Elliptic integral

In integral calculus, an elliptic integral is one of a number of related functions defined as the value of certain integrals, which were first studied by Giulio Fagnano and Leonhard Euler (c. 1750). Their name originates from their originally arising in connection with the problem of finding the arc length of an ellipse.

Modern mathematics defines an "elliptic integral" as any function $f$ which can be expressed in the form

f(x)=\int _{c}^{x}R{\left({\textstyle t,{\sqrt {P(t)}}}\right)}\,dt,

where $R$ is a rational function of its two arguments, $P$ is a polynomial of degree 3 or 4 with no repeated roots, and $c$ is a constant.

In general, integrals in this form cannot be expressed in terms of elementary functions. Exceptions to this general rule are when $P$ has repeated roots, or when $R (x, y)$ contains no odd powers of $y$ or if the integral is pseudo-elliptic. However, with the appropriate reduction formula, every elliptic integral can be brought into a form that involves integrals over rational functions and the three Legendre canonical forms (i.e. the elliptic integrals of the first, second and third kind).

Besides the Legendre form given below, the elliptic integrals may also be expressed in Carlson symmetric form. Additional insight into the theory of the elliptic integral may be gained through the study of the Schwarz–Christoffel mapping. Historically, elliptic functions were discovered as inverse functions of elliptic integrals.

Argument notation

Incomplete elliptic integrals are functions of two arguments; complete elliptic integrals are functions of a single argument. These arguments are expressed in a variety of different but equivalent ways (they give the same elliptic integral). Most texts adhere to a canonical naming scheme, using the following naming conventions.

For expressing one argument:

$α$ , the modular angle
$k = sin α$ , the elliptic modulus or eccentricity
$m = k 2 = sin 2 α$ , the parameter

Each of the above three quantities is completely determined by any of the others (given that they are non-negative). Thus, they can be used interchangeably.

The other argument can likewise be expressed as $φ$ , the amplitude, or as $x$ or $u$ , where $x = sin φ = sn u$ and $sn$ is one of the Jacobian elliptic functions.

Specifying the value of any one of these quantities determines the others. Note that $u$ also depends on $m$ . Some additional relationships involving $u$ include

\cos \varphi =\operatorname {cn} u,\quad {\textrm {and}}\quad {\sqrt {1-m\sin ^{2}\varphi }}=\operatorname {dn} u.

The latter is sometimes called the delta amplitude and written as $Δ(φ) = dn u$ . Sometimes the literature also refers to the complementary parameter, the complementary modulus, or the complementary modular angle. These are further defined in the article on quarter periods.

In this notation, the use of a vertical bar as delimiter indicates that the argument following it is the "parameter" (as defined above), while the backslash indicates that it is the modular angle. The use of a semicolon implies that the argument preceding it is the sine of the amplitude:

{\displaystyle F(\varphi ,\sin \alpha )=F\left(\varphi \mid \sin ^{2}\alpha \right)=F(\varphi \setminus \alpha )=F(\sin \varphi

This potentially confusing use of different argument delimiters is traditional in elliptic integrals and much of the notation is compatible with that used in the reference book by Abramowitz and Stegun and that used in the integral tables by Gradshteyn and Ryzhik.

There are still other conventions for the notation of elliptic integrals employed in the literature. The notation with interchanged arguments, $F (k, φ)$ , is often encountered; and similarly $E (k, φ)$ for the integral of the second kind. Abramowitz and Stegun substitute the integral of the first kind, $F (φ, k)$ , for the argument $φ$ in their definition of the integrals of the second and third kinds, unless this argument is followed by a vertical bar: i.e. $E (F (φ, k) | k 2)$ for $E (φ | k 2)$ . Moreover, their complete integrals employ the parameter $k 2$ as argument in place of the modulus $k$ , i.e. $K (k 2)$ rather than $K (k)$ . And the integral of the third kind defined by Gradshteyn and Ryzhik, $Π(φ, n, k)$ , puts the amplitude $φ$ first and not the "characteristic" $n$ .

Thus one must be careful with the notation when using these functions, because various reputable references and software packages use different conventions in the definitions of the elliptic functions. For example, Wolfram's Mathematica software and Wolfram Alpha define the complete elliptic integral of the first kind in terms of the parameter $m$ , instead of the elliptic modulus $k$ .

Incomplete elliptic integral of the first kind

The incomplete elliptic integral of the first kind $F$ is defined as

F(\varphi ,k)=F\left(\varphi \mid k^{2}\right)=F(\sin \varphi ;k)=\int _{0}^{\varphi }{\frac {d\theta }{\sqrt {1-k^{2}\sin ^{2}\theta }}}.

This is the trigonometric form of the integral; substituting $t = sin θ$ and $x = sin φ$ , one obtains the Legendre normal form:

F(x;k)=\int _{0}^{x}{\frac {dt}{\sqrt {\left(1-t^{2}\right)\left(1-k^{2}t^{2}\right)}}}.

Equivalently, in terms of the amplitude and modular angle one has:

F(\varphi \setminus \alpha )=F(\varphi ,\sin \alpha )=\int _{0}^{\varphi }{\frac {d\theta }{\sqrt {1-\left(\sin \theta \sin \alpha \right)^{2}}}}.

With $x = sn(u, k)$ one has:

F(x;k)=u;

demonstrating that this Jacobian elliptic function is a simple inverse of the incomplete elliptic integral of the first kind.

