c06laf estimates values of the inverse Laplace transform of a given function using a Fourier series approximation. Real and imaginary parts of the function, and a bound on the exponential order of the inverse, are required.

2

Specification

Fortran Interface

Subroutine c06laf (

fun, n, t, valinv, errest, relerr, alphab, tfac, mxterm, nterms, na, alow, ahigh, nfeval, work, ifail)

Integer, Intent (In)	::	n, mxterm
Integer, Intent (Inout)	::	ifail
Integer, Intent (Out)	::	nterms, na, nfeval
Real (Kind=nag_wp), Intent (In)	::	t(n), relerr, alphab, tfac
Real (Kind=nag_wp), Intent (Out)	::	valinv(n), errest(n), alow, ahigh, work(4*mxterm+2)
External	::	fun

C Header Interface

#include nagmk26.h

void

c06laf_ (
void (NAG_CALL *fun)( const double *pr, const double *pi, double *fr, double *fi),
const Integer *n, const double t[], double valinv[], double errest[], const double *relerr, const double *alphab, const double *tfac, const Integer *mxterm, Integer *nterms, Integer *na, double *alow, double *ahigh, Integer *nfeval, double work[], Integer *ifail)

3

Description

Given a function

F (p)

defined for complex values of

p

, c06laf estimates values of its inverse Laplace transform by Crump's method (see Crump (1976)). (For a definition of the Laplace transform and its inverse, see the C06 Chapter Introduction.)

Crump's method applies the epsilon algorithm (see Wynn (1956)) to the summation in Durbin's Fourier series approximation (see Durbin (1974))

f (t_{j}) ≃ \frac{e^{a t_{j}}}{τ} [\frac{1}{2} F (a) - \sum_{k = 1}^{\infty} \{Re (F (a + \frac{k π i}{τ})) \cos \frac{k π t_{j}}{τ} - Im (F (a + \frac{k π i}{τ})) \sin \frac{k π t_{j}}{τ}\}],

for

j = 1, 2, \dots, n

, by choosing

a

such that a prescribed relative error should be achieved. The method is modified slightly if

t = 0.0

so that an estimate of

f (0.0)

can be obtained when it has a finite value.

τ

is calculated as

t_{fac} \times \max (0.01, t_{j})

, where

t_{fac} > 0.5

. You specify

t_{fac}

and

α_{b}

, an upper bound on the exponential order

α

of the inverse function

f (t)

α

has two alternative interpretations:

(i)

α

is the smallest number such that

|f (t)| \leq m \times \exp (α t)

for large

t

(ii)

α

is the real part of the singularity of

F (p)

with largest real part.

The method depends critically on the value of

α

. See Section 9 for further details. The routine calculates at least two different values of the argument

a

, such that

a > α_{b}

, in an attempt to achieve the requested relative error and provide error estimates. The values of

t_{j}

, for

j = 1, 2, \dots, n

, must be supplied in monotonically increasing order. The routine calculates the values of the inverse function

f (t_{j})

in decreasing order of

j

4

References

Crump K S (1976) Numerical inversion of Laplace transforms using a Fourier series approximation J. Assoc. Comput. Mach. 23 89–96

Durbin F (1974) Numerical inversion of Laplace transforms: An efficient improvement to Dubner and Abate's method Comput. J. 17 371–376

Wynn P (1956) On a device for computing the

e_{m} (S_{n})

transformation Math. Tables Aids Comput. 10 91–96

5

Arguments

1: $fun$ – Subroutine, supplied by the user.External Procedure

fun must evaluate the real and imaginary parts of the function

F (p)

for a given value of

p

The specification of fun is:

Fortran Interface

Subroutine fun (

pr, pi, fr, fi)

Real (Kind=nag_wp), Intent (In)	::	pr, pi
Real (Kind=nag_wp), Intent (Out)	::	fr, fi

C Header Interface

#include nagmk26.h

void	fun ( const double pr, const double pi, double fr, double fi)

1: $pr$ – Real (Kind=nag_wp)Input
2: $pi$ – Real (Kind=nag_wp)Input: On entry: the real and imaginary parts of the argument $p$ .
3: $fr$ – Real (Kind=nag_wp)Output
4: $fi$ – Real (Kind=nag_wp)Output: On exit: the real and imaginary parts of the value $F (p)$ .

fun must either be a module subprogram USEd by, or declared as EXTERNAL in, the (sub)program from which c06laf is called. Arguments denoted as Input must not be changed by this procedure.

Note: fun should not return floating-point NaN (Not a Number) or infinity values, since these are not handled by c06laf. If your code inadvertently does return any NaNs or infinities, c06laf is likely to produce unexpected results.

2: $n$ – IntegerInput

On entry:

n

, the number of points at which the value of the inverse Laplace transform is required.

