19.24 Inequalities19.26 Addition Theorems

§19.25 Relations to Other Functions

Contents

§19.25(i) Legendre’s Integrals as Symmetric Integrals

Let {k^{{\prime}}}^{2}=1-k^{2} and c={\mathop{\csc\/}\nolimits^{{2}}}\phi. Then

19.25.1
\mathop{K\/}\nolimits\!\left(k\right)=\mathop{R_{F}\/}\nolimits\!\left(0,{k^{{\prime}}}^{2},1\right),
\mathop{E\/}\nolimits\!\left(k\right)=2\!\mathop{R_{G}\/}\nolimits\!\left(0,{k^{{\prime}}}^{2},1\right),
\mathop{E\/}\nolimits\!\left(k\right)=\tfrac{1}{3}{k^{{\prime}}}^{2}\left(\mathop{R_{D}\/}\nolimits\!\left(0,{k^{{\prime}}}^{2},1\right)+\mathop{R_{D}\/}\nolimits\!\left(0,1,{k^{{\prime}}}^{2}\right)\right),
\mathop{K\/}\nolimits\!\left(k\right)-\mathop{E\/}\nolimits\!\left(k\right)=k^{2}\mathop{D\/}\nolimits\!\left(k\right)=\tfrac{1}{3}k^{2}\mathop{R_{D}\/}\nolimits\!\left(0,{k^{{\prime}}}^{2},1\right),
\mathop{E\/}\nolimits\!\left(k\right)-{k^{{\prime}}}^{2}\mathop{K\/}\nolimits\!\left(k\right)=\tfrac{1}{3}k^{2}{k^{{\prime}}}^{2}\mathop{R_{D}\/}\nolimits\!\left(0,1,{k^{{\prime}}}^{2}\right).
19.25.2 \mathop{\Pi\/}\nolimits\!\left(\alpha^{2},k\right)-\mathop{K\/}\nolimits\!\left(k\right)=\tfrac{1}{3}\alpha^{2}\mathop{R_{J}\/}\nolimits\!\left(0,{k^{{\prime}}}^{2},1,1-\alpha^{2}\right).
19.25.3 \mathop{\Pi\/}\nolimits\!\left(\alpha^{2},k\right)=\tfrac{1}{2}\pi\mathop{R_{{-\frac{1}{2}}}\/}\nolimits\!\left(\tfrac{1}{2},-\tfrac{1}{2},1;{k^{{\prime}}}^{2},1,1-\alpha^{2}\right),

with Cauchy principal value

19.25.4 \mathop{\Pi\/}\nolimits\!\left(\alpha^{2},k\right)=-\tfrac{1}{3}(k^{2}/\alpha^{2})\mathop{R_{J}\/}\nolimits\!\left(0,1-k^{2},1,1-(k^{2}/\alpha^{2})\right), -\infty<k^{2}<1<\alpha^{2}.
19.25.7 \mathop{E\/}\nolimits\!\left(\phi,k\right)=2\!\mathop{R_{G}\/}\nolimits\!\left(c-1,c-k^{2},c\right)-(c-1)\mathop{R_{F}\/}\nolimits\!\left(c-1,c-k^{2},c\right)-\sqrt{(c-1)(c-k^{2})/c},
19.25.8 \mathop{E\/}\nolimits\!\left(\phi,k\right)=\mathop{R_{{-\frac{1}{2}}}\/}\nolimits\!\left(\tfrac{1}{2},-\tfrac{1}{2},\tfrac{3}{2};c-1,c-k^{2},c\right),
19.25.9 \mathop{E\/}\nolimits\!\left(\phi,k\right)=\mathop{R_{F}\/}\nolimits\!\left(c-1,c-k^{2},c\right)-\tfrac{1}{3}k^{2}\mathop{R_{D}\/}\nolimits\!\left(c-1,c-k^{2},c\right),
19.25.10 \mathop{E\/}\nolimits\!\left(\phi,k\right)={k^{{\prime}}}^{2}\mathop{R_{F}\/}\nolimits\!\left(c-1,c-k^{2},c\right)+\tfrac{1}{3}k^{2}{k^{{\prime}}}^{2}\mathop{R_{D}\/}\nolimits\!\left(c-1,c,c-k^{2}\right)+k^{2}\sqrt{(c-1)/(c(c-k^{2}))}, c>k^{2},
19.25.11 \mathop{E\/}\nolimits\!\left(\phi,k\right)=-\tfrac{1}{3}{k^{{\prime}}}^{2}\mathop{R_{D}\/}\nolimits\!\left(c-k^{2},c,c-1\right)+\sqrt{(c-k^{2})/(c(c-1))}, \phi\neq\tfrac{1}{2}\pi.