The incomplete elliptic integral of the first kind has following addition theorem:

F{\bigl [}\arctan(x),k{\bigr ]}+F{\bigl [}\arctan(y),k{\bigr ]}=F\left[\arctan \left({\frac {x{\sqrt {k'^{2}y^{2}+1}}}{\sqrt {y^{2}+1}}}\right)+\arctan \left({\frac {y{\sqrt {k'^{2}x^{2}+1}}}{\sqrt {x^{2}+1}}}\right),k\right]

The elliptic modulus can be transformed that way:

F{\bigl [}\arcsin(x),k{\bigr ]}={\frac {2}{1+{\sqrt {1-k^{2}}}}}F\left[\arcsin \left({\frac {\left(1+{\sqrt {1-k^{2}}}\right)x}{1+{\sqrt {1-k^{2}x^{2}}}}}\right),{\frac {1-{\sqrt {1-k^{2}}}}{1+{\sqrt {1-k^{2}}}}}\right]

Incomplete elliptic integral of the second kind

The incomplete elliptic integral of the second kind $E$ in trigonometric form is

E(\varphi ,k)=E\left(\varphi \,|\,k^{2}\right)=E(\sin \varphi ;k)=\int _{0}^{\varphi }{\sqrt {1-k^{2}\sin ^{2}\theta }}\,d\theta .

Substituting $t = sin θ$ and $x = sin φ$ , one obtains the Legendre normal form:

E(x;k)=\int _{0}^{x}{\frac {\sqrt {1-k^{2}t^{2}}}{\sqrt {1-t^{2}}}}\,dt.

Equivalently, in terms of the amplitude and modular angle:

E(\varphi \setminus \alpha )=E(\varphi ,\sin \alpha )=\int _{0}^{\varphi }{\sqrt {1-\left(\sin \theta \sin \alpha \right)^{2}}}\,d\theta .

Relations with the Jacobi elliptic functions include

{\begin{aligned}E{\left(\operatorname {sn} (u;k);k\right)}=\int _{0}^{u}\operatorname {dn} ^{2}(w;k)\,dw&=u-k^{2}\int _{0}^{u}\operatorname {sn} ^{2}(w;k)\,dw\\[1ex]&=\left(1-k^{2}\right)u+k^{2}\int _{0}^{u}\operatorname {cn} ^{2}(w;k)\,dw.\end{aligned}}

The meridian arc length from the equator to latitude $φ$ is written in terms of $E$ :

m(\varphi )=a\left(E(\varphi ,e)+{\frac {d^{2}}{d\varphi ^{2}}}E(\varphi ,e)\right),

where $a$ is the semi-major axis, and $e$ is the eccentricity.

The incomplete elliptic integral of the second kind has following addition theorem:

E{\left[\arctan(x),k\right]}+E{\left[\arctan(y),k\right]}=E{\left[\arctan \left({\frac {x{\sqrt {k'^{2}y^{2}+1}}}{\sqrt {y^{2}+1}}}\right)+\arctan \left({\frac {y{\sqrt {k'^{2}x^{2}+1}}}{\sqrt {x^{2}+1}}}\right),k\right]}+{\frac {k^{2}xy}{k'^{2}x^{2}y^{2}+x^{2}+y^{2}+1}}\left({\frac {x{\sqrt {k'^{2}y^{2}+1}}}{\sqrt {y^{2}+1}}}+{\frac {y{\sqrt {k'^{2}x^{2}+1}}}{\sqrt {x^{2}+1}}}\right)

The elliptic modulus can be transformed that way:

E{\left[\arcsin(x),k\right]}=\left(1+{\sqrt {1-k^{2}}}\right)E{\left[\arcsin \left({\frac {\left(1+{\sqrt {1-k^{2}}}\right)x}{1+{\sqrt {1-k^{2}x^{2}}}}}\right),{\frac {1-{\sqrt {1-k^{2}}}}{1+{\sqrt {1-k^{2}}}}}\right]}-{\sqrt {1-k^{2}}}F{\left[\arcsin(x),k\right]}+{\frac {k^{2}x{\sqrt {1-x^{2}}}}{1+{\sqrt {1-k^{2}x^{2}}}}}

Incomplete elliptic integral of the third kind

The incomplete elliptic integral of the third kind $Π$ is

\Pi (n;\varphi \setminus \alpha )=\int _{0}^{\varphi }{\frac {1}{1-n\sin ^{2}\theta }}{\frac {d\theta }{\sqrt {1-\left(\sin \theta \sin \alpha \right)^{2}}}}

or

\Pi (n;\varphi \,|\,m)=\int _{0}^{\sin \varphi }{\frac {1}{1-nt^{2}}}{\frac {dt}{\sqrt {\left(1-mt^{2}\right)\left(1-t^{2}\right)}}}.

The number $n$ is called the characteristic and can take on any value, independently of the other arguments. Note though that the value $Π(1; .mw-parser-output .sfrac{white-space:nowrap}.mw-parser-output .sfrac.tion,.mw-parser-output .sfrac .tion{display:inline-block;vertical-align:-0.5em;font-size:85%;text-align:center}.mw-parser-output .sfrac .num,.mw-parser-output .sfrac .den{display:block;line-height:1em;margin:0 0.1em}.mw-parser-output .sfrac .den{border-top:1px solid}.mw-parser-output .sr-only{border:0;clip:rect(0,0,0,0);height:1px;margin:-1px;overflow:hidden;padding:0;position:absolute;width:1px}π/2 | m)$ is infinite, for any $m$ .

