LECTURE 20: TRANSFORMS OF DERIVATIVES AND ODES MINGFENG ZHAO October 22, 2014 Proposition 1. There holds that I. Linearity: L[af (t) + bg(t)](s) = aL[f (t)](s) + bL[g(t)](s). That is, L−1 [aF (s) + bG(s)](t) = aL−1 [F (s)](t) + bL−1 [G(s)](t). II. First Shifting Property: L e−at f (t) (s) = L[f (t)](s + a). That is, L−1 [F (s + a)] (t) = e−at L−1 [F (s)](t). III. Transforms of derivatives: L[f 0 ](s) = sL[f ](s) − f (0) L[f 00 ](s) = s2 L[f ](s) − sf (0) − f 0 (0). Using the Heaviside function The Heaviside function: Let a be a constant, then 0, if t < a, ua (t) = 1, if t ≥ a. Proposition 2 (Second Shifting Property). For any constant a, then L[ua (t)f (t − a)](s) = e−as L[f (t)](s), 1 for all s > 0. 2 MINGFENG ZHAO That is, L−1 e−as F (s) = ua (t)L−1 [F (s)](t − a). Proof. By the definition of Laplace transform, we have Z ∞ L[ua (t)f (t − a)] = ua (t)f (t − a)e−st dt 0 Z ∞ f (t − a)e−st dt = By the definition of ua (t) a Z ∞ = 0 f (t0 )e−s(t +a) dt0 Let t − a = t0 0 = e −as = e −as Z ∞ 0 f (t0 )e−st dt0 0 L[f (t)], for all s > 0. Example 1. Solve x00 + x = f (t), x(0) = x0 (0) = 0, where 1, if 1 ≤ t < 5 f (t) = 0, otherwise. Let X(s) = L[x] and F (s) = L[f (t)], apply the Laplace transform on the both sides of x00 + x = f (t), then L[x00 ] + L[x] = L[f (t)] = F (s). Since x(0) = x0 (0) = 0, then L[x00 ] = s2 L[x] − sx(0) − x00 (0) = s2 X(s). So we get s2 X(s) + X(s) = F (s). That is, X(s) = F (s) . s2 + 1 For F (s) = L[f (t)], by the definition of f (t), we know that f (t) = u1 (t) − u5 (t), Then F (s) = L[f (t)] ∀t ≥ 0. LECTURE 20: TRANSFORMS OF DERIVATIVES AND ODES 3 = L[u1 (t)] − L[u5 (t)] e−s e−5s − . s s = So X(s) = F (s) e−s e−5s = − . s2 + 1 s(s2 + 1) s(s2 + 1) In orde to compute L−1 [X(s)], by the Second Shifting Property, we need to compute L−1 h 1 s(s2 +1) i . Use the method of partial fractions, we have 1 A Bs + C = + 2 . s(s2 + 1) s s +1 Then 1 = A(s2 + 1) + (Bs + C)s = (A + B)s2 + Cs + A. So A + B = 0, C = 0, and A = 1. Then B = −1. and C = 0. A = 1, Then 1 s 1 = − 2 . s(s2 + 1) s s +1 So we have −1 L 1 s(s2 + 1) −1 1 s −1 −L s s2 + 1 = L = 1 − cos(t) By looking the table. So we know that x(t) = L−1 [X(s)] e−s e−5s −1 = L−1 − L s(s2 + 1) s(s2 + 1) = u1 (t)[1 − cos(t − 1)] − u5 (t)[1 − cos(t − 5)], By the Second Shifting Property. Therefore, the solution to x00 + x = f (t), x(0) = x0 (0) = 0 is: x(t) = u1 (t)[1 − cos(t − 1)] − u5 (t)[1 − cos(t − 5)] . 4 MINGFENG ZHAO Transform of integrals Proposition 3 (Transform of integrals). There holds that Z t L[f (t)](s) f (τ ) dτ (s) = L . s 0 That is, L −1 Z t F (s) = L−1 [F (s)](τ ) dτ. s 0 t Z Proof. Let g(t) = f (τ ) dτ , by the Fundamental Theorem of Calculus, we know that 0 g(0) = 0, and g 0 (t) = f (t). Then we have Z L t f (τ ) dτ Z ∞ g(t) · e−st dt = L[g(t)] = 0 0 = = = ∞ Z 1 ∞ 0 1 −st g (t)e−st dt − e g(t) + s s 0 0 Z 1 ∞ 0 g (t)e−st dt s 0 Use the integration by parts L[f (t)] . s 1 . s(s2 + 1) By looking up the table, we have Example 2. Find L−1 L By the transform of integrals, we have −1 L −1 1 s(s2 + 1) 1 = sin(t). s2 + 1 " = −1 1 s2 +1 t s L Z L−1 = 0 Z = 1 (τ ) dτ s2 + 1 t sin(τ ) dτ 0 = # 1 − cos(t). LECTURE 20: TRANSFORMS OF DERIVATIVES AND ODES So L−1 Example 3. Solve t2 = Z 1 = 1 − cos(t) . s(s2 + 1) t eτ x(τ ) dτ . 0 Let X(s) = L[x(t)], apply the Laplace transform on the both sides of t2 = Z t eτ x(τ ) dτ , we have 0 L[t2 ] = L t Z eτ x(τ ) dτ . 0 By the transform of integrals, then Z t τ L e x(τ ) dτ = 0 = = L [et x(t)] s L[x(t)](s − 1) s X(s − 1) . s By the First Shifting Property By looking up the table, we have L[t2 ] = 2 . s3 Then 2 X