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Solving Recurrence Relations Using Differential Operators - Sections

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<strong>Using</strong> the intial values a0 = h(0) = 2 and a1 = h 0 (0) = 3 we get A = 5 and<br />

B = 2; hence<br />

h(x) = 5xe x + 2e x : (17)<br />

We now use the McLaurin series expansion of the right hand side of equation<br />

(14) to get<br />

1X 5n( 1)<br />

h(x) =<br />

n+1xn 1X 2( x)<br />

+<br />

n!<br />

n<br />

: (18)<br />

n!<br />

n=0<br />

n=0<br />

Thus an = 5n( 1) n+1 + 2( 1) n = ( 1) n ( 5n + 2).<br />

The following table shows several values of an.<br />

n 0 1 2 3 4<br />

an 2 3 8 13 18<br />

2.2 Di¤erential Operator: Example 2<br />

Consider the reccurence relation<br />

an+2 2an+1 + 2an = 0 where a0 = 1 and a1 = 0: (19)<br />

We begin by multipling the relation by xn<br />

n! and then sum it up from n = 0 to<br />

n = 1. Thus,<br />

1X<br />

n=0<br />

an+2x n<br />

n!<br />

By equations (9), (10), and (11)<br />

Hence,<br />

2<br />

1X<br />

n=0<br />

an+1x n<br />

n!<br />

+ 2<br />

1X anxn = 0: (20)<br />

n!<br />

n=0<br />

h 00 (x) 2h 0 (x) + 2h(x) = 0: (21)<br />

(D 2<br />

Completing the square, we get<br />

A general solution of this di¤erential equation is<br />

2D + 2I)h(x) = 0: (22)<br />

((D I) 2 + I)h(x) = 0: (23)<br />

h(x) = Ae x cos(x) + Be x sin(x): (24)<br />

Now using the initial conditions a0 = h(0) = 1 and a1 = h 0 (0) = 0 we get A = 1<br />

and B = 1, so<br />

h(x) = e x cos(x) e x sin(x): (25)<br />

Next we …nd the McLaurin series of the function h(x).<br />

4

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