A relation with the Jacobian elliptic functions is

\Pi {\bigl (}n;\,\operatorname {am} (u;k);\,k{\bigr )}=\int _{0}^{u}{\frac {dw}{1-n\,\operatorname {sn} ^{2}(w;k)}}.

The meridian arc length from the equator to latitude $φ$ is also related to a special case of $Π$ :

m(\varphi )=a\left(1-e^{2}\right)\Pi \left(e^{2};\varphi \,|\,e^{2}\right).

Complete elliptic integral of the first kind

Plot of the complete elliptic integral of the first kind

K (k)

Elliptic Integrals are said to be 'complete' when the amplitude $φ = π / 2$ and therefore $x = 1$ . The complete elliptic integral of the first kind $K$ may thus be defined as

K(k)=\int _{0}^{\tfrac {\pi }{2}}{\frac {d\theta }{\sqrt {1-k^{2}\sin ^{2}\theta }}}=\int _{0}^{1}{\frac {dt}{\sqrt {\left(1-t^{2}\right)\left(1-k^{2}t^{2}\right)}}},

or more compactly in terms of the incomplete integral of the first kind as

K(k)=F\left({\tfrac {\pi }{2}},k\right)=F\left({\tfrac {\pi }{2}}\,|\,k^{2}\right)=F(1;k).

It can be expressed as a power series

K(k)={\frac {\pi }{2}}\sum _{n=0}^{\infty }\left({\frac {(2n)!}{2^{2n}(n!)^{2}}}\right)^{2}k^{2n}={\frac {\pi }{2}}\sum _{n=0}^{\infty }{\bigl (}P_{2n}(0){\bigr )}^{2}k^{2n},

where $P n$ is the Legendre polynomials, which is equivalent to

K(k)={\frac {\pi }{2}}\left(1+\left({\frac {1}{2}}\right)^{2}k^{2}+\left({\frac {1\cdot 3}{2\cdot 4}}\right)^{2}k^{4}+\cdots +\left({\frac {\left(2n-1\right)!!}{\left(2n\right)!!}}\right)^{2}k^{2n}+\cdots \right),

where $n!!$ denotes the double factorial. In terms of the Gauss hypergeometric function, the complete elliptic integral of the first kind can be expressed as

K(k)={\tfrac {\pi }{2}}\,{}_{2}F_{1}\left({\tfrac {1}{2}},{\tfrac {1}{2}};1;k^{2}\right).

The complete elliptic integral of the first kind is sometimes called the quarter period. It can be computed very efficiently in terms of the arithmetic–geometric mean:^[1]

K(k)={\frac {\pi }{2\operatorname {agm} \left(1,{\sqrt {1-k^{2}}}\right)}}.

Therefore the modulus can be transformed as:

{\begin{aligned}K(k)&={\frac {\pi }{2\operatorname {agm} \left(1,{\sqrt {1-k^{2}}}\right)}}\\[4pt]&={\frac {\pi }{2\operatorname {agm} \left({\frac {1}{2}}+{\frac {\sqrt {1-k^{2}}}{2}},{\sqrt[{4}]{1-k^{2}}}\right)}}\\[4pt]&={\frac {\pi }{\left(1+{\sqrt {1-k^{2}}}\right)\operatorname {agm} \left(1,{\frac {2{\sqrt[{4}]{1-k^{2}}}}{\left(1+{\sqrt {1-k^{2}}}\right)}}\right)}}\\[4pt]&={\frac {2}{1+{\sqrt {1-k^{2}}}}}K\left({\frac {1-{\sqrt {1-k^{2}}}}{1+{\sqrt {1-k^{2}}}}}\right)\end{aligned}}

This expression is valid for all $n\in \mathbb {N}$ and $0 \leq k \leq 1$ :

K(k)=n\left[\sum _{a=1}^{n}\operatorname {dn} \left({\frac {2a}{n}}K(k);k\right)\right]^{-1}K\left[k^{n}\prod _{a=1}^{n}\operatorname {sn} \left({\frac {2a-1}{n}}K(k);k\right)^{2}\right]

Relation to the gamma function

If $k 2 = λ (i \sqrt r)$ and $r\in \mathbb {Q} ^{+}$ (where $λ$ is the modular lambda function), then $K (k)$ is expressible in closed form in terms of the gamma function.^[2] For example, $r = 2$ , $r = 3$ and $r = 7$ give, respectively,^[3]

K\left({\sqrt {2}}-1\right)={\frac {\Gamma \left({\frac {1}{8}}\right)\Gamma \left({\frac {3}{8}}\right){\sqrt {{\sqrt {2}}+1}}}{8{\sqrt[{4}]{2}}{\sqrt {\pi }}}},

and

K\left({\frac {{\sqrt {3}}-1}{2{\sqrt {2}}}}\right)={\frac {1}{8\pi }}{\sqrt[{4}]{3}}\,{\sqrt[{3}]{4}}\,\Gamma {\biggl (}{\frac {1}{3}}{\biggr )}^{3}

and

K\left({\frac {3-{\sqrt {7}}}{4{\sqrt {2}}}}\right)={\frac {\Gamma \left({\frac {1}{7}}\right)\Gamma \left({\frac {2}{7}}\right)\Gamma \left({\frac {4}{7}}\right)}{4{\sqrt[{4}]{7}}\pi }}.

