NAG Library Routine Document

S17AVF

+− Contents

1 Purpose

2 Specification

3 Description

4 References

5 Parameters

6 Error Indicators and Warnings

7 Accuracy

8 Further Comments

+− 9 Example

9.1 Program Text

9.2 Program Data

9.3 Program Results

1 Purpose

S17AVF returns an array of values of the Airy function,

Bi (x)

2 Specification

SUBROUTINE S17AVF (

N, X, F, IVALID, IFAIL)

INTEGER	N, IVALID(N), IFAIL
REAL (KIND=nag_wp)	X(N), F(N)

3 Description

S17AVF evaluates an approximation to the Airy function

Bi (x_{i})

for an array of arguments

x_{i}

, for

i = 1, 2, \dots, n

. It is based on a number of Chebyshev expansions.

For

x < - 5

Bi (x) = \frac{a (t) \cos z + b (t) \sin z}{{(- x)}^{1 / 4}},

where

z = \frac{π}{4} + \frac{2}{3} \sqrt{- x^{3}}

and

a (t)

and

b (t)

are expansions in the variable

t = - 2 {(\frac{5}{x})}^{3} - 1

For

- 5 \leq x \leq 0

Bi (x) = \sqrt{3} (f (t) + x g (t)),

where

f

and

g

are expansions in

t = - 2 {(\frac{x}{5})}^{3} - 1

For

0 < x < 4.5

Bi (x) = e^{11 x / 8} y (t),

where

y

is an expansion in

t = 4 x / 9 - 1

For

4.5 \leq x < 9

Bi (x) = e^{5 x / 2} v (t),

where

v

is an expansion in

t = 4 x / 9 - 3

For

x \geq 9

Bi (x) = \frac{e^{z} u (t)}{x^{1 / 4}},

where

z = \frac{2}{3} \sqrt{x^{3}}

and

u

is an expansion in

t = 2 (\frac{18}{z}) - 1

For

|x| < machine precision

, the result is set directly to

Bi (0)

. This both saves time and avoids possible intermediate underflows.

For large negative arguments, it becomes impossible to calculate the phase of the oscillating function with any accuracy so the routine must fail. This occurs if

x < - {(\frac{3}{2 ε})}^{2 / 3}

, where

ε

is the machine precision.

For large positive arguments, there is a danger of causing overflow since Bi grows in an essentially exponential manner, so the routine must fail.

4 References

Abramowitz M and Stegun I A (1972) Handbook of Mathematical Functions (3rd Edition) Dover Publications

5 Parameters

1: N – INTEGERInput

On entry:

n

, the number of points.

Constraint:

N \geq 0

2: X(N) – REAL (KIND=nag_wp) arrayInput

On entry: the argument

x_{i}

of the function, for

i = 1, 2, \dots, N

3: F(N) – REAL (KIND=nag_wp) arrayOutput

On exit:

Bi (x_{i})

, the function values.

4: IVALID(N) – INTEGER arrayOutput

On exit:

IVALID (i)

contains the error code for

x_{i}

, for

i = 1, 2, \dots, N

$IVALID (i) = 0$: No error.
$IVALID (i) = 1$: $x_{i}$ is too large and positive. $F (i)$ contains zero. The threshold value is the same as for $IFAIL = 1$ in S17AHF, as defined in the Users' Note for your implementation.
$IVALID (i) = 2$: $x_{i}$ is too large and negative. $F (i)$ contains zero. The threshold value is the same as for $IFAIL = 2$ in S17AHF, as defined in the Users' Note for your implementation.

5: IFAIL – INTEGERInput/Output

On 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, if you are not familiar with this parameter, 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

- 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 value of X was invalid.
Check IVALID for more information.

$IFAIL = 2$: On entry, $N = ⟨value⟩$ .
Constraint: $N \geq 0$ .

7 Accuracy

For negative arguments the function is oscillatory and hence absolute error is the appropriate measure. In the positive region the function is essentially exponential-like and here relative error is appropriate. The absolute error,

E

, and the relative error,

ε

, are related in principle to the relative error in the argument,

δ

, by

E ≃ |x {Bi}^{'} (x)| δ, ε ≃ |\frac{x {Bi}^{'} (x)}{Bi (x)}| δ .

In practice, approximate equality is the best that can be expected. When

δ

ε

E

is of the order of the machine precision, the errors in the result will be somewhat larger.

For small

x

, errors are strongly damped and hence will be bounded essentially by the machine precision.

For moderate to large negative

x

, the error behaviour is clearly oscillatory but the amplitude of the error grows like amplitude

(\frac{E}{δ}) \sim \frac{{|x|}^{5 / 4}}{\sqrt{π}}

However the phase error will be growing roughly as

\frac{2}{3} \sqrt{{|x|}^{3}}

and hence all accuracy will be lost for large negative arguments. This is due to the impossibility of calculating sin and cos to any accuracy if

\frac{2}{3} \sqrt{{|x|}^{3}} > \frac{1}{δ}

For large positive arguments, the relative error amplification is considerable:

\frac{ε}{δ} \sim \sqrt{x^{3}} .

This means a loss of roughly two decimal places accuracy for arguments in the region of

20

. However very large arguments are not possible due to the danger of causing overflow and errors are therefore limited in practice.

8 Further Comments

None.

9 Example

This example reads values of X from a file, evaluates the function at each value of

x_{i}

and prints the results.

NAG Library Routine DocumentS17AVF

+− Contents

1 Purpose

2 Specification

3 Description

4 References

5 Parameters

6 Error Indicators and Warnings

7 Accuracy

8 Further Comments

9 Example

9.1 Program Text

9.2 Program Data

9.3 Program Results

NAG Library Routine Document

S17AVF