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In [[mathematics]], a '''lemniscatic elliptic function''' is an [[elliptic function]] related to the arc length of a [[lemniscate of Bernoulli]] studied by [[Giulio Carlo de' Toschi di Fagnano]] in 1718. It has a square period lattice and is closely related to the [[Weierstrass elliptic function]] when the Weierstrass invariants satisfy ''g''<sub>2</sub> = 1 and ''g''<sub>3</sub> = 0.
In the lemniscatic case, the minimal half period
:<math>\frac{\Gamma^2(\tfrac{1}{4})}{4\sqrt{\pi}}</math>
where
and equal to ''
The [[mathematical constant|constant]]s ''e<sub>''1</sub>, ''e<sub>''2</sub>, and ''e<sub>''3</sub> are given by
:<math>
e_1=\
e_2=0,\qquad
e_3=-\
</math>
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==Lemniscate sine and cosine functions==
The [[lemniscate]] sine and cosine functions '''sl''' and '''cl''' are analogues of the usual sine and cosine functions, with a circle replaced by a lemniscate. They are defined by
:<math>\operatorname{sl}(r)=s</math>
where
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:<math>\operatorname{cl}(r)=c</math>
:<math> r=\int_c^1\frac{dt}{\sqrt{1-t^4}}.</math>
They are doubly periodic (or elliptic) functions in the complex plane, with periods
:<math>G=\frac{2}{\pi}\int_0^1\frac{dt}{\sqrt{1-t^4}}= 0.8346\ldots.</math>
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The [[lemniscate of Bernoulli]]
:<math>(x^2+y^2)^2=x^2-y^2</math>
consists of the points such that the product of their distances from two the two points ({{frac|1
:<math> r=\int_0^s\frac{dt}{\sqrt{1-t^4}}.</math>
In other words, the sine lemniscatic function gives the distance from the origin as a function of the arc length from the origin. Similarly the cosine lemniscate function gives the distance from the origin as a function of the arc length from (1, 0).
==See also==
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