Bessel functions: Difference between revisions

From SklogWiki
Jump to navigation Jump to search
(New page: '''Bessel functions''' of the first kind <math>J_n(x)</math> are defined as the solutions to the Bessel differential equation :<math>x^2 \frac{d^2y}{dx^2} + x\frac{dy}{dx} + (x^2-n^2)y=0...)
 
m (Added applications section.)
 
Line 7: Line 7:


:<math>J_n (z) = \frac{1}{2 \pi i} \oint e^{(z/2)(t-1/t)}t^{-n-1}{\rm d}t</math>
:<math>J_n (z) = \frac{1}{2 \pi i} \oint e^{(z/2)(t-1/t)}t^{-n-1}{\rm d}t</math>
 
==Applications in statistical mechanics==
*[[Computational implementation of integral equations]]
==See also==
==See also==
*[http://mathworld.wolfram.com/BesselFunctionoftheFirstKind.html Bessel Function of the First Kind -- from Wolfram MathWorld]
*[http://mathworld.wolfram.com/BesselFunctionoftheFirstKind.html Bessel Function of the First Kind -- from Wolfram MathWorld]
[[category: mathematics]]
[[category: mathematics]]

Latest revision as of 11:58, 7 July 2008

Bessel functions of the first kind Jn(x) are defined as the solutions to the Bessel differential equation

x2d2ydx2+xdydx+(x2−n2)y=0

which are nonsingular at the origin. They are sometimes also called cylinder functions or cylindrical harmonics. The Bessel function Jn(z) can also be defined by the contour integral

Jn(z)=12πi∮e(z/2)(t−1/t)t−n−1dt

Applications in statistical mechanics[edit]

See also[edit]