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19 Elliptic IntegralsSymmetric Integrals

§19.21 Connection Formulas

Contents
  1. §19.21(i) Complete Integrals
  2. §19.21(ii) Incomplete Integrals
  3. §19.21(iii) Change of Parameter of R_{J}

§19.21(i) Complete Integrals

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

19.21.4 R_{F}\left(0,z-1,z\right)=R_{F}\left(0,1-z,1\right)\mp\mathrm{i}R_{F}\left(0,z%
,1\right),

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 R_{J} can be expressed in terms of R_{F} and R_{D}:

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

R_{D}\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

19.21.7 (x-y)R_{D}\left(y,z,x\right)+(z-y)R_{D}\left(x,y,z\right)=3R_{F}\left(x,y,z%
\right)-3y^{1/2}x^{-1/2}z^{-1/2},

or the corresponding equation with x and y interchanged.

19.21.8 R_{D}\left(y,z,x\right)+R_{D}\left(z,x,y\right)+R_{D}\left(x,y,z\right)=3x^{-1%
/2}y^{-1/2}z^{-1/2},
19.21.10 2R_{G}\left(x,y,z\right)=zR_{F}\left(x,y,z\right)-\tfrac{1}{3}(x-z)(y-z)R_{D}%
\left(x,y,z\right)+x^{1/2}y^{1/2}z^{-1/2},z\neq 0.

Because R_{G} 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 R_{G} is calculated from R_{F} and R_{D} (see §19.36(i)).

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

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

§19.21(iii) Change of Parameter of R_{J}

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 R_{J} 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 R_{C}\left(\xi,\eta\right)=0; hence