Equations (19.25.9)–(19.25.11) correspond to three (nonzero) choices for the last variable of \mathop{R_{D}\/}\nolimits; see (19.21.7). All terms on the right-hand sides are nonnegative when k^{2}\leq 0, 0\leq k^{2}\leq 1, or 1\leq k^{2}\leq c, respectively.

19.25.12 \frac{\partial\mathop{E\/}\nolimits\!\left(\phi,k\right)}{\partial k}=-\tfrac{1}{3}k\mathop{R_{D}\/}\nolimits\!\left(c-1,c-k^{2},c\right).
19.25.13 \mathop{D\/}\nolimits\!\left(\phi,k\right)=\tfrac{1}{3}\mathop{R_{D}\/}\nolimits\!\left(c-1,c-k^{2},c\right).
19.25.14 \mathop{\Pi\/}\nolimits\!\left(\phi,\alpha^{2},k\right)-\mathop{F\/}\nolimits\!\left(\phi,k\right)=\tfrac{1}{3}\alpha^{2}\mathop{R_{J}\/}\nolimits\!\left(c-1,c-k^{2},c,c-\alpha^{2}\right),
19.25.15 \mathop{\Pi\/}\nolimits\!\left(\phi,\alpha^{2},k\right)=\mathop{R_{{-\frac{1}{2}}}\/}\nolimits\!\left(\tfrac{1}{2},\tfrac{1}{2},-\tfrac{1}{2},1;c-1,c-k^{2},c,c-\alpha^{2}\right).

If \alpha^{2}>c, then the Cauchy principal value is

19.25.16 \mathop{\Pi\/}\nolimits\!\left(\phi,\alpha^{2},k\right)=-\tfrac{1}{3}\omega^{2}\mathop{R_{J}\/}\nolimits\!\left(c-1,c-k^{2},c,c-\omega^{2}\right)+\sqrt{\frac{(c-1)(c-k^{2})}{(\alpha^{2}-1)(1-\omega^{2})}}\*\mathop{R_{C}\/}\nolimits\!\left(c(\alpha^{2}-1)(1-\omega^{2}),(\alpha^{2}-c)(c-\omega^{2})\right), \omega^{2}=k^{2}/\alpha^{2}.

The transformations in §19.7(ii) result from the symmetry and homogeneity of functions on the right-hand sides of (19.25.5), (19.25.7), and (19.25.14). For example, if we write (19.25.5) as

19.25.17 \mathop{F\/}\nolimits\!\left(\phi,k\right)=\mathop{R_{F}\/}\nolimits\!\left(x,y,z\right),

with

19.25.18 (x,y,z)=(c-1,c-k^{2},c),

then the five nontrivial permutations of x,y,z that leave \mathop{R_{F}\/}\nolimits invariant change k^{2} (=(z-y)/(z-x)) into 1/k^{2}, {k^{{\prime}}}^{2}, 1/{k^{{\prime}}}^{2}, -k^{2}/{k^{{\prime}}}^{2}, -{k^{{\prime}}}^{2}/k^{2}, and \mathop{\sin\/}\nolimits\phi (=\sqrt{(z-x)/z}) into k\mathop{\sin\/}\nolimits\phi, -i\mathop{\tan\/}\nolimits\phi, -ik^{{\prime}}\mathop{\tan\/}\nolimits\phi, (k^{{\prime}}\mathop{\sin\/}\nolimits\phi)/\sqrt{1-k^{2}{\mathop{\sin\/}\nolimits^{{2}}}\phi}, -ik\mathop{\sin\/}\nolimits\phi/\sqrt{1-k^{2}{\mathop{\sin\/}\nolimits^{{2}}}\phi}. Thus the five permutations induce five transformations of Legendre’s integrals (and also of the Jacobian elliptic functions).

