The Chemistry Maths Book, Second Edition

(Grace) #1

13.3 The Frobenius method 373


EXAMPLE 13.3Indicial equations


(i)


We haveb


0

1 = 1 − 122 ,c


0

1 = 1122 , and the indicial equation isr


2

1 − 13 r 221 + 11221 = 10 with


rootsr


1

1 = 11 andr


2

1 = 1122.


(ii)x


2

y′′ 1 + 1 xy′ 1 + 1 (x


2

1 − 112 4)y 1 = 10


This is the Bessel equation (see Table 13.1) forn 1 = 1122. We haveb(x) 1 = 111 = 1 b


0

and


c(x) 1 = 1 x


2

1 − 1124 so thatc


0

1 = 1 − 124. Thenr


2

1 − 11241 = 1 (r 1 − 112 2)(r 1 + 112 2) 1 = 10 and the


indicial parameters arer 1 = 1 ± 12 2.


(iii)xy′′ 1 + 12 y′ 1 + 14 xy 1 = 10


We havex


2

y′′ 1 + 12 xy′ 1 + 14 x


2

y 1 = 10. Therefore,b(x) 1 = 121 = 1 b


0

and c(x) 1 = 1 x


2

so that


c


0

1 = 10. The indicial equation isr


2

1 + 1 (b


0

1 − 1 1)r 1 + 1 c


0

1 = 1 r


2

1 + 1 r 1 = 10 , with rootsr


1

1 = 10


andr


2

1 = 1 −1.


0 Exercises 6–9


Once the values of the indicial parameter have been determined, the solution of


the differential equation can proceed as in the power-series method. The general


solution is


y(x) 1 = 1 c


1

y


1

(x) 1 + 1 c


2

y


2

(x) (13.9)


in which c


1

and c


2

are arbitrary constants, andy


1

(x)andy


2

(x)are independent


particular solutions. At least one of y


1

and y


2

has the form (13.4), and the other


depends on the solutions,r


1

andr


2

, of the indicial equation. We have the following


three cases.


1 Distinct roots not differing by an integer


Bothy


1

andy


2

have the form (13.4),


y


1

(x) 1 = 1 x


r

1

(a


0

1 + 1 a


1

x 1 + 1 a


2

x


2

1 +1-) (13.10a)


y


2

(x) 1 = 1 x


r

2

(A


0

1 + 1 A


1

x 1 + 1 A


2

x


2

1 +1-) (13.10b)


2 Double root


Ifr


1

1 = 1 r


2

1 = 1 r, one solution has the form (13.4),


y


1

(x) 1 = 1 x


r

(a


0

1 + 1 a


1

x 1 + 1 a


2

x


2

1 +1-) (13.11a)


and the second solution is


y


2

(x) 1 = 1 y


1

(x) 1 ln 1 x 1 + 1 x


r+ 1

(A


0

1 + 1 A


1

x 1 + 1 A


2

x


2

1 +1-) (13.11b)


xy xy y


2

1


2


1


2


′′− ′+= 0

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