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19 Elliptic IntegralsSymmetric Integrals

§19.21 Connection Formulas

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§19.21(i) Complete Integrals

The complete cases of \mathop{R_{F}\/}\nolimits and \mathop{R_{G}\/}\nolimits have connection formulas resulting from those for the Gauss hypergeometric function (Erdélyi et al. (1953a, §2.9)). Upper signs apply if 0<\mathop{\mathrm{ph}\/}\nolimits z<\pi, and lower signs if -\pi<\mathop{\mathrm{ph}\/}\nolimits z<0:

Let y, z, and p be positive and distinct, and permute y and z to ensure that y does not lie between z and p. The complete case of \mathop{R_{J}\/}\nolimits can be expressed in terms of \mathop{R_{F}\/}\nolimits and \mathop{R_{D}\/}\nolimits:

If 0<p<z and y=z+1, then as p\to 0 (19.21.6) reduces to Legendre’s relation (19.21.1).

§19.21(ii) Incomplete Integrals

\mathop{R_{D}\/}\nolimits\!\left(x,y,z\right) is symmetric only in x and y, but either (nonzero) x or (nonzero) y can be moved to the third position by using

or the corresponding equation with x and y interchanged.

Because \mathop{R_{G}\/}\nolimits is completely symmetric, x,y,z can be permuted on the right-hand side of (19.21.10) so that (x-z)(y-z)\leq 0 if the variables are real, thereby avoiding cancellations when \mathop{R_{G}\/}\nolimits is calculated from \mathop{R_{F}\/}\nolimits and \mathop{R_{D}\/}\nolimits (see §19.36(i)).

where both summations extend over the three cyclic permutations of x,y,z.

Connection formulas for \mathop{R_{{-a}}\/}\nolimits\!\left(\mathbf{b};\mathbf{z}\right) are given in Carlson (1977b, pp. 99, 101, and 123–124).

§19.21(iii) Change of Parameter of \mathop{R_{J}\/}\nolimits

Let x,y,z be real and nonnegative, with at most one of them 0. Change-of-parameter relations can be used to shift the parameter p of \mathop{R_{J}\/}\nolimits from either circular region to the other, or from either hyperbolic region to the other (§19.20(iii)). The latter case allows evaluation of Cauchy principal values (see (19.20.14)).

where

19.21.13
(p-x)(q-x)=(y-x)(z-x),
\xi=yz/x,
\eta=pq/x,

and x,y,z may be permuted. Also,

19.21.14\eta-\xi=p+q-y-z=\frac{(p-y)(p-z)}{p-x}=\frac{(q-y)(q-z)}{q-x}=\frac{(p-y)(q-y%
)}{x-y}=\frac{(p-z)(q-z)}{x-z}.

For each value of p, permutation of x,y,z produces three values of q, one of which lies in the same region as p and two lie in the other region of the same type. In (19.21.12), if x is the largest (smallest) of x,y, and z, then p and q lie in the same region if it is circular (hyperbolic); otherwise p and q lie in different regions, both circular or both hyperbolic. If x=0, then \xi=\eta=\infty and \mathop{R_{C}\/}\nolimits\!\left(\xi,\eta\right)=0; hence