More generally, the condition that

{\frac {iK'}{K}}={\frac {iK\left({\sqrt {1-k^{2}}}\right)}{K(k)}}

be in an imaginary quadratic field^{[note 1]} is sufficient.^[4]^[5] For instance, if $k = e 5 πi /6$ , then $iK' / K = e 2 πi /3$ and^[6]

K\left(e^{5\pi i/6}\right)={\frac {e^{-\pi i/12}\Gamma ^{3}\left({\frac {1}{3}}\right){\sqrt[{4}]{3}}}{4{\sqrt[{3}]{2}}\pi }}.

Relation to Jacobi theta function

The relation to Jacobi's theta function is given by

K(k)={\frac {\pi }{2}}\theta _{3}^{2}(q),

where the nome $q$ is

q(k)=\exp \left(-\pi {\frac {K\left({\sqrt {1-k^{2}}}\right)}{K(k)}}\right).

Asymptotic expressions

K\left(k\right)\approx {\frac {\pi }{2}}+{\frac {\pi }{8}}{\frac {k^{2}}{1-k^{2}}}-{\frac {\pi }{16}}{\frac {k^{4}}{1-k^{2}}}

This approximation has a relative precision better than 3×10⁻⁴ for $k < 1 / 2$ . Keeping only the first two terms is correct to 0.01 precision for $k < 1 / 2$ .

Differential equation

The differential equation for the elliptic integral of the first kind is

{\frac {d}{dk}}\left(k\left(1-k^{2}\right){\frac {dK(k)}{dk}}\right)=k\,K(k)

A second solution to this equation is $K\left({\sqrt {1-k^{2}}}\right)$ . This solution satisfies the relation

{\frac {d}{dk}}K(k)={\frac {E(k)}{k\left(1-k^{2}\right)}}-{\frac {K(k)}{k}}.

Continued fraction

A continued fraction expansion is:^[7]

{\frac {K(k)}{2\pi }}=-{\frac {1}{4}}+\sum _{n=0}^{\infty }{\frac {q^{n}}{1+q^{2n}}}=-{\frac {1}{4}}+{\cfrac {1}{1-q+{\cfrac {\left(1-q\right)^{2}}{1-q^{3}+{\cfrac {q\left(1-q^{2}\right)^{2}}{1-q^{5}+{\cfrac {q^{2}\left(1-q^{3}\right)^{2}}{1-q^{7}+{\cfrac {q^{3}\left(1-q^{4}\right)^{2}}{1-q^{9}+\cdots }}}}}}}}}},

where the nome is $q=q(k)=\exp[-\pi K'(k)/K(k)]$ in its definition.

Complete elliptic integral of the second kind

Plot of the complete elliptic integral of the second kind

E (k)

The complete elliptic integral of the second kind $E$ is defined as

E(k)=\int _{0}^{\tfrac {\pi }{2}}{\sqrt {1-k^{2}\sin ^{2}\theta }}\,d\theta =\int _{0}^{1}{\frac {\sqrt {1-k^{2}t^{2}}}{\sqrt {1-t^{2}}}}\,dt,

or more compactly in terms of the incomplete integral of the second kind $E (φ, k)$ as

E(k)=E\left({\tfrac {\pi }{2}},k\right)=E(1;k).

For an ellipse with semi-major axis $a$ and semi-minor axis $b$ and eccentricity $e = \sqrt 1 - b 2 / a 2$ , the complete elliptic integral of the second kind $E (e)$ is equal to one quarter of the circumference $C$ of the ellipse measured in units of the semi-major axis $a$ . In other words:

C=4aE(e).

The complete elliptic integral of the second kind can be expressed as a power series^[8]

E(k)={\frac {\pi }{2}}\sum _{n=0}^{\infty }\left({\frac {(2n)!}{2^{2n}\left(n!\right)^{2}}}\right)^{2}{\frac {k^{2n}}{1-2n}},

which is equivalent to

E(k)={\frac {\pi }{2}}\left(1-\left({\frac {1}{2}}\right)^{2}{\frac {k^{2}}{1}}-\left({\frac {1\cdot 3}{2\cdot 4}}\right)^{2}{\frac {k^{4}}{3}}-\cdots -\left({\frac {(2n-1)!!}{(2n)!!}}\right)^{2}{\frac {k^{2n}}{2n-1}}-\cdots \right).

In terms of the Gauss hypergeometric function, the complete elliptic integral of the second kind can be expressed as

E(k)={\tfrac {\pi }{2}}\,{}_{2}F_{1}\left({\tfrac {1}{2}},-{\tfrac {1}{2}};1;k^{2}\right).

The modulus can be transformed that way:

E(k)=\left(1+{\sqrt {1-k^{2}}}\right)\,E\left({\frac {1-{\sqrt {1-k^{2}}}}{1+{\sqrt {1-k^{2}}}}}\right)-{\sqrt {1-k^{2}}}\,K(k)

Computation

Like the integral of the first kind, the complete elliptic integral of the second kind can be computed very efficiently using the arithmetic–geometric mean.^[1]

Define sequences $a n$ and $g n$ , where $a 0 = 1$ , $g 0 = \sqrt 1 - k 2 = k'$ and the recurrence relations $a n + 1 = a n + g n / 2$ , $g n + 1 = \sqrt a n g n$ hold. Furthermore, define

c_{n}={\sqrt {\left|a_{n}^{2}-g_{n}^{2}\right|}}.

