Legendre’s relation (19.7.1) can be written

The case
shows that the product of the two lemniscate constants,
(19.20.2) and (19.20.22), is
.
The complete cases of
and
have connection formulas
resulting from those for the Gauss hypergeometric function
(Erdélyi et al. (1953a, §2.9)). Upper signs apply if
,
and lower signs if
:
Let
,
, and
be positive and distinct, and permute
and
to
ensure that
does not lie between
and
. The complete case of
can be expressed in terms of
and
:

If
and
, then as
(19.21.6) reduces to
Legendre’s relation (19.21.1).
is symmetric only in
and
, but either (nonzero)
or (nonzero)
can be moved to the third position by using
Suggested 2021-06-07 by Luc Maisonobe
or the corresponding equation with
and
interchanged.
Suggested 2021-06-07 by Luc Maisonobe

Suggested 2022-06-27 by Abdulhafeez Abdulsalam
Suggested 2021-06-07 by Luc Maisonobe
Because
is completely symmetric,
can be permuted on the
right-hand side of (19.21.10) so that
if the
variables are real, thereby avoiding cancellations when
is
calculated from
and
(see §19.36(i)).
where both summations extend over the three cyclic permutations of
.
Connection formulas for
are given in
Carlson (1977b, pp. 99, 101, and 123–124).
Let
be real and nonnegative, with at most one of them 0.
Change-of-parameter relations can be used to shift the parameter
of
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
and
may be permuted. Also,
For each value of
, permutation of
produces three values
of
, one of which lies in the same region as
and two lie in the other
region of the same type. In (19.21.12), if
is the largest
(smallest) of
, and
, then
and
lie in the same region if it
is circular (hyperbolic); otherwise
and
lie in different regions, both
circular or both hyperbolic. If
, then
and
; hence
