hide long namesshow long names
hide short namesshow short names
Integer type:  int32  int64  nag_int  show int32  show int32  show int64  show int64  show nag_int  show nag_int

PDF version (NAG web site, 64-bit version, 64-bit version)
Chapter Contents
Chapter Introduction
NAG Toolbox

NAG Toolbox: nag_specfun_airy_bi_deriv_vector (s17ax)

 Contents

    1  Purpose
    2  Syntax
    7  Accuracy
    9  Example

Purpose

nag_specfun_airy_bi_deriv_vector (s17ax) returns an array of values for the derivative of the Airy function Bix.

Syntax

[f, ivalid, ifail] = s17ax(x, 'n', n)
[f, ivalid, ifail] = nag_specfun_airy_bi_deriv_vector(x, 'n', n)

Description

nag_specfun_airy_bi_deriv_vector (s17ax) calculates an approximate value for the derivative of the Airy function Bixi for an array of arguments xi, for i=1,2,,n. It is based on a number of Chebyshev expansions.
For x<-5,
Bix=-x4 -atsinz+btζcosz ,  
where z= π4+ζ, ζ= 23-x3 and at and bt are expansions in the variable t=-2 5x 3-1.
For -5x0,
Bix=3x2ft+gt,  
where f and g are expansions in t=-2 x5 3-1.
For 0<x<4.5,
Bix=e3x/2yt,  
where yt is an expansion in t=4x/9-1.
For 4.5x<9,
Bix=e21x/8ut,  
where ut is an expansion in t=4x/9-3.
For x9,
Bix=x4ezvt,  
where z= 23x3 and vt is an expansion in t=2 18z-1.
For x< the square of the machine precision, the result is set directly to Bi0. This saves time and avoids possible underflows in calculation.
For large negative arguments, it becomes impossible to calculate a result for the oscillating function with any accuracy so the function must fail. This occurs for x<- πε 4/7 , where ε is the machine precision.
For large positive arguments, where Bi grows in an essentially exponential manner, there is a danger of overflow so the function must fail.

References

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

Parameters

Compulsory Input Parameters

1:     xn – double array
The argument xi of the function, for i=1,2,,n.

Optional Input Parameters

1:     n int64int32nag_int scalar
Default: the dimension of the array x.
n, the number of points.
Constraint: n0.

Output Parameters

1:     fn – double array
Bixi, the function values.
2:     ivalidn int64int32nag_int array
ivalidi contains the error code for xi, for i=1,2,,n.
ivalidi=0
No error.
ivalidi=1
xi is too large and positive. fi contains zero. The threshold value is the same as for ifail=1 in nag_specfun_airy_bi_deriv (s17ak), as defined in the Users' Note for your implementation.
ivalidi=2
xi is too large and negative. fi contains zero. The threshold value is the same as for ifail=2 in nag_specfun_airy_bi_deriv (s17ak), as defined in the Users' Note for your implementation.
3:     ifail int64int32nag_int scalar
ifail=0 unless the function detects an error (see Error Indicators and Warnings).

Error Indicators and Warnings

Errors or warnings detected by the function:

Cases prefixed with W are classified as warnings and do not generate an error of type NAG:error_n. See nag_issue_warnings.

W  ifail=1
On entry, at least one value of x was invalid.
Check ivalid for more information.
   ifail=2
Constraint: n0.
   ifail=-99
An unexpected error has been triggered by this routine. Please contact NAG.
   ifail=-399
Your licence key may have expired or may not have been installed correctly.
   ifail=-999
Dynamic memory allocation failed.

Accuracy

For negative arguments the function is oscillatory and hence absolute error is appropriate. In the positive region the function has essentially exponential behaviour and hence relative error is needed. The absolute error, E, and the relative error ε, are related in principle to the relative error in the argument δ, by
E x2 Bix δ ε x2 Bix Bix δ.  
In practice, approximate equality is the best that can be expected. When δ, ε or E is of the order of the machine precision, the errors in the result will be somewhat larger.
For small x, positive or negative, errors are strongly attenuated by the function and hence will effectively be bounded by the machine precision.
For moderate to large negative x, the error is, like the function, oscillatory. However, the amplitude of the absolute error grows like x7/4π . Therefore it becomes impossible to calculate the function with any accuracy if x7/4> πδ .
For large positive x, the relative error amplification is considerable: εδx3. However, very large arguments are not possible due to the danger of overflow. Thus in practice the actual amplification that occurs is limited.

Further Comments

None.

Example

This example reads values of x from a file, evaluates the function at each value of xi and prints the results.
function s17ax_example


fprintf('s17ax example results\n\n');

x = [-10; -1; 0; 1; 5; 10; 20];

[f, ivalid, ifail] = s17ax(x);

fprintf('     x           Bi''(x)   ivalid\n');
for i=1:numel(x)
  fprintf('%12.3e%12.3e%5d\n', x(i), f(i), ivalid(i));
end


s17ax example results

     x           Bi'(x)   ivalid
  -1.000e+01   1.194e-01    0
  -1.000e+00   5.924e-01    0
   0.000e+00   4.483e-01    0
   1.000e+00   9.324e-01    0
   5.000e+00   1.436e+03    0
   1.000e+01   1.429e+09    0
   2.000e+01   9.382e+25    0

PDF version (NAG web site, 64-bit version, 64-bit version)
Chapter Contents
Chapter Introduction
NAG Toolbox

© The Numerical Algorithms Group Ltd, Oxford, UK. 2009–2015