Constraint:

n \geq 1

3: $t (n)$ – Real (Kind=nag_wp) arrayInput

On entry: each

t (j)

must specify a point at which the inverse Laplace transform is required, for

j = 1, 2, \dots, n

Constraint:

0.0 \leq t (1) < t (2) < \dots < t (n)

4: $valinv (n)$ – Real (Kind=nag_wp) arrayOutput

On exit: an estimate of the value of the inverse Laplace transform at

t = t (j)

, for

j = 1, 2, \dots, n

5: $errest (n)$ – Real (Kind=nag_wp) arrayOutput

On exit: an estimate of the error in

valinv (j)

. This is usually an estimate of relative error but, if

valinv (j) < relerr

errest (j)

estimates the absolute error.

errest (j)

is unreliable when

valinv (j)

is small but slightly greater than relerr.

6: $relerr$ – Real (Kind=nag_wp)Input

On entry: the required relative error in the values of the inverse Laplace transform. If the absolute value of the inverse is less than relerr, absolute accuracy is used instead. relerr must be in the range

0.0 \leq relerr < 1.0

. If relerr is set too small or to

0.0

, the routine uses a value sufficiently larger than machine precision.

7: $alphab$ – Real (Kind=nag_wp)Input

On entry:

α_{b}

, an upper bound for

α

(see Section 3). Usually,

α_{b}

should be specified equal to, or slightly larger than, the value of

α

. If

α_{b} < α

then the prescribed accuracy may not be achieved or completely incorrect results may be obtained. If

α_{b}

is too large c06laf will be inefficient and convergence may not be achieved.

Note: it is as important to specify

α_{b}

correctly as it is to specify the correct function for inversion.

8: $tfac$ – Real (Kind=nag_wp)Input

On entry:

t_{fac}

, a factor to be used in calculating the parameter

τ

. Larger values (e.g.,

5.0

) may be specified for difficult problems, but these may require very large values of mxterm.

Suggested value:

tfac = 0.8

Constraint:

tfac > 0.5

9: $mxterm$ – IntegerInput

On entry: the maximum number of (complex) terms to be used in the evaluation of the Fourier series.

Suggested value:

mxterm \geq 100

, except for very simple problems.

Constraint:

mxterm \geq 1

10: $nterms$ – IntegerOutput

On exit: the number of (complex) terms actually used.

11: $na$ – IntegerOutput

On exit: the number of values of

a

used by the routine. See Section 9.

12: $alow$ – Real (Kind=nag_wp)Output

On exit: the smallest value of

a

used in the algorithm. This may be used for checking the value of

alphab -

see Section 9.

13: $ahigh$ – Real (Kind=nag_wp)Output

On exit: the largest value of

a

used in the algorithm. This may be used for checking the value of

alphab -

see Section 9.

14: $nfeval$ – IntegerOutput

On exit: the number of calls to fun made by the routine.

15: $work (4 \times mxterm + 2)$ – Real (Kind=nag_wp) arrayWorkspace

16: $ifail$ – IntegerInput/Output

On entry: ifail must be set to

0

- 1 ​ or ​ 1

. If you are unfamiliar with this argument you should refer to Section 3.4 in How to Use the NAG Library and its Documentation 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 arguments may be useful even if

ifail \neq 0

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 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

- 1

, explanatory error messages are output on the current error message unit (as defined by x04aaf).

Note: c06laf may return useful information for one or more of the following detected errors or warnings.

Errors or warnings detected by the routine:

$ifail = 1$

On entry,	$n < 1$ ,
or	$mxterm < 1$ ,
or	$relerr < 0.0$ ,
or	$relerr \geq 1.0$ ,
or	$tfac \leq 0.5$ .

$ifail = 2$

On entry,	$t (1) < 0.0$ ,
or	$t (1), t (2), \dots, t (n)$ are not in strictly increasing order.

$ifail = 3$: $t (n)$ is too large for this value of alphab. If necessary, scale the problem as described in Section 9.

$ifail = 4$: The required accuracy cannot be obtained. It is possible that alphab is less than $α$ . Alternatively, the problem may be especially difficult. Try increasing tfac, alphab or both.

$ifail = 5$: Convergence failure in the epsilon algorithm. Some values of $valinv (j)$ may be calculated to the desired accuracy; this may be determined by examining the values of $errest (j)$ . Try reducing the range of t or increasing mxterm. If $ifail = 5$ still results, try reducing tfac.

$ifail = 6$: All values of $valinv (j)$ have been calculated but not all are to the requested accuracy; the values of $errest (j)$ should be examined carefully. Try reducing the range of $t$ , or increasing tfac, alphab or both.

$ifail = - 99$: An unexpected error has been triggered by this routine. Please contact NAG.
See Section 3.9 in How to Use the NAG Library and its Documentation for further information.

$ifail = - 399$: Your licence key may have expired or may not have been installed correctly.
See Section 3.8 in How to Use the NAG Library and its Documentation for further information.

$ifail = - 999$: Dynamic memory allocation failed.
See Section 3.7 in How to Use the NAG Library and its Documentation for further information.

