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NAG Toolbox: nag_specfun_kelvin_ker (s19ac)
Purpose
nag_specfun_kelvin_ker (s19ac) returns a value for the Kelvin function , via the function name.
Syntax
Description
nag_specfun_kelvin_ker (s19ac) evaluates an approximation to the Kelvin function .
Note: for the function is undefined and at it is infinite so we need only consider .
The function is based on several Chebyshev expansions:
For
,
where
,
and
are expansions in the variable
.
For
,
where
is an expansion in the variable
.
For
,
where
, and
and
are expansions in the variable
.
When
is sufficiently close to zero, the result is computed as
and when
is even closer to zero, simply as
.
For large , is asymptotically given by and this becomes so small that it cannot be computed without underflow and the function fails.
References
Abramowitz M and Stegun I A (1972) Handbook of Mathematical Functions (3rd Edition) Dover Publications
Parameters
Compulsory Input Parameters
- 1:
– double scalar
-
The argument of the function.
Constraint:
.
Optional Input Parameters
None.
Output Parameters
- 1:
– double scalar
The result of the function.
- 2:
– int64int32nag_int scalar
unless the function detects an error (see
Error Indicators and Warnings).
Error Indicators and Warnings
Errors or warnings detected by the function:
-
-
On entry,
x is too large: the result underflows. On soft failure, the function returns zero.
-
-
On entry, : the function is undefined. On soft failure the function returns zero.
-
An unexpected error has been triggered by this routine. Please
contact
NAG.
-
Your licence key may have expired or may not have been installed correctly.
-
Dynamic memory allocation failed.
Accuracy
Let
be the absolute error in the result,
be the relative error in the result and
be the relative error in the argument. If
is somewhat larger than the
machine precision, then we have:
For very small
, the relative error amplification factor is approximately given by
, which implies a strong attenuation of relative error. However,
in general cannot be less than the
machine precision.
For small
, errors are damped by the function and hence are limited by the
machine precision.
For medium and large , the error behaviour, like the function itself, is oscillatory, and hence only the absolute accuracy for the function can be maintained. For this range of , the amplitude of the absolute error decays like which implies a strong attenuation of error. Eventually, , which asymptotically behaves like , becomes so small that it cannot be calculated without causing underflow, and the function returns zero. Note that for large the errors are dominated by those of the standard function exp.
Further Comments
Underflow may occur for a few values of close to the zeros of , below the limit which causes a failure with .
Example
This example reads values of the argument from a file, evaluates the function at each value of and prints the results.
Open in the MATLAB editor:
s19ac_example
function s19ac_example
fprintf('s19ac example results\n\n');
x = [0.1 1 2.5 5 10 15];
n = size(x,2);
result = x;
for j=1:n
[result(j), ifail] = s19ac(x(j));
end
disp(' x ker(x)');
fprintf('%12.3e%12.3e\n',[x; result]);
s19ac example results
x ker(x)
1.000e-01 2.420e+00
1.000e+00 2.867e-01
2.500e+00 -6.969e-02
5.000e+00 -1.151e-02
1.000e+01 1.295e-04
1.500e+01 -1.514e-08
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