By definition,

a_{\infty }=\lim _{n\to \infty }a_{n}=\lim _{n\to \infty }g_{n}=\operatorname {agm} \left(1,{\sqrt {1-k^{2}}}\right).

Also

\lim _{n\to \infty }c_{n}=0.

Then

E(k)={\frac {\pi }{2a_{\infty }}}\left(1-\sum _{n=0}^{\infty }2^{n-1}c_{n}^{2}\right).

In practice, the arithmetic-geometric mean would simply be computed up to some limit. This formula converges quadratically for all $| k | \leq 1$ . To speed up computation further, the relation $c n + 1 = c n 2 / 4 a n + 1$ can be used.

Furthermore, if $k 2 = λ (i \sqrt r)$ and $r\in \mathbb {Q} ^{+}$ (where $λ$ is the modular lambda function), then $E (k)$ is expressible in closed form in terms of

K(k)={\frac {\pi }{2\operatorname {agm} \left(1,{\sqrt {1-k^{2}}}\right)}}

and hence can be computed without the need for the infinite summation term. For example, $r = 1$ , $r = 3$ and $r = 7$ give, respectively,^[9]

E\left({\frac {1}{\sqrt {2}}}\right)={\frac {1}{2}}K\left({\frac {1}{\sqrt {2}}}\right)+{\frac {\pi }{4K\left({\frac {1}{\sqrt {2}}}\right)}},

and

E\left({\frac {{\sqrt {3}}-1}{2{\sqrt {2}}}}\right)={\frac {3+{\sqrt {3}}}{6}}K\left({\frac {{\sqrt {3}}-1}{2{\sqrt {2}}}}\right)+{\frac {\pi {\sqrt {3}}}{12K\left({\frac {{\sqrt {3}}-1}{2{\sqrt {2}}}}\right)}},

and

E\left({\frac {3-{\sqrt {7}}}{4{\sqrt {2}}}}\right)={\frac {7+2{\sqrt {7}}}{14}}K\left({\frac {3-{\sqrt {7}}}{4{\sqrt {2}}}}\right)+{\frac {\pi {\sqrt {7}}}{28K\left({\frac {3-{\sqrt {7}}}{4{\sqrt {2}}}}\right)}}.

Derivative and differential equation

{\frac {dE(k)}{dk}}={\frac {E(k)-K(k)}{k}}

\left(k^{2}-1\right){\frac {d}{dk}}\left(k\;{\frac {dE(k)}{dk}}\right)=kE(k)

A second solution to this equation is $E (\sqrt 1 - k 2) - K (\sqrt 1 - k 2)$ .

Complete elliptic integral of the third kind

Plot of the complete elliptic integral of the third kind

Π(n, k)

with several fixed values of

n

The complete elliptic integral of the third kind $Π$ can be defined as

\Pi (n,k)=\int _{0}^{\frac {\pi }{2}}{\frac {d\theta }{\left(1-n\sin ^{2}\theta \right){\sqrt {1-k^{2}\sin ^{2}\theta }}}}.

Note that sometimes the elliptic integral of the third kind is defined with an inverse sign for the characteristic $n$ ,

\Pi '(n,k)=\int _{0}^{\frac {\pi }{2}}{\frac {d\theta }{\left(1+n\sin ^{2}\theta \right){\sqrt {1-k^{2}\sin ^{2}\theta }}}}.

Just like the complete elliptic integrals of the first and second kind, the complete elliptic integral of the third kind can be computed very efficiently using the arithmetic-geometric mean.^[1]

Partial derivatives

{\begin{aligned}{\frac {\partial \Pi (n,k)}{\partial n}}&={\frac {1}{2\left(k^{2}-n\right)(n-1)}}\left(E(k)+{\frac {1}{n}}\left(k^{2}-n\right)K(k)+{\frac {1}{n}}\left(n^{2}-k^{2}\right)\Pi (n,k)\right)\\[8pt]{\frac {\partial \Pi (n,k)}{\partial k}}&={\frac {k}{n-k^{2}}}\left({\frac {E(k)}{k^{2}-1}}+\Pi (n,k)\right)\end{aligned}}

Jacobi zeta function

In 1829, Jacobi defined the Jacobi zeta function:

Z(\varphi ,k)=E(\varphi ,k)-{\frac {E(k)}{K(k)}}F(\varphi ,k).

It is periodic in $\varphi$ with minimal period $\pi$ . It is related to the Jacobi zn function by $Z(\varphi ,k)=\operatorname {zn} (F(\varphi ,k),k)$ . In the literature (e.g. Whittaker and Watson (1927)), sometimes $Z$ means Wikipedia's $\operatorname {zn}$ . Some authors (e.g. King (1924)) use $Z$ for both Wikipedia's $Z$ and $\operatorname {zn}$ .

