Chapter 7 - Lecture notes 7 PDF

Title Chapter 7 - Lecture notes 7
Course Differential Equations and Linear Algebra
Institution San José State University
Pages 17
File Size 295.7 KB
File Type PDF
Total Downloads 69
Total Views 211

Summary

Lecture notes with example practice for chapter 7...


Description

CHAPTER 7: POWER SERIES SOLUTION ABOUT AN ORDINARY POINT Suppose the DE a2(x)y + a1(x)y + a0y = 0  (*) has no solution that is expressible as a finite linear combination of known element function. Question 1 Does it have a power series solution of the form 

 C n (x – x0)n

n 0

Question 2 Under what conditions can we be certain that it does have such a solution? To answer these questions, we need to introduce certain basic definitions. First, let us write the DE (*) in the form y’’ + P(x)y’ + Q(x)y = 0  (**) where a1 ( x ) a 0 (x) , Q(x) = P(x) = a 2 (x) a 2 (x) Definition: 1. A function f is said to be analytic at x0 if its Taylor series about x0, (n)  f (x 0 ) (x – x0)n  n ! n 0 exist and converge to f(x) for all x in some open interval containing x0. 2.

The point x0 is called an ordinary point of (*) if both P(x) and Q(x) are analytic at x0. If either or both of these functions is not analytic at x 0, then x0 is called a singular point of (*).

#

For a LDE an(x)y(n) + … + a0(x)y = g(x) with polynomial coefficients, the point x = x0 is called ordinary point if an(x0)  0. A singular point is any point x = x1 for which an(x1) = 0

e.g.1 y’’+ xy’+ (x2+2)y = 0 P(x) =x, Q(x)= x2+2 are polynomial. So they are analytic everywhere. Thus all points are ordinary points of this DE.

y =0 x

e.g.2 (x-1)y’’ +xy’ +

y’’+ (

P(x) =

1 x )y’+ y= 0 x 1 x( x  1) 1 x , Q(x) = ( x x  1) x 1

P(x) is analytic except x=1 Q(x) is analytic except at x=0 and x=1 So x=0 and x=1 are singular point. Solution About Ordinary Point We can now state a theorem concerning the existence of power series solution for (**). THEOREM If x = x0 is an ordinary point of the DE (**), then the DE(**) has two nontrivial linear independent power series solutions of the form 

 C n (x – x0)n

n 0

and these power series converge in some interval x – x0 <  (where  > 0) about x. Remarks If x0 is an ordinary point of (**), then we can write the general solution of (**) as a liner combination of these two linear independent power series. e.g.1 use the power series method to solve DE y’=y ------(1) solution: 

assume that y=



anxn

n 1



y’=  n anxn-1 n 1

substitute this into (1) 

 n 1

i.e.



anxn =

 n anxn-1 n 1

a1=a0 2a2=a1=a0 3a3=a2

a2=a0/2=a0/2! a3=a0/3x2=a0/3!

kak=ak-1 

y=

ak=a0/k!

 1 a0x =a0 (  n! n 0



n 0

xn ) n!

y=a0ex eg 2. we know that all the real numbers are ordinary points of theDE y’’+xy”+(x2+2)y=0 so the DE has two linear independent power series solutions about any point x0. that is the general solution of this DE has the form 



y=A

k 0



ak(x-x0)n + B  bk(x-x0)n k 0

where x0 is any real number and ak and bk eg 3. The DE y’’+

1 x y’+ y =0 has two singular points x=0 x ( x  1) x 1

and x=1. so this DE has two linear independent power series solutions of the form 



cn(x-x0)n

n 0

about any point x0 not equal to 0, 1 for example, it has 2 linear independent power series solutions of the form 



cn(x-2)n

n 0

eg 4. Find the power series solution of the DE y’’+xy’+(x2+2)=0-------(1) in power of x. solution: x0=0 is an ordinary point of the DE. Assume 

y=



cnxn

n 0



y’=



ncnxn-1

n 1



y’’=



n(n-1)cnxn-2

n 2

substitute these into (1)



 n 2



n(n-1)cnxn-2 +x  ncnxn-1 + x2 n 1







 n 0

n 0



ncnxn +



cnxn =0



cn-2xn +

n 2

n 1

 n 0





(n+2)(n+2)cn+2 xn +



cnxn + 2



2cnxn =0

n 0





[ (n+2)(n+2)cn+2 + (n+2)cn + cn-2] xn + (2c2 +6c3x) +c1x +(2c0+2c1x)=0

n 0

So

2c2 +2c0 =0 or c2 =-c0 6c3+3c1=0 or c3=-0.5c1 (n+2)(n+1)cn+2 +(n+2)cn +cn-2 =0 ; n 2

(n  2)Cn  Cn  2 ; n 2 (n  1)(n  2) 4C 2  C 0 3C 0 1 C4 == = C0 3X 4 12 4 5C 3  C 1 3 C5 == C1 4X5 40 1 3 6  y= C0 (1-x2 + 1 x4 +……..)+C1(x- x3 + x +…….) 4 2 40

Cn+2 = -

Eg 5. Find a power series solution of the IVP (x2 -1)y’’ +3xy’ +xy =0------(1), y(0)=4, y’(0)=6 Solution: All points except x=1,-1 are ordinary points. So we can assume a general solution of the form 



cn(x-x0)n

n 0

Since we are interested in the solution at x=0, we take x0 =0. 

