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In [[mathematics]], '''Struve functions''' <math>\mathbf{H}_\alpha(x)</math>, are  solutions ''y''(''x'') of the non-homogenous [[Bessel's differential equation]]:


: <math>x^2 \frac{d^2 y}{dx^2} + x \frac{dy}{dx} + (x^2 - \alpha^2)y = \frac{4{(x/2)}^{\alpha+1}}{\sqrt{\pi}\Gamma(\alpha+\frac{1}{2})}</math>


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introduced by {{harvs|txt|last=Struve|first=Hermann|authorlink=Hermann Struve|year=1882}}.
The [[complex number]] α is  the '''order''' of the Struve function, and is often an integer.
The '''modified Struve functions''' <math>\mathbf{L}_\alpha(x)</math> are equal to
<math>-i e^{-i\alpha \pi /2} \mathbf{H}_\alpha(ix)</math>.
 
==Definitions==
 
Since this is a [[Ordinary differential equation#Nonhomogeneous equations|non-homogenous]] equation,  
solutions can be constructed from a single particular solution by adding the solutions of the homogeneous problem.
In this case, the homogenous solutions are the [[Bessel function]]s, and the particular solution may be chosen as the corresponding Struve function.
 
===Power series expansion===
 
Struve functions, denoted as <math>\mathbf{H}_\alpha(x)</math> have the following power series form
 
:<math> \mathbf{H}_\alpha(x) =
  \sum_{m=0}^\infty \frac{(-1)^m}{\Gamma(m+\frac{3}{2}) \Gamma(m+\alpha+\frac{3}{2})}
                                  {\left({\frac{x}{2}}\right)}^{2m+\alpha+1} </math>
 
where <math>\Gamma(z)</math> is the [[gamma function]].
 
The modified Struve function, denoted as <math>\mathbf{L}_{\nu}(z)</math> have the following power series form
 
:<math> \mathbf{L}_{\nu}(z) = {\left({\frac{z}{2}}\right)}^{\nu+1}
  \sum_{k=0}^\infty \frac{1}{\Gamma(\frac{3}{2}+k) \Gamma(\frac{3}{2}+k+\nu)}
                                  {\left({\frac{z}{2}}\right)}^{2k} </math>
 
===Integral form===
 
Another definition of the Struve function, for values of α satisfying <math>\operatorname{Re}\{ \alpha \} > -1/2</math>, is possible using an integral representation:
 
:<math>\mathbf{H}_\alpha(x) =
      \frac{2{(x/2)}^{\alpha}}{\sqrt{\pi}\Gamma(\alpha+\frac{1}{2})}
      \int_{0}^{\pi/2} \sin (x \cos \tau)\sin^{2\alpha}(\tau) d\tau.</math>
 
==Asymptotic forms==
 
For small x, the power series expansion is given [[#Power series expansion|above]].
 
For large x, one obtains:
 
:<math>\mathbf{H}_\alpha(x) - Y_\alpha(x) \rightarrow
      \frac{1}{\sqrt{\pi}\Gamma(\alpha+\frac{1}{2})} {\left(\frac{x}{2}\right)}^{\alpha-1}
      + O\left({(x/2)}^{\alpha-3}\right) </math>
 
where <math>Y_\alpha(x)</math> is the
[[Bessel function#Bessel functions of the second kind : Y.CE.B1|Neumann function]].
 
==Properties==
 
The Struve functions satisfy the following recurrence relations:
 
:<math>
\mathbf{H}_{\alpha -1}(x) + \mathbf{H}_{\alpha+1}(x) =
  \frac{2\alpha}{x} \mathbf{H}_\alpha (x) + \frac{{(x/2)}^\alpha}{\sqrt{\pi}\Gamma(\alpha + \frac{3}{2})}
</math>
 
:<math>
\mathbf{H}_{\alpha -1}(x) - \mathbf{H}_{\alpha+1}(x) =
  2\frac{\mathrm{d}\mathbf{H}_\alpha}{\mathrm{d}x}  -
  \frac{{(x/2)}^\alpha}{\sqrt{\pi}\Gamma(\alpha + \frac{3}{2})}.
</math>
 
==Relation to other functions==
Struve functions of integer order can be expressed in terms of [[Anger function|Weber function]]s '''E'''<sub>''n''</sub> and vice versa: if ''n'' is a non-negative integer then
:<math>\mathbf{E}_n(z)=\frac{1}{\pi} \sum_{k=0}^{[\frac{n-1}{2}]}\frac{\Gamma(k+1/2)(z/2)^{n-2k-1}}{\Gamma(n-1/2-k)}\mathbf{H}_n </math>
:<math>\mathbf{E}_{-n}(z)=\frac{(-1)^{n+1}}{\pi}\sum_{k=0}^{[\frac{n-1}{2}]} \frac{\Gamma(n-k-1/2)(z/2)^{-n+2k+1}}{\Gamma(k+3/2)}\mathbf{H}_{-n}. </math>
 
Struve functions of  order ''n''+1/2 (''n'' an integer) can be expressed in terms of elementary functions. In particular if ''n'' is a non-negative integer then
:<math>\mathbf{H}_{-n-1/2}(z) = (-1)^nJ_{n+1/2}(z)</math>
where the right hand side is a [[spherical Bessel function]].  
 
