§10.67 Asymptotic Expansions for Large Argument

Define $a_k(\nu )$ and $b_k(\nu )$ as in §§10.17(i) and 10.17(ii). Then as $x\to \mathrm{\infty }$ with $\nu$ fixed,

10.67.1		${\ker }_{\nu }x$	$\sim {\mathrm{e}}^{-x/\sqrt{2}}{\left({\displaystyle \frac{\pi }{2x}}\right)}^{\frac{1}{2}}{\displaystyle \sum _{k=0}^{\mathrm{\infty }}}{\displaystyle \frac{a_k(\nu )}{x^k}}\cos \left({\displaystyle \frac{x}{\sqrt{2}}}+\left({\displaystyle \frac{\nu }{2}}+{\displaystyle \frac{k}{4}}+{\displaystyle \frac{1}{8}}\right)\pi \right),$
ⓘ Symbols: ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\cos z$: cosine function, $\mathrm{e}$: base of natural logarithm, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $a_k(\nu )$: polynomial coefficient A&S Ref: 9.10.3, 9.10.5--9.10.7 (modified) Referenced by: §10.61(v), §10.67(ii), §10.68(iii) Permalink: http://dlmf.nist.gov/10.67.E1 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10
10.67.2		${\mathrm{kei}}_{\nu }x$	$\sim -{\mathrm{e}}^{-x/\sqrt{2}}{\left({\displaystyle \frac{\pi }{2x}}\right)}^{\frac{1}{2}}{\displaystyle \sum _{k=0}^{\mathrm{\infty }}}{\displaystyle \frac{a_k(\nu )}{x^k}}\sin \left({\displaystyle \frac{x}{\sqrt{2}}}+\left({\displaystyle \frac{\nu }{2}}+{\displaystyle \frac{k}{4}}+{\displaystyle \frac{1}{8}}\right)\pi \right).$
ⓘ Symbols: ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm, $\sin z$: sine function, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $a_k(\nu )$: polynomial coefficient A&S Ref: 9.10.4, 9.10.5--9.10.7 (modified) Referenced by: §10.61(v) Permalink: http://dlmf.nist.gov/10.67.E2 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10

10.67.3		$${\mathrm{ber}}_{\nu }x\sim \begin{array}{l}\frac{{\mathrm{e}}^{x/\sqrt{2}}}{{(2\pi x)}^{\frac{1}{2}}}\sum _{k=0}^{\mathrm{\infty }}\frac{a_k(\nu )}{x^k}\cos \left(\frac{x}{\sqrt{2}}+\left(\frac{\nu }{2}+\frac{3k}{4}-\frac{1}{8}\right)\pi \right)\\ -\frac{1}{\pi }(\sin \left(2\nu \pi \right){\ker }_{\nu }x+\cos \left(2\nu \pi \right){\mathrm{kei}}_{\nu }x),\end{array}$$
ⓘ Symbols: ${\mathrm{ber}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\cos z$: cosine function, $\mathrm{e}$: base of natural logarithm, $\sin z$: sine function, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $a_k(\nu )$: polynomial coefficient A&S Ref: 9.10.1, 9.10.5--9.10.7 (modified) Referenced by: §10.61(v), §10.67(i), §10.67(i), §10.68(iii), §10.69 Permalink: http://dlmf.nist.gov/10.67.E3 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10

10.67.4		$${\mathrm{bei}}_{\nu }x\sim \begin{array}{l}\frac{{\mathrm{e}}^{x/\sqrt{2}}}{{(2\pi x)}^{\frac{1}{2}}}\sum _{k=0}^{\mathrm{\infty }}\frac{a_k(\nu )}{x^k}\sin \left(\frac{x}{\sqrt{2}}+\left(\frac{\nu }{2}+\frac{3k}{4}-\frac{1}{8}\right)\pi \right)\\ +\frac{1}{\pi }(\cos \left(2\nu \pi \right){\ker }_{\nu }x-\sin \left(2\nu \pi \right){\mathrm{kei}}_{\nu }x).\end{array}$$
ⓘ Symbols: ${\mathrm{bei}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\cos z$: cosine function, $\mathrm{e}$: base of natural logarithm, $\sin z$: sine function, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $a_k(\nu )$: polynomial coefficient A&S Ref: 9.10.2, 9.10.5--9.10.7 (modified) Referenced by: §10.61(v), §10.67(i), §10.67(i), §10.67(ii), §10.68(iii), §10.69 Permalink: http://dlmf.nist.gov/10.67.E4 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10