Assume y=



cnxn

n 0



y’=



ncnxn-1

n 1



y’’=



n(n-1)cnxn-2

n 2

substitude into (1) 





n(n-1)cnxn -

n 2

 n 2





n 1

n 0

n(n-1)cnxn-2 +3  ncnxn +  cnxn+1 =0 

-2C2 + (C0+3C1-6C3)x+  [-(n+2)(n+1)Cn+2 +n(n+2)Cn +Cn-1]xn =0 n 2

-2C2 =0

C0 +3C1-6C3=0 -(n+2)(n+1)Cn+2 +n(n+2)Cn +Cn-1 =0 ; n 2 1 1 C0 + C1 6 2 n(n  2)Cn  Cn  1 Cn+2 = ; n 2 ( n  1)( n  2) 1 8C 2  C1 = C1 C4 = 12 12 3 15C3  C 2 1 C5 = = C0 + C1 20 8 8 1 1 1 1 4 3 5 y=C0(1+ x3+ x5+…….)+ C1(x+ x3+ x + x +…….) 6 8 2 12 8 1 2 3 4 3 2 y’= C0( x + x +……)+C1(1+ x +…….) 2 8 2

C2 =0, C3=

y(0)=4  C0=4 y’(0)=6  C1=6

 y= 4(1+ 1

1 5 1 1 4 3 5 x +…….)+ 6(x+ x3+ x + x +…….) 6 8 2 12 8 11 3 1 4 =4+6x+ x + x +……. 3 2

x3+

Solution Around Singular Points Consider the DE a2(x)y + a1(x)y + a0y = 0  (*) Let x0 be a singular point of (*) Question: What type of solution can we expect? It turns out that under certain conditions we are justified in assuming a solution of the form n r y =  C n ( x  x 0 ) n 0

where r is a constant that must be determined. Thus, it is necessary to classify singular point as follow: Rewrite (6.3) as y + P(x)y + Q(x)y = 0  (**) a1 ( x ) a 0 (x) where P(x) = , Q(x) = a 2 (x) a 2 (x) Definition A singular point x0 of equation (**) is said to be a regular singular point if both (x – x0)P(x) and (x – x0)2 Q(x) are analytic at x0 that means both (x – x0)P(x) and (x – x0) Q(x) have a power series solution in (x – x0) with a positive radius of convergence.

A singular point that is not regular is said to be an irregular singular point of the equation. 2x2y’’-xy’+(x-5)=0

eg 1.

1 x 5 y’+ y=0 2x 2x 2 1 x 5 P(x)=, Q(x)= 2x 2x 2

y’’-

1. P,Qare not analytic at x=0, so x=0 is a singular point. 2. xP(x) =-

1 x 5 and x2Q(x)= are analytic at x=0. 2 2

x=0 is a regular singular point.

Eg 2. x2(x-2)2y’’ +2(x-2)y’ +(x+1)y=0 x 1 2 y’ + y=0 x 2(x  2) x 2 ( x  2 )2 2 x 1 P(x)= 2( , Q(x)= x x  2) x 2(x  2)2

y’’+

1. P,Q are not analytic at x=0, x=2, so x=0,2 are singular points. For x=0, 2

is not analytic at x=0, so x=0 is an irregular singular point. x P(x)= ( x x  2) For x=2, (x-2) P(x)=

2 x 1 are analytic at x=2. , (x-2)2 Q(x)= x2 x2

x=2 is a regular singular point.

To solve the DE (1) a2(x)y’’+a1(x)y’+a0y=0 about a regular singular point, we shall state the following theoem. THEOREM 1 (The Method of Frobenius) If x = x0 is a regular singular point of equation (1), then there exists at least one nontrivial solution of the form 

y = (x – x0)r  C n (x – x0)n n 0



=  C n (x – x0)n + r n 0

where r is a definite constant which may be determined. This solution is valid in some selected interval 0 < x – x0 <  (where  > 0) about x0. Eg 1. 2x2y’’-xy’+(x-5)=0 X=0 is a regular singular point Theorem 1 state that this DE has at least one solution of 

the form, xr  Cnxn n 0

Valid in some selected interval 0<

x...


Similar Free PDFs