The three changes of parameter of \mathop{\Pi\/}\nolimits\!\left(\phi,\alpha^{2},k\right) in §19.7(iii) are unified in (19.21.12) by way of (19.25.14).

§19.25(iii) Symmetric Integrals as Legendre’s Integrals

Assume 0\leq x\leq y\leq z, x<z, and p>0. Let

19.25.23
\phi=\mathop{\mathrm{arccos}\/}\nolimits\sqrt{\ifrac{x}{z}}=\mathop{\mathrm{arcsin}\/}\nolimits\sqrt{\ifrac{(z-x)}{z}},
k=\sqrt{\frac{z-y}{z-x}},
\alpha^{2}=\frac{z-p}{z-x},

with \alpha\neq 0. Then

19.25.24 (z-x)^{{1/2}}\mathop{R_{F}\/}\nolimits\!\left(x,y,z\right)=\mathop{F\/}\nolimits\!\left(\phi,k\right),
19.25.25 (z-x)^{{3/2}}\mathop{R_{D}\/}\nolimits\!\left(x,y,z\right)=(3/k^{2})(\mathop{F\/}\nolimits\!\left(\phi,k\right)-\mathop{E\/}\nolimits\!\left(\phi,k\right)),
19.25.26 (z-x)^{{3/2}}\mathop{R_{J}\/}\nolimits\!\left(x,y,z,p\right)=(3/\alpha^{2}){(\mathop{\Pi\/}\nolimits\!\left(\phi,\alpha^{2},k\right)-\mathop{F\/}\nolimits\!\left(\phi,k\right))},
19.25.27 2(z-x)^{{-1/2}}\mathop{R_{G}\/}\nolimits\!\left(x,y,z\right)=\mathop{E\/}\nolimits\!\left(\phi,k\right)+(\mathop{\cot\/}\nolimits\phi)^{2}\mathop{F\/}\nolimits\!\left(\phi,k\right)+(\mathop{\cot\/}\nolimits\phi)\sqrt{1-k^{2}{\mathop{\sin\/}\nolimits^{{2}}}\phi}.

§19.25(iv) Theta Functions

For relations of symmetric integrals to theta functions, see §20.9(i).

§19.25(v) Jacobian Elliptic Functions

For the notation see §§22.2, 22.15, and 22.16(i).

With 0\leq k^{2}\leq 1 and \mathrm{p,q,r} any permutation of the letters \mathrm{c,d,n}, define

19.25.28 \Delta(\mathrm{p,q})={\mathop{\mathrm{ps}\/}\nolimits^{{2}}}\left(u,k\right)-{\mathop{\mathrm{qs}\/}\nolimits^{{2}}}\left(u,k\right)=-\Delta(\mathrm{q,p}),

which implies

19.25.29
\Delta(\mathrm{n,d})=k^{2},
\Delta(\mathrm{d,c})={k^{{\prime}}}^{2},
\Delta(\mathrm{n,c})=1.

If {\mathop{\mathrm{cs}\/}\nolimits^{{2}}}\left(u,k\right)\geq 0, then

19.25.30 \mathop{\mathrm{am}\/}\nolimits\left(u,k\right)=\mathop{R_{C}\/}\nolimits\!\left({\mathop{\mathrm{cs}\/}\nolimits^{{2}}}\left(u,k\right),{\mathop{\mathrm{ns}\/}\nolimits^{{2}}}\left(u,k\right)\right),
19.25.31 u=\mathop{R_{F}\/}\nolimits\!\left({\mathop{\mathrm{ps}\/}\nolimits^{{2}}}\left(u,k\right),{\mathop{\mathrm{qs}\/}\nolimits^{{2}}}\left(u,k\right),{\mathop{\mathrm{rs}\/}\nolimits^{{2}}}\left(u,k\right)\right);

compare (19.25.35) and (20.9.3).

