x,t = exp t 1-x - 1.0   and   U2 x,t = - t exp t 1-x , ​ x 0,1 ,  
and the coupling point is at ξ1=1.0.
This problem is exactly the same as the d03phf/​d03pha example problem, but reduced to first-order by the introduction of a second PDE variable (as mentioned in Section 9).

10.1 Program Text

Program Text (d03pkfe.f90)

10.2 Program Data

Program Data (d03pkfe.d)

10.3 Program Results

Program Results (d03pkfe.r)
GnuplotProduced by GNUPLOT 5.0 patchlevel 0 Example Program Two PDEs Coupled with One ODE using Keller, Box and BDF Solution U(1,x,t) U(1,x,t) gnuplot_plot_1 gnuplot_plot_2 0.1 0.5 1 2 3 Time (logscale) 0 0.2 0.4 0.6 0.8 1 x −5 0 5 10 15 20 25
GnuplotProduced by GNUPLOT 5.0 patchlevel 0 Two PDEs Coupled with One ODE using Keller, Box and BDF Solution U(2,x,t) U(2,x,t) gnuplot_plot_1 gnuplot_plot_2 0.1 0.5 1 2 3 Time (logscale) 0 0.2 0.4 0.6 0.8 1 x −80 −70 −60 −50 −40 −30 −20 −10 0