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19.8 Bessel’s equation and Bessel functions 587

19.8 BESSEL’SEQUATIONANDBESSELFUNCTIONS

Alineardifferentialequationthathasimportantapplicationsinthetheoryofwavepropagation,

particularly when using cylindrical or spherical polar coordinates, is known as

Bessel’sequation.InfactthetermBessel’sequationrepresentsawholefamilyofequations

having the form

x 2d2 y

dx +xdy 2 dx +(x2 −v 2 )y=0.

Herexandyaretheindependentvariableanddependentvariablerespectively.Thethird

quantity v,termedaparameter,isknownastheorderoftheequation. 1 Aswevarythe

parameter v we obtain the family of differential equations. Note that v can be any real

number. In Sections 19.8.1 and 19.8.2 we will solve Bessel’s equation when v = 0 and

v = 1.Intheengineeringapplicationswhichfollowlaterinthechapteryouwillseethat

v may be other integers including those that are negative. Observe that the equation is

linearandhomogeneous,butitdoesnothaveconstantcoefficients:thecoefficientof d2 y

dx 2

isx 2 , a function of the independent variable. In what follows we show that solutions of

Bessel’sequationcanbefoundintheformofinfinitepowerserieswhichwecallBessel

functions.

Bessel functions have many applications in physics and engineering. In electrical

engineeringtheyarecommonlyusedinthefieldofcommunications.Theyareimportant

in finding the bandwidth and frequency content of some radio signals. They are also

essentialintheanalysisofpropagatingmodesincylindricalwaveguidesandcylindrical

cavityresonators,bothofwhichareimportantdevicesusedinhighfrequencymicrowave

engineering(seeEngineeringapplication19.12).Besselfunctionsarealsoutilisedinthe

design of filters.

19.8.1 Bessel’sequationoforderzero

To introduce the solution of Bessel’s equation and thereby introduce a Bessel function

the following example deals with the specialcase when v = 0.

Example19.31 By seeking a power series solution in the form

∞∑

a m

x m obtain the first four non-zero

termsinapower series solution ofBessel’s equation inthe specialcase when v = 0.

Solution When v = 0 Bessel’s equation is:

x 2d2 y

dx +xdy 2 dx +x2 y=0.

which fornon-zeroxbecomes

x d2 y

dx + dy +xy=0. (19.25)

2 dx

m=0

1 Note that in this context the word ‘order’ means something different from the order of a differential

equation, which wasdefined in 19.2.1.

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