Digital Library of Mathematical Functions
About the Project
NIST
28 Mathieu Functions and Hill’s EquationModified Mathieu Functions

§28.26 Asymptotic Approximations for Large q

Contents

§28.26(i) Goldstein’s Expansions

Denote

where

28.26.3\phi=2h\mathop{\sinh\/}\nolimits z-\left(m+\tfrac{1}{2}\right)\mathop{\mathrm{%
arctan}\/}\nolimits\!\left(\mathop{\sinh\/}\nolimits z\right).

Then as h\to+\infty with fixed z in \realpart{z}>0 and fixed s=2m+1,

28.26.4\mathop{\mathrm{Fc}_{{m}}\/}\nolimits\!\left(z,h\right)\sim 1+\dfrac{s}{8h{%
\mathop{\cosh\/}\nolimits^{{2}}}z}+\dfrac{1}{2^{{11}}h^{2}}\left(\dfrac{s^{4}+%
86s^{2}+105}{{\mathop{\cosh\/}\nolimits^{{4}}}z}-\dfrac{s^{4}+22s^{2}+57}{{%
\mathop{\cosh\/}\nolimits^{{2}}}z}\right)+\dfrac{1}{2^{{14}}h^{3}}\left(-%
\dfrac{s^{5}+14s^{3}+33s}{{\mathop{\cosh\/}\nolimits^{{2}}}z}-\dfrac{2s^{5}+12%
4s^{3}+1122s}{{\mathop{\cosh\/}\nolimits^{{4}}}z}+\dfrac{3s^{5}+290s^{3}+1627s%
}{{\mathop{\cosh\/}\nolimits^{{6}}}z}\right)+\cdots,
28.26.5\mathop{\mathrm{Gc}_{{m}}\/}\nolimits\!\left(z,h\right)\sim\dfrac{\mathop{%
\sinh\/}\nolimits z}{{\mathop{\cosh\/}\nolimits^{{2}}}z}\left(\dfrac{s^{2}+3}{%
2^{5}h}+\dfrac{1}{2^{9}h^{2}}\left(s^{3}+3s+\dfrac{4s^{3}+44s}{{\mathop{\cosh%
\/}\nolimits^{{2}}}z}\right)+\dfrac{1}{2^{{14}}h^{3}}\left(5s^{4}+34s^{2}+9-%
\dfrac{s^{6}-47s^{4}+667s^{2}+2835}{12{\mathop{\cosh\/}\nolimits^{{2}}}z}+%
\dfrac{s^{6}+505s^{4}+12139s^{2}+10395}{12{\mathop{\cosh\/}\nolimits^{{4}}}z}%
\right)\right)+\cdots.

The asymptotic expansions of \mathop{\mathrm{Fs}_{{m}}\/}\nolimits\!\left(z,h\right) and \mathop{\mathrm{Gs}_{{m}}\/}\nolimits\!\left(z,h\right) in the same circumstances are also given by the right-hand sides of (28.26.4) and (28.26.5), respectively.

For additional terms see Goldstein (1927).

§28.26(ii) Uniform Approximations

See §28.8(iv). For asymptotic approximations for \mathop{{\mathrm{M}^{{(3,4)}}_{{\nu}}}\/}\nolimits\!\left(z,h\right) see also Naylor (1984, 1987, 1989).