19.25.32 \mathop{\mathrm{arcps}\/}\nolimits\left(x,k\right)=\mathop{R_{F}\/}\nolimits\!\left(x^{2},x^{2}+\Delta(\mathrm{q,p}),x^{2}+\Delta(\mathrm{r,p})\right),
19.25.33 \mathop{\mathrm{arcsp}\/}\nolimits\left(x,k\right)=x\mathop{R_{F}\/}\nolimits\!\left(1,1+\Delta(\mathrm{q,p})x^{2},1+\Delta(\mathrm{r,p})x^{2}\right),
19.25.34 \mathop{\mathrm{arcpq}\/}\nolimits\left(x,k\right)=\sqrt{w}\mathop{R_{F}\/}\nolimits\!\left(x^{2},1,1+\Delta(\mathrm{r,q})w\right), w=\ifrac{(1-x^{2})}{\Delta(\mathrm{q,p})},

where we assume 0\leq x^{2}\leq 1 if x=\mathop{\mathrm{sn}\/}\nolimits, \mathop{\mathrm{cn}\/}\nolimits, or \mathop{\mathrm{cd}\/}\nolimits; x^{2}\geq 1 if x=\mathop{\mathrm{ns}\/}\nolimits, \mathop{\mathrm{nc}\/}\nolimits, or \mathop{\mathrm{dc}\/}\nolimits; x real if x=\mathop{\mathrm{cs}\/}\nolimits or \mathop{\mathrm{sc}\/}\nolimits; k^{{\prime}}\leq x\leq 1 if x=\mathop{\mathrm{dn}\/}\nolimits; 1\leq x\leq 1/k^{{\prime}} if x=\mathop{\mathrm{nd}\/}\nolimits; x^{2}\geq{k^{{\prime}}}^{2} if x=\mathop{\mathrm{ds}\/}\nolimits; 0\leq x^{2}\leq 1/{k^{{\prime}}}^{2} if x=\mathop{\mathrm{sd}\/}\nolimits.

For the use of R-functions with \Delta(\mathrm{p,q}) in unifying other properties of Jacobian elliptic functions, see Carlson (2004, 2006a, 2006b, 2008).

Inversions of 12 elliptic integrals of the first kind, producing the 12 Jacobian elliptic functions, are combined and simplified by using the properties of \mathop{R_{F}\/}\nolimits\!\left(x,y,z\right). See (19.29.19), Carlson (2005), and (22.15.11), and compare with Abramowitz and Stegun (1964, Eqs. (17.4.41)–(17.4.52)). For analogous integrals of the second kind, which are not invertible in terms of single-valued functions, see (19.29.20) and (19.29.21) and compare with Gradshteyn and Ryzhik (2000, §3.153,1–10 and §3.156,1–9).

§19.25(vi) Weierstrass Elliptic Functions

§19.25(vii) Hypergeometric Function

19.25.42 \mathop{{{}_{{2}}F_{{1}}}\/}\nolimits\!\left(a,b;c;z\right)=\mathop{R_{{-a}}\/}\nolimits\!\left(b,c-b;1-z,1\right),
19.25.43 \mathop{R_{{-a}}\/}\nolimits\!\left(b_{1},b_{2};z_{1},z_{2}\right)=z_{2}^{{-a}}\mathop{{{}_{{2}}F_{{1}}}\/}\nolimits\!\left(a,b_{1};b_{1}+b_{2};1-(z_{1}/z_{2})\right).

For these results and extensions to the Appell function \mathop{{F_{{1}}}\/}\nolimits16.13) and Lauricella’s function \mathop{F_{D}\/}\nolimits see Carlson (1963). (\mathop{{F_{{1}}}\/}\nolimits and \mathop{F_{D}\/}\nolimits are equivalent to the R-function of 3 and n variables, respectively, but lack full symmetry.)