10.67.5		${\ker }_{\nu }^{\prime }x$	$\sim -{\mathrm{e}}^{-x/\sqrt{2}}{\left({\displaystyle \frac{\pi }{2x}}\right)}^{\frac{1}{2}}{\displaystyle \sum _{k=0}^{\mathrm{\infty }}}{\displaystyle \frac{b_k(\nu )}{x^k}}\cos \left({\displaystyle \frac{x}{\sqrt{2}}}+\left({\displaystyle \frac{\nu }{2}}+{\displaystyle \frac{k}{4}}-{\displaystyle \frac{1}{8}}\right)\pi \right),$
ⓘ Symbols: ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\cos z$: cosine function, $\mathrm{e}$: base of natural logarithm, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $b_k(\nu )$: polynomial coefficient A&S Ref: §9.10 (modified) Permalink: http://dlmf.nist.gov/10.67.E5 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10
10.67.6		${\mathrm{kei}}_{\nu }^{\prime }x$	$\sim {\mathrm{e}}^{-x/\sqrt{2}}{\left({\displaystyle \frac{\pi }{2x}}\right)}^{\frac{1}{2}}{\displaystyle \sum _{k=0}^{\mathrm{\infty }}}{\displaystyle \frac{b_k(\nu )}{x^k}}\sin \left({\displaystyle \frac{x}{\sqrt{2}}}+\left({\displaystyle \frac{\nu }{2}}+{\displaystyle \frac{k}{4}}-{\displaystyle \frac{1}{8}}\right)\pi \right).$
ⓘ Symbols: ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm, $\sin z$: sine function, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $b_k(\nu )$: polynomial coefficient A&S Ref: §9.10 (modified) Permalink: http://dlmf.nist.gov/10.67.E6 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10

10.67.7		$${\mathrm{ber}}_{\nu }^{\prime }x\sim \begin{array}{l}\frac{{\mathrm{e}}^{x/\sqrt{2}}}{{(2\pi x)}^{\frac{1}{2}}}\sum _{k=0}^{\mathrm{\infty }}\frac{b_k(\nu )}{x^k}\cos \left(\frac{x}{\sqrt{2}}+\left(\frac{\nu }{2}+\frac{3k}{4}+\frac{1}{8}\right)\pi \right)\\ -\frac{1}{\pi }(\sin \left(2\nu \pi \right){\ker }_{\nu }^{\prime }x+\cos \left(2\nu \pi \right){\mathrm{kei}}_{\nu }^{\prime }x),\end{array}$$
ⓘ Symbols: ${\mathrm{ber}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\cos z$: cosine function, $\mathrm{e}$: base of natural logarithm, $\sin z$: sine function, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $b_k(\nu )$: polynomial coefficient A&S Ref: §9.10 (modified) Referenced by: §10.67(i), §10.67(i), §10.69 Permalink: http://dlmf.nist.gov/10.67.E7 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10

10.67.8		$${\mathrm{bei}}_{\nu }^{\prime }x\sim \begin{array}{l}\frac{{\mathrm{e}}^{x/\sqrt{2}}}{{(2\pi x)}^{\frac{1}{2}}}\sum _{k=0}^{\mathrm{\infty }}\frac{b_k(\nu )}{x^k}\sin \left(\frac{x}{\sqrt{2}}+\left(\frac{\nu }{2}+\frac{3k}{4}+\frac{1}{8}\right)\pi \right)\\ +\frac{1}{\pi }(\cos \left(2\nu \pi \right){\ker }_{\nu }^{\prime }x-\sin \left(2\nu \pi \right){\mathrm{kei}}_{\nu }^{\prime }x).\end{array}$$
ⓘ Symbols: ${\mathrm{bei}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\cos z$: cosine function, $\mathrm{e}$: base of natural logarithm, $\sin z$: sine function, $k$: nonnegative integer, $x$: real variable, $\nu$: complex parameter and $b_k(\nu )$: polynomial coefficient A&S Ref: §9.10 (modified) Referenced by: §10.67(i), §10.67(i), §10.69 Permalink: http://dlmf.nist.gov/10.67.E8 Encodings: TeX, pMML, png See also: Annotations for §10.67(i), §10.67 and Ch.10

