MATH 255 Lecture Notes - Lecture 9: Oliver Heaviside, Partial Fraction Decomposition, Step Function

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24 Apr 2015
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Solving odes by laplace transform (i) applying laplace transform to a second-order ode with constant coe - cients we obtain ax. + cx = f (t); a[s2x(s) sx(0) x (0)] + b[sx(s) x(0)] + cx(s) = f (s); where l{x(t)} = x(s);l{f (t)} = f (s). F (s) + a[sx(0) + x (0)] + bx(0) a[sx(0) + x as2 + bs + c (0)] + bx(0) as2 + bs + c. F (s) as2 + bs + c where x(0); x we need to take the inverse laplace transform (0) are given by initial conditions. To nd the solution of this equation, x(t) = l 1{x(s)}: } + l 1{ ax a[(s + b (0) + bx(0) 1 we can always use the convolution theorem. = l 1{f (s)} l 1{ as2 + bs + c. 0x = f (t); x(0) = 0; x (0) = 0; !0 d(cid:28): (ii) note that if f (t) = (cid:14)(t), then.

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