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Lecture Notes in Differential Equations - Bruce E. Shapiro

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413<br />

The result<strong>in</strong>g equation is l<strong>in</strong>ear and<br />

y(t) =<br />

[ ( ∫ 1<br />

C +<br />

µ<br />

)] 1/(1−n)<br />

µ(t)(1 − n)q(t)dt<br />

where<br />

( ∫<br />

µ(t) = exp (1 − n)<br />

)<br />

p(t)dt<br />

Second Order Homogeneous L<strong>in</strong>ear Equation with Constant<br />

Coefficients<br />

To solve the differential equation<br />

ay ′′ + by ′ + cy = 0<br />

f<strong>in</strong>d the roots of the characteristic equation<br />

ar 2 + br + c = 0<br />

If the roots (real or complex) are dist<strong>in</strong>ct, then<br />

If the roots are repeated then<br />

y = Ae r1t + Be r2t<br />

y = (A + Bt)e rt<br />

Method of Undeterm<strong>in</strong>ed Coefficients<br />

To solve the differential equation<br />

ay ′′ + by ′ + cy = f(t)<br />

where f(t) is a polynomial, exponential, or trigonometric function, or any<br />

product thereof, the solution is<br />

y = y H + y P<br />

where y H is the complete solution of the homogeneous equation<br />

ay ′′ + by ′ + cy = 0

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