Legendre's relation

The Legendre's relation or Legendre Identity shows the relation of the integrals K and E of an elliptic modulus and its anti-related counterpart^[10]^[11] in an integral equation of second degree:

For two modules that are Pythagorean counterparts to each other, this relation is valid:

K(\varepsilon )E\left({\sqrt {1-\varepsilon ^{2}}}\right)+E(\varepsilon )K\left({\sqrt {1-\varepsilon ^{2}}}\right)-K(\varepsilon )K\left({\sqrt {1-\varepsilon ^{2}}}\right)={\frac {\pi }{2}}

For example:

K({\color {blueviolet}{\tfrac {3}{5}}})E({\color {blue}{\tfrac {4}{5}}})+E({\color {blueviolet}{\tfrac {3}{5}}})K({\color {blue}{\tfrac {4}{5}}})-K({\color {blueviolet}{\tfrac {3}{5}}})K({\color {blue}{\tfrac {4}{5}}})={\tfrac {1}{2}}\pi

And for two modules that are tangential counterparts to each other, the following relationship is valid:

(1+\varepsilon )K(\varepsilon )E({\tfrac {1-\varepsilon }{1+\varepsilon }})+{\tfrac {2}{1+\varepsilon }}E(\varepsilon )K({\tfrac {1-\varepsilon }{1+\varepsilon }})-2K(\varepsilon )K({\tfrac {1-\varepsilon }{1+\varepsilon }})={\tfrac {1}{2}}\pi

For example:

{\tfrac {4}{3}}K({\color {blue}{\tfrac {1}{3}}})E({\color {green}{\tfrac {1}{2}}})+{\tfrac {3}{2}}E({\color {blue}{\tfrac {1}{3}}})K({\color {green}{\tfrac {1}{2}}})-2K({\color {blue}{\tfrac {1}{3}}})K({\color {green}{\tfrac {1}{2}}})={\tfrac {1}{2}}\pi

The Legendre's relation for tangential modular counterparts results directly from the Legendre's identity for Pythagorean modular counterparts by using the Landen modular transformation on the Pythagorean counter modulus.

Special identity for the lemniscatic case

For the lemniscatic case, the elliptic modulus or specific eccentricity ε is equal to half the square root of two. Legendre's identity for the lemniscatic case can be proved as follows:

According to the Chain rule these derivatives hold:

{\frac {\mathrm {d} }{\mathrm {d} y}}\,K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-F{\biggl [}\arccos(xy);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}={\frac {{\sqrt {2}}\,x}{\sqrt {1-x^{4}y^{4}}}}

{\frac {\mathrm {d} }{\mathrm {d} y}}\,2E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-2E{\biggl [}\arccos(xy);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}+F{\biggl [}\arccos(xy);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}={\frac {{\sqrt {2}}\,x^{3}y^{2}}{\sqrt {1-x^{4}y^{4}}}}

By using the Fundamental theorem of calculus these formulas can be generated:

K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-F{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}=\int _{0}^{1}{\frac {{\sqrt {2}}\,x}{\sqrt {1-x^{4}y^{4}}}}\,\mathrm {d} y

2E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-2E{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}+F{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}=\int _{0}^{1}{\frac {{\sqrt {2}}\,x^{3}y^{2}}{\sqrt {1-x^{4}y^{4}}}}\,\mathrm {d} y

The Linear combination of the two now mentioned integrals leads to the following formula:

{\frac {\sqrt {2}}{\sqrt {1-x^{4}}}}{\biggl \{}2E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-2E{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}+F{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}{\biggr \}}\,+

+\,{\frac {{\sqrt {2}}\,x^{2}}{\sqrt {1-x^{4}}}}{\biggl \{}K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-F{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}{\biggr \}}=\int _{0}^{1}{\frac {2\,x^{3}(y^{2}+1)}{\sqrt {(1-x^{4})(1-x^{4}\,y^{4})}}}\,\mathrm {d} y

By forming the original antiderivative related to x from the function now shown using the Product rule this formula results:

{\biggl \{}K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-F{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}{\biggr \}}{\biggl \{}2E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-2E{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}+F{\biggl [}\arccos(x);{\frac {1}{2}}{\sqrt {2}}{\biggr ]}{\biggr \}}=

=\int _{0}^{1}{\frac {1}{y^{2}}}(y^{2}+1){\biggl [}{\text{artanh}}(y^{2})-{\text{artanh}}{\bigl (}{\frac {{\sqrt {1-x^{4}}}\,y^{2}}{\sqrt {1-x^{4}y^{4}}}}{\bigr )}{\biggr ]}\mathrm {d} y

If the value $x=1$ is inserted in this integral identity, then the following identity emerges:

K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}{\biggl [}2\,E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}{\biggr ]}=\int _{0}^{1}{\frac {1}{y^{2}}}(y^{2}+1)\,{\text{artanh}}(y^{2})\,\mathrm {d} y=

={\biggl [}2\arctan(y)-{\frac {1}{y}}(1-y^{2})\,{\text{artanh}}(y^{2}){\biggr ]}_{y=0}^{y=1}=2\arctan(1)={\frac {\pi }{2}}

This is how this lemniscatic excerpt from Legendre's identity appears:

2E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}^{2}={\frac {\pi }{2}}

Generalization for the overall case

Now the modular general case^[12]^[13] is worked out. For this purpose, the derivatives of the complete elliptic integrals are derived after the modulus $\varepsilon$ and then they are combined. And then the Legendre's identity balance is determined.