The contributions of the terms in ${\ker }_{\nu }x$, ${\mathrm{kei}}_{\nu }x$, ${\ker }_{\nu }^{\prime }x$, and ${\mathrm{kei}}_{\nu }^{\prime }x$ on the right-hand sides of (10.67.3), (10.67.4), (10.67.7), and (10.67.8) are exponentially small compared with the other terms, and hence can be neglected in the sense of Poincaré asymptotic expansions (§2.1(iii)). However, their inclusion improves numerical accuracy.

As $x\to \mathrm{\infty }$

10.67.9		${\mathrm{ber}}^{2}x+{\mathrm{bei}}^{2}x$	$\sim {\displaystyle \frac{{\mathrm{e}}^{x\sqrt{2}}}{2\pi x}}\left(1+{\displaystyle \frac{1}{4\sqrt{2}}}{\displaystyle \frac{1}{x}}+{\displaystyle \frac{1}{64}}{\displaystyle \frac{1}{x^2}}-{\displaystyle \frac{33}{256\sqrt{2}}}{\displaystyle \frac{1}{x^3}}-{\displaystyle \frac{1797}{8192}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right),$
ⓘ Symbols: ${\mathrm{bei}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{ber}}_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.27 Permalink: http://dlmf.nist.gov/10.67.E9 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.10		$\mathrm{ber}x{\mathrm{bei}}^{\prime }x-{\mathrm{ber}}^{\prime }x\mathrm{bei}x$	$\sim {\displaystyle \frac{{\mathrm{e}}^{x\sqrt{2}}}{2\pi x}}\left({\displaystyle \frac{1}{\sqrt{2}}}+{\displaystyle \frac{1}{8}}{\displaystyle \frac{1}{x}}+{\displaystyle \frac{9}{64\sqrt{2}}}{\displaystyle \frac{1}{x^2}}+{\displaystyle \frac{39}{512}}{\displaystyle \frac{1}{x^3}}+{\displaystyle \frac{75}{8192\sqrt{2}}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right),$
ⓘ Symbols: ${\mathrm{bei}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{ber}}_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.28 Permalink: http://dlmf.nist.gov/10.67.E10 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.11		$\mathrm{ber}x{\mathrm{ber}}^{\prime }x+\mathrm{bei}x{\mathrm{bei}}^{\prime }x$	$\sim {\displaystyle \frac{{\mathrm{e}}^{x\sqrt{2}}}{2\pi x}}\left({\displaystyle \frac{1}{\sqrt{2}}}-{\displaystyle \frac{3}{8}}{\displaystyle \frac{1}{x}}-{\displaystyle \frac{15}{64\sqrt{2}}}{\displaystyle \frac{1}{x^2}}-{\displaystyle \frac{45}{512}}{\displaystyle \frac{1}{x^3}}+{\displaystyle \frac{315}{8192\sqrt{2}}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right),$
ⓘ Symbols: ${\mathrm{bei}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{ber}}_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.29 Permalink: http://dlmf.nist.gov/10.67.E11 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.12		${\left({\mathrm{ber}}^{\prime }x\right)}^2+{\left({\mathrm{bei}}^{\prime }x\right)}^2$	$\sim {\displaystyle \frac{{\mathrm{e}}^{x\sqrt{2}}}{2\pi x}}\left(1-{\displaystyle \frac{3}{4\sqrt{2}}}{\displaystyle \frac{1}{x}}+{\displaystyle \frac{9}{64}}{\displaystyle \frac{1}{x^2}}+{\displaystyle \frac{75}{256\sqrt{2}}}{\displaystyle \frac{1}{x^3}}+{\displaystyle \frac{2475}{8192}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right).$
