Mathematical Methods for Physics and Engineering : A Comprehensive Guide

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SERIES SOLUTIONS OF ORDINARY DIFFERENTIAL EQUATIONS


singular points, whereas any singular point not satisfying both these criteria is


termed anirregularoressentialsingularity.


Legendre’s equation has the form

(1−z^2 )y′′− 2 zy′+(+1)y=0, (16.8)
whereis a constant. Show thatz=0is an ordinary point andz=± 1 are regular singular
points of this equation.

Firstly, divide through by 1−z^2 to put the equation into our standard form (16.7):


y′′−

2 z
1 −z^2

y′+

(+1)


1 −z^2

y=0.

Comparing this with (16.7), we identifyp(z)andq(z)as


p(z)=

− 2 z
1 −z^2

=


− 2 z
(1 +z)(1−z)

,q(z)=

(+1)


1 −z^2

=


(+1)


(1 +z)(1−z)

.


By inspection,p(z)andq(z) are analytic atz= 0, which is therefore an ordinary point,
but both diverge forz=±1, which are thus singular points. However, atz=1wesee
that both (z−1)p(z)and(z−1)^2 q(z) are analytic and hencez= 1 is a regular singular
point. Similarly, atz=−1 both (z+1)p(z)and(z+1)^2 q(z) are analytic, and it too is a
regular singular point.


So far we have assumed thatz 0 is finite. However, we may sometimes wish to

determine the nature of the point|z|→∞. This may be achieved straightforwardly


by substitutingw=1/zinto the equation and investigating the behaviour at


w=0.


Show that Legendre’s equation has a regular singularity at|z|→∞.

Lettingw=1/z, the derivatives with respect tozbecome


dy
dz

=


dy
dw

dw
dz

=−


1


z^2

dy
dw

=−w^2

dy
dw

,


d^2 y
dz^2

=


dw
dz

d
dw

(


dy
dz

)


=−w^2

(


− 2 w

dy
dw

−w^2

d^2 y
dw^2

)


=w^3

(


2


dy
dw

+w

d^2 y
dw^2

)


.


If we substitute these derivatives intoLegendre’s equation (16.8) we obtain
(
1 −


1


w^2

)


w^3

(


2


dy
dw

+w

d^2 y
dw^2

)


+2


1


w

w^2

dy
dw

+(+1)y=0,

which simplifies to give


w^2 (w^2 −1)

d^2 y
dw^2

+2w^3

dy
dw

+(+1)y=0.

Dividing through byw^2 (w^2 −1) to put the equation into standard form, and comparing
with (16.7), we identifyp(w)andq(w)as


p(w)=

2 w
w^2 − 1

,q(w)=

(+1)


w^2 (w^2 −1)

.


Atw=0,p(w) is analytic butq(w) diverges, and so the point|z|→∞is a singular point
of Legendre’s equation. However, sincewpandw^2 qare both analytic atw=0,|z|→∞
is a regular singular point.

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