7

Accuracy

The error estimates are often very close to the true error but, because the error control depends on an asymptotic formula, the required error may not always be met. There are two principal causes of this: Gibbs' phenomena, and zero or small values of the inverse Laplace transform.

Gibbs' phenomena (see the C06 Chapter Introduction) are exhibited near

t = 0.0

(due to the method) and around discontinuities in the inverse Laplace transform

f (t)

. If there is a discontinuity at

t = c

then the method converges such that

f (c) \to (f (c -) + f (c +)) / 2

Apparent loss of accuracy, when

f (t)

is small, may not be serious. Crump's method keeps control of relative error so that good approximations to small function values may appear to be very inaccurate. If

|f (t)|

is estimated to be less than relerr then this routine switches to absolute error estimation. However, when

|f (t)|

is slightly larger than relerr the relative error estimates are likely to cause

ifail = 6

. If this is found inconvenient it can sometimes be avoided by adding

k / p

to the function

F (p)

, which shifts the inverse to

k + f (t)

Loss of accuracy may also occur for highly oscillatory functions.

More serious loss of accuracy can occur if

α

is unknown and is incorrectly estimated. See Section 9.

8

Parallelism and Performance

c06laf is not threaded in any implementation.

9

Further Comments

9.1

Timing

The value of

n

is less important in general than the value of nterms. Unless fun is very inexpensive to compute, the timing is proportional to

na \times nterms

. For simple problems

na = 2

but in difficult problems na may be somewhat larger.

9.2

Precautions

You are referred to the C06 Chapter Introduction for advice on simplifying problems with particular difficulties, e.g., where the inverse is known to be a step function.

The method does not work well for large values of

t

when

α

is positive. It is advisable, especially if

ifail = 3

is obtained, to scale the problem if

|α|

is much greater than

1.0

. See the C06 Chapter Introduction.

The range of values of

t

specified for a particular call should not be greater than about

10

units. This is because the method uses arguments based on the value

t (n)

and these tend to be less appropriate as

t

becomes smaller. However, as the timing of the routine is not especially dependent on

n

, it is usually far more efficient to evaluate the inverse for ranges of

t

than to make separate calls to the routine for each value of

t

The most important argument to specify correctly is alphab, an upper bound for

α

. If, on entry, alphab is sufficiently smaller than

α

then completely incorrect results will be obtained with

ifail = 0

. Unless

α

is known theoretically it is strongly advised that you should test any estimated value used. This may be done by specifying a single value of

t

(i.e

t (n)

n = 1

) with two sets of suitable values of tfac, relerr and mxterm, and examining the resulting values of alow and ahigh. The value of

t (1)

should be chosen very carefully and the following points should be borne in mind:

(i)

t (1)

should be small but not too close to

0.0

because of Gibbs' phenomenon (see Section 7),

(ii)

the larger the value of

t (1)

, the smaller the range of values of

a

that will be used in the algorithm,

(iii)

t (1)

should ideally not be chosen such that

f (t (1)) = 0.0

or a very small value. For suitable problems

t (1)

might be chosen as, say,

0.1

1.0

depending on these factors. The routine calculates alow from the formula

alow = alphab - \frac{\ln (0.1 \times relerr)}{2 \times τ} .

Additional values of

a

are computed by adding

1 / τ

to the previous value. As

τ = tfac \times t (n)

, it will be seen that large values of tfac and relerr will test for

a

close to alphab. Small values of tfac and relerr will test for

a

large. If the result of both tests is

ifail = 0

, with comparable values for the inverse, then this gives some credibility to the chosen value of alphab. You should note that this test could be more computationally expensive than the calculation of the inverse itself. The example program (see Section 10) illustrates how such a test may be performed.

10

Example

This example estimates the inverse Laplace transform of the function

F (p) = 1 / (p + 1 / 2)

. The true inverse of

F (p)

\exp (- t / 2)

. Two preliminary calls to the routine are made to verify that the chosen value of alphab is suitable. For these tests the single value

t (1) = 1.0

is used. To test values of

a

close to alphab, the values

tfac = 5.0

and

relerr = 0.01

are chosen. To test larger

a

, the values

tfac = 0.8

and

relerr = 1.0E−3

are used. Because the values of the computed inverse are similar and

ifail = 0

in each case, these tests show that there is unlikely to be a singularity of

F (p)

in the region

- 0.04 \leq Re (p) \leq 6.51

NAG Library Routine Document

c06laf (invlaplace_crump)

▸▿ Contents

1 Purpose

2 Specification

3 Description

4 References

5 Arguments

6 Error Indicators and Warnings

7 Accuracy

8 Parallelism and Performance

9 Further Comments

9.1 Timing

9.2 Precautions

10 Example

10.1 Program Text

10.2 Program Data

10.3 Program Results

1

Purpose

2

Specification

3

Description

4

References

5

Arguments

6

Error Indicators and Warnings

7

Accuracy

8

Parallelism and Performance

9

Further Comments

9.1

Timing

9.2

Precautions

10

Example

10.1

Program Text

10.2

Program Data

10.3

Program Results