Because the derivative of the circle function is the negative product of the identical mapping function and the reciprocal of the circle function:

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}{\sqrt {1-\varepsilon ^{2}}}=-\,{\frac {\varepsilon }{\sqrt {1-\varepsilon ^{2}}}}

These are the derivatives of K and E shown in this article in the sections above:

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}K(\varepsilon )={\frac {1}{\varepsilon (1-\varepsilon ^{2})}}{\bigl [}E(\varepsilon )-(1-\varepsilon ^{2})K(\varepsilon ){\bigr ]}

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}E(\varepsilon )=-\,{\frac {1}{\varepsilon }}{\bigl [}K(\varepsilon )-E(\varepsilon ){\bigr ]}

In combination with the derivative of the circle function these derivatives are valid then:

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}K({\sqrt {1-\varepsilon ^{2}}})={\frac {1}{\varepsilon (1-\varepsilon ^{2})}}{\bigl [}\varepsilon ^{2}K({\sqrt {1-\varepsilon ^{2}}})-E({\sqrt {1-\varepsilon ^{2}}}){\bigr ]}

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}E({\sqrt {1-\varepsilon ^{2}}})={\frac {\varepsilon }{1-\varepsilon ^{2}}}{\bigl [}K({\sqrt {1-\varepsilon ^{2}}})-E({\sqrt {1-\varepsilon ^{2}}}){\bigr ]}

Legendre's identity includes products of any two complete elliptic integrals. For the derivation of the function side from the equation scale of Legendre's identity, the Product rule is now applied in the following:

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}K(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})={\frac {1}{\varepsilon (1-\varepsilon ^{2})}}{\bigl [}E(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})-K(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})+\varepsilon ^{2}K(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}}){\bigr ]}

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}E(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})={\frac {1}{\varepsilon (1-\varepsilon ^{2})}}{\bigl [}-E(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})+E(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})-(1-\varepsilon ^{2})K(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}}){\bigr ]}

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}K(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})={\frac {1}{\varepsilon (1-\varepsilon ^{2})}}{\bigl [}E(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})-K(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})-(1-2\varepsilon ^{2})K(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}}){\bigr ]}

Of these three equations, adding the top two equations and subtracting the bottom equation gives this result:

{\frac {\mathrm {d} }{\mathrm {d} \varepsilon }}{\bigl [}K(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})+E(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})-K(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}}){\bigr ]}=0

In relation to the $\varepsilon$ the equation balance constantly gives the value zero.

The previously determined result shall be combined with the Legendre equation to the modulus $\varepsilon =1/{\sqrt {2}}$ that is worked out in the section before:

2E{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}-K{\bigl (}{\frac {1}{2}}{\sqrt {2}}{\bigr )}^{2}={\frac {\pi }{2}}

The combination of the last two formulas gives the following result:

K(\varepsilon )E({\sqrt {1-\varepsilon ^{2}}})+E(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})-K(\varepsilon )K({\sqrt {1-\varepsilon ^{2}}})={\tfrac {1}{2}}\pi

Because if the derivative of a continuous function constantly takes the value zero, then the concerned function is a constant function. This means that this function results in the same function value for each abscissa value $\varepsilon$ and the associated function graph is therefore a horizontal straight line.

References

Notes

↑ $K$ can be analytically extended to the complex plane.

References

1 2 3 Carlson 2010, 19.8.
↑ Borwein, Jonathan M.; Borwein, Peter B. (1987). Pi and the AGM: A Study in Analytic Number Theory and Computational Complexity (First ed.). Wiley-Interscience. ISBN 0-471-83138-7. p. 296
↑ Borwein, Jonathan M.; Borwein, Peter B. (1987). Pi and the AGM: A Study in Analytic Number Theory and Computational Complexity (First ed.). Wiley-Interscience. ISBN 0-471-83138-7. p. 298
↑ Chowla, S.; Selberg, A. (1949). "On Epstein's Zeta Function (I)". Proceedings of the National Academy of Sciences. 35 (7): 373. Bibcode:1949PNAS...35..371C. doi:10.1073/PNAS.35.7.371. PMC 1063041. PMID 16588908. S2CID 45071481.
↑ Chowla, S.; Selberg, A. (1967). "On Epstein's Zeta-Function". Journal für die Reine und Angewandte Mathematik. 227: 86–110.
↑ "Legendre elliptic integrals (Entry 175b7a)".
↑ N.Bagis,L.Glasser.(2015)"Evaluations of a Continued fraction of Ramanujan". Rend.Sem.Mat.Univ.Padova, Vol.133 pp 1-10
↑ "Complete elliptic integral of the second kind: Series representations (Formula 08.01.06.0002)".
↑ Borwein, Jonathan M.; Borwein, Peter B. (1987). Pi and the AGM: A Study in Analytic Number Theory and Computational Complexity (First ed.). Wiley-Interscience. ISBN 0-471-83138-7. p. 26, 161
↑ "Legendre-Relation" (in German). Retrieved 2022-11-29.
↑ "Legendre Relation". Retrieved 2022-11-29.
↑ "integration - Proving Legendres Relation for elliptic curves". Retrieved 2023-02-10.
↑ Internet Archive (1991), Paul Halmos celebrating 50 years of mathematics, New York : Springer-Verlag, ISBN 0-387-97509-8, retrieved 2023-02-10

