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Problems in Mathematical Analysis.pdf - pwp.net.ipl.pt

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.Sec. 16} Integration of Differential Equations by Power Series 361<br />

3091**. A shell leaves a gun with <strong>in</strong>itial velocity u at an<br />

angle a to the horizon. F<strong>in</strong>d the equation of motion if we take<br />

the air resistance as proportional to the velocity.<br />

3092*. A material po<strong>in</strong>t is attracted by a centre with a<br />

force proportional to the distance. The motion beg<strong>in</strong>s from po<strong>in</strong>t A<br />

at a distance a from the centre with <strong>in</strong>itial velocity perpen-<br />

dicular to OA. F<strong>in</strong>d the trajectory.<br />

Sec. 16. Integration of Differential Equations by Means of Power Series<br />

If it is not possible to <strong>in</strong>tegrate a differential equation with the help of<br />

elementary functions, then <strong>in</strong> some cases its solution may be sought <strong>in</strong> the<br />

form of a power series:<br />

00<br />

y=2 '(* *o) n - 0)<br />

n = o<br />

The undeterm<strong>in</strong>ed coefficients cn (n = \, 2, ...) are found by putt<strong>in</strong>g the<br />

series (1) <strong>in</strong>to the equation and equat<strong>in</strong>g the coefficients of identical powers<br />

of the b<strong>in</strong>omial x x on the left-hand and right-hand sides of the result<strong>in</strong>g<br />

equation.<br />

We can also seek the solution of the equation<br />

<strong>in</strong> the form of the Taylor's series<br />

y(*) = ^ y^^ (*-*)" (3)<br />

where y(x Q) = yQ , y' (x ) = f (* , t/ ) and the subsequent derivatives y (n) (x )<br />

(n- 2, 3, ...) are successively found by differentiat<strong>in</strong>g equation (2) and by<br />

putt<strong>in</strong>g X Q <strong>in</strong> place of x<br />

Example 1. F<strong>in</strong>d the solution of the equation<br />

Solution. We put<br />

y =<br />

whence, differentiat<strong>in</strong>g, we get<br />

y" = 2.\Ct + 3.2c sx+...+n(n-\)cn x n -* + (n+l<br />

+ In + 2)(rt-t-l)

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