ⓘ Symbols: ${\mathrm{bei}}_{\nu }\left(x\right)$: Kelvin function, ${\mathrm{ber}}_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.30 Permalink: http://dlmf.nist.gov/10.67.E12 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.13		${\ker }^{2}x+{\mathrm{kei}}^{2}x$	$\sim {\displaystyle \frac{\pi }{2x}}{\mathrm{e}}^{-x\sqrt{2}}\left(1-{\displaystyle \frac{1}{4\sqrt{2}}}{\displaystyle \frac{1}{x}}+{\displaystyle \frac{1}{64}}{\displaystyle \frac{1}{x^2}}+{\displaystyle \frac{33}{256\sqrt{2}}}{\displaystyle \frac{1}{x^3}}-{\displaystyle \frac{1797}{8192}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right),$
ⓘ Symbols: ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.31 Permalink: http://dlmf.nist.gov/10.67.E13 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.14		$\ker x{\mathrm{kei}}^{\prime }x-{\ker }^{\prime }x\mathrm{kei}x$	$\sim -{\displaystyle \frac{\pi }{2x}}{\mathrm{e}}^{-x\sqrt{2}}\left({\displaystyle \frac{1}{\sqrt{2}}}-{\displaystyle \frac{1}{8}}{\displaystyle \frac{1}{x}}+{\displaystyle \frac{9}{64\sqrt{2}}}{\displaystyle \frac{1}{x^2}}-{\displaystyle \frac{39}{512}}{\displaystyle \frac{1}{x^3}}+{\displaystyle \frac{75}{8192\sqrt{2}}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right),$
ⓘ Symbols: ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.32 Permalink: http://dlmf.nist.gov/10.67.E14 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.15		$\ker x{\ker }^{\prime }x+\mathrm{kei}x{\mathrm{kei}}^{\prime }x$	$\sim -{\displaystyle \frac{\pi }{2x}}{\mathrm{e}}^{-x\sqrt{2}}\left({\displaystyle \frac{1}{\sqrt{2}}}+{\displaystyle \frac{3}{8}}{\displaystyle \frac{1}{x}}-{\displaystyle \frac{15}{64\sqrt{2}}}{\displaystyle \frac{1}{x^2}}+{\displaystyle \frac{45}{512}}{\displaystyle \frac{1}{x^3}}+{\displaystyle \frac{315}{8192\sqrt{2}}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right),$
ⓘ Symbols: ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.33 Permalink: http://dlmf.nist.gov/10.67.E15 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10
10.67.16		${\left({\ker }^{\prime }x\right)}^2+{\left({\mathrm{kei}}^{\prime }x\right)}^2$	$\sim {\displaystyle \frac{\pi }{2x}}{\mathrm{e}}^{-x\sqrt{2}}\left(1+{\displaystyle \frac{3}{4\sqrt{2}}}{\displaystyle \frac{1}{x}}+{\displaystyle \frac{9}{64}}{\displaystyle \frac{1}{x^2}}-{\displaystyle \frac{75}{256\sqrt{2}}}{\displaystyle \frac{1}{x^3}}+{\displaystyle \frac{2475}{8192}}{\displaystyle \frac{1}{x^4}}+\mathrm{\cdots }\right).$
ⓘ Symbols: ${\mathrm{kei}}_{\nu }\left(x\right)$: Kelvin function, ${\ker }_{\nu }\left(x\right)$: Kelvin function, $\sim$: Poincaré asymptotic expansion, $\pi$: the ratio of the circumference of a circle to its diameter, $\mathrm{e}$: base of natural logarithm and $x$: real variable A&S Ref: 9.10.34 Permalink: http://dlmf.nist.gov/10.67.E16 Encodings: TeX, pMML, png See also: Annotations for §10.67(ii), §10.67 and Ch.10