Struve functions (of any order) can be expressed in terms of the [[generalized hypergeometric function]] <sub>1</sub>F<sub>2</sub> (which is '''not''' the  Gauss hypergeometric function <sub>2</sub>F<sub>1</sub>) :
:<math>\mathbf{H}_{\alpha}(z) = \frac{(z/2)^{\alpha+1/2}}{\sqrt{2\pi}\Gamma(\alpha+3/2)}{}_1F_2(1,3/2,\alpha+3/2,-z^2/4).</math>
 
==References==
*{{cite journal|doi=10.1121/1.1564019|author=R.M. Aarts and Augustus J.E.M. Janssen|title=Approximation of the Struve function H1 occurring in impedance calculations|journal= J. Acoust. Soc. Am. |volume= 113 |pages= 2635–2637 |year= 2003|pmid=12765381|issue=5|bibcode = 2003ASAJ..113.2635A }}
*{{AS ref|12|496}}
*{{springer|id=S/s090700|first=A.B. |last=Ivanov}}
*{{dlmf|id=11|Struve and Related Functions|first=R. B. |last=Paris}}
*{{cite journal|doi=10.1002/andp.18822531319 |first=H. |last=Struve |title=Beitrag zur Theorie der Diffraction an Fernröhren |journal= Ann. Physik Chemie |volume= 17|issue=13 |year=1882 |pages= 1008–1016|bibcode = 1882AnP...253.1008S }}
 
==External links==
*[http://functions.wolfram.com/Bessel-TypeFunctions/StruveH/introductions/Struves/ Struve functions] at [http://functions.wolfram.com the Wolfram functions site].
 
{{DEFAULTSORT:Struve Function}}
[[Category:Special functions]]
[[Category:Struve family]]

Revision as of 01:40, 25 October 2013

In mathematics, Struve functions Hα(x), are solutions y(x) of the non-homogenous Bessel's differential equation:

x2d2ydx2+xdydx+(x2α2)y=4(x/2)α+1πΓ(α+12)

introduced by Template:Harvs. The complex number α is the order of the Struve function, and is often an integer. The modified Struve functions Lα(x) are equal to ieiαπ/2Hα(ix).

Definitions

Since this is a non-homogenous equation, solutions can be constructed from a single particular solution by adding the solutions of the homogeneous problem. In this case, the homogenous solutions are the Bessel functions, and the particular solution may be chosen as the corresponding Struve function.

Power series expansion

Struve functions, denoted as Hα(x) have the following power series form

Hα(x)=m=0(1)mΓ(m+32)Γ(m+α+32)(x2)2m+α+1

where Γ(z) is the gamma function.

The modified Struve function, denoted as Lν(z) have the following power series form

Lν(z)=(z2)ν+1k=01Γ(32+k)Γ(32+k+ν)(z2)2k

Integral form

Another definition of the Struve function, for values of α satisfying {α}>1/2, is possible using an integral representation:

Hα(x)=2(x/2)απΓ(α+12)0π/2sin(xcosτ)sin2α(τ)dτ.

Asymptotic forms

For small x, the power series expansion is given above.

For large x, one obtains:

Hα(x)Yα(x)1πΓ(α+12)(x2)α1+O((x/2)α3)

where Yα(x) is the Neumann function.

Properties

The Struve functions satisfy the following recurrence relations:

Hα1(x)+Hα+1(x)=2αxHα(x)+(x/2)απΓ(α+32)
Hα1(x)Hα+1(x)=2dHαdx(x/2)απΓ(α+32).

Relation to other functions

Struve functions of integer order can be expressed in terms of Weber functions En and vice versa: if n is a non-negative integer then

En(z)=1πk=0[n12]Γ(k+1/2)(z/2)n2k1Γ(n1/2k)Hn
En(z)=(1)n+1πk=0[n12]Γ(nk1/2)(z/2)n+2k+1Γ(k+3/2)Hn.

Struve functions of order n+1/2 (n an integer) can be expressed in terms of elementary functions. In particular if n is a non-negative integer then

Hn1/2(z)=(1)nJn+1/2(z)

where the right hand side is a spherical Bessel function.

Struve functions (of any order) can be expressed in terms of the generalized hypergeometric function 1F2 (which is not the Gauss hypergeometric function 2F1) :

Hα(z)=(z/2)α+1/22πΓ(α+3/2)1F2(1,3/2,α+3/2,z2/4).

References

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External links