For ,
the inverse
-sine
is defined on
by (Lindqvist 1995)
|
(1)
|
The -sine
is the inverse function on the interval
,
where its quarter-period is
|
(2)
| |||
|
(3)
| |||
|
(4)
|
On this interval, the -cosine is defined by
. Extending the functions to the real line
by reflection and periodicity gives
|
(5)
|
so
parameterizes the unit superellipse
. When
, these definitions reduce to the ordinary sine
and cosine and
.
The -tangent
is defined by
and satisfies
|
(6)
|
Consequently, the substitution gives the improper
integral
|
(7)
| |||
|
(8)
| |||
|
(9)
|
where
is the beta function. It follows by symmetry that
|
(10)
|
(Poodiack 2026).
The term squigonometry is used for the broader study of analogues of trigonometry associated with
superellipses (Wood 2011, Poodiack and Wood 2022).
These -trigonometric
functions should not be confused with the area-parameterized squigonometric
functions. Both systems parameterize the same unit superellipse,
but the defining inverse integrands have exponents
and
, respectively. The
-trigonometric half-period
tends to 2 as
, whereas the constant denoted
for the squigonometric functions is the area
of the unit
-circle
and tends to 4. The two conventions coincide when
(Poodiack 2026).