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19 Elliptic IntegralsLegendre’s Integrals

§19.5 Maclaurin and Related Expansions

If |k|<1 and |α|<1, then

19.5.1 K⁡(k)=π2⁢∑m=0∞(12)m⁢(12)mm!⁢m!⁢k2⁢m=π2⁢F12⁡(12,121;k2),

where F12 is the Gauss hypergeometric function (§§15.1 and 15.2(i)).

19.5.2 E⁡(k)=π2⁢∑m=0∞(−12)m⁢(12)mm!⁢m!⁢k2⁢m=π2⁢F12⁡(−12,121;k2),
19.5.3 D⁡(k)=π4⁢∑m=0∞(32)m⁢(12)m(m+1)!⁢m!⁢k2⁢m=π4⁢F12⁡(32,122;k2),
19.5.4 Π⁡(α2,k)=π2⁢∑n=0∞(12)nn!⁢∑m=0n(12)mm!⁢k2⁢m⁢α2⁢n−2⁢m=π2⁢F1⁡(12;12,1;1;k2,α2),
19.5.4_1 F⁡(ϕ,k)=∑m=0∞(12)m⁢sin2⁢m+1⁡ϕ(2⁢m+1)⁢m!⁢F12⁡(m+12,12m+32;sin2⁢ϕ)⁢k2⁢m=sin⁡ϕ⁢F1⁡(12;12,12;32;sin2⁡ϕ,k2⁢sin2⁡ϕ),
19.5.4_2 E⁡(ϕ,k)=∑m=0∞(−12)m⁢sin2⁢m+1⁡ϕ(2⁢m+1)⁢m!⁢F12⁡(m+12,12m+32;sin2⁢ϕ)⁢k2⁢m=sin⁡ϕ⁢F1⁡(12;12,−12;32;sin2⁡ϕ,k2⁢sin2⁡ϕ),
19.5.4_3 Π⁡(ϕ,α2,k)=∑m=0∞(12)m⁢sin2⁢m+1⁡ϕ(2⁢m+1)⁢m!⁢F1⁡(m+12;12,1;m+32;sin2⁡ϕ,α2⁢sin2⁡ϕ)⁢k2⁢m,

where F1⁡(α;β,β′;γ;x,y) is an Appell function (§16.13).

For Jacobi’s nome q:

19.5.5 q=exp⁡(−π⁢K′⁡(k)/K⁡(k))=r+8⁢r2+84⁢r3+992⁢r4+⋯,
r=116⁢k2, 0≤k≤1.

Also,

19.5.6 q=λ+2⁢λ5+15⁢λ9+150⁢λ13+1707⁢λ17+⋯,
0≤k≤1,

where

19.5.7 λ=(1−k′)/(2⁢(1+k′)).

Coefficients of terms up to λ49 are given in Lee (1990), along with tables of fractional errors in K⁡(k) and E⁡(k), 0.1≤k2≤0.9999, obtained by using 12 different truncations of (19.5.6) in (19.5.8) and (19.5.9).

19.5.8 K⁡(k)=π2⁢(1+2⁢∑n=1∞qn2)2,
|q|<1,
19.5.9 E⁡(k)=K⁡(k)+2⁢π2K⁡(k)⁢∑n=1∞(−1)n⁢n2⁢qn21+2⁢∑n=1∞(−1)n⁢qn2,
|q|<1.

An infinite series for ln⁡K⁡(k) is equivalent to the infinite product

19.5.10 K⁡(k)=π2⁢∏m=1∞(1+km),

where k0=k and

19.5.11 km+1=1−1−km21+1−km2,
m=0,1,….

Series expansions of F⁡(ϕ,k) and E⁡(ϕ,k) are surveyed and improved in Van de Vel (1969), and the case of F⁡(ϕ,k) is summarized in Gautschi (1975, §1.3.2). For series expansions of Π⁡(ϕ,α2,k) when |α2|<1 see Erdélyi et al. (1953b, §13.6(9)). See also Karp et al. (2007).