Sources

Abramowitz, Milton; Stegun, Irene Ann, eds. (1983) [June 1964]. "Chapter 17". Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. Applied Mathematics Series. Vol. 55 (Ninth reprint with additional corrections of tenth original printing with corrections (December 1972); first ed.). Washington D.C.; New York: United States Department of Commerce, National Bureau of Standards; Dover Publications. p. 587. ISBN 978-0-486-61272-0. LCCN 64-60036. MR 0167642. LCCN 65-12253.
Byrd, P. F.; Friedman, M.D. (1971). Handbook of Elliptic Integrals for Engineers and Scientists (2nd ed.). New York: Springer-Verlag. ISBN 0-387-05318-2.
Carlson, B. C. (1995). "Numerical Computation of Real or Complex Elliptic Integrals". Numerical Algorithms. 10 (1): 13–26. arXiv:math/9409227. Bibcode:1995NuAlg..10...13C. doi:10.1007/BF02198293. S2CID 11580137.
Carlson, B. C. (2010), "Elliptic integral", in Olver, Frank W. J.; Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W. (eds.), NIST Handbook of Mathematical Functions, Cambridge University Press, ISBN 978-0-521-19225-5, MR 2723248.
Erdélyi, Arthur; Magnus, Wilhelm; Oberhettinger, Fritz; Tricomi, Francesco G. (1953). Higher transcendental functions. Vol II (PDF). McGraw-Hill Book Company, Inc., New York-Toronto-London. MR 0058756.
Gradshteyn, Izrail Solomonovich; Ryzhik, Iosif Moiseevich; Geronimus, Yuri Veniaminovich; Tseytlin, Michail Yulyevich; Jeffrey, Alan (2015) [October 2014]. "8.1.". In Zwillinger, Daniel; Moll, Victor Hugo (eds.). Table of Integrals, Series, and Products. Translated by Scripta Technica, Inc. (8 ed.). Academic Press, Inc. ISBN 978-0-12-384933-5. LCCN 2014010276.
Greenhill, Alfred George (1892). The applications of elliptic functions. New York: Macmillan.
Hancock, Harris (1910). Lectures on the Theory of Elliptic Functions. New York: J. Wiley & sons.
King, Louis V. (1924). On The Direct Numerical Calculation Of Elliptic Functions And Integrals. Cambridge University Press.
Press, W. H.; Teukolsky, S. A.; Vetterling, W. T.; Flannery, B. P. (2007), "Section 6.12. Elliptic Integrals and Jacobian Elliptic Functions", Numerical Recipes: The Art of Scientific Computing (3rd ed.), New York: Cambridge University Press, ISBN 978-0-521-88068-8

External links

"Elliptic integral", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
Eric W. Weisstein, "Elliptic Integral" (Mathworld)
Matlab code for elliptic integrals evaluation by elliptic project
Rational Approximations for Complete Elliptic Integrals (Exstrom Laboratories)
A Brief History of Elliptic Integral Addition Theorems

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[4] $K$ can be analytically extended to the complex plane.

[FOOTNOTECarlson201019.8-1] 1 2 3 Carlson 2010, 19.8.

[2] Borwein, Jonathan M.; Borwein, Peter B. (1987). Pi and the AGM: A Study in Analytic Number Theory and Computational Complexity (First ed.). Wiley-Interscience. ISBN 0-471-83138-7. p. 296

[3] Borwein, Jonathan M.; Borwein, Peter B. (1987). Pi and the AGM: A Study in Analytic Number Theory and Computational Complexity (First ed.). Wiley-Interscience. ISBN 0-471-83138-7. p. 298

[5] Chowla, S.; Selberg, A. (1949). "On Epstein's Zeta Function (I)". Proceedings of the National Academy of Sciences. 35 (7): 373. Bibcode:1949PNAS...35..371C. doi:10.1073/PNAS.35.7.371. PMC 1063041. PMID 16588908. S2CID 45071481.

[6] Chowla, S.; Selberg, A. (1967). "On Epstein's Zeta-Function". Journal für die Reine und Angewandte Mathematik. 227: 86–110.

[7] "Legendre elliptic integrals (Entry 175b7a)".

[8] N.Bagis,L.Glasser.(2015)"Evaluations of a Continued fraction of Ramanujan". Rend.Sem.Mat.Univ.Padova, Vol.133 pp 1-10

[9] "Complete elliptic integral of the second kind: Series representations (Formula 08.01.06.0002)".

[10] Borwein, Jonathan M.; Borwein, Peter B. (1987). Pi and the AGM: A Study in Analytic Number Theory and Computational Complexity (First ed.). Wiley-Interscience. ISBN 0-471-83138-7. p. 26, 161

[11] "Legendre-Relation" (in German). Retrieved 2022-11-29.

[12] "Legendre Relation". Retrieved 2022-11-29.

[13] "integration - Proving Legendres Relation for elliptic curves". Retrieved 2023-02-10.

[14] Internet Archive (1991), Paul Halmos celebrating 50 years of mathematics, New York : Springer-Verlag, ISBN 0-387-97509-8, retrieved 2023-02-10

[1]

[2]

[3]

[note 1]

[4]

[5]

[6]

[7]

[8]

[9]

[10]

[11]

[12]

[13]

Argument notation

Incomplete elliptic integral of the first kind

Incomplete elliptic integral of the second kind

Incomplete elliptic integral of the third kind

Complete elliptic integral of the first kind

Relation to the gamma function

Relation to Jacobi theta function

Asymptotic expressions

Differential equation

Continued fraction

Complete elliptic integral of the second kind

Computation

Derivative and differential equation

Complete elliptic integral of the third kind

Partial derivatives

Jacobi zeta function

Legendre's relation

Special identity for the lemniscatic case

Generalization for the overall case

See also

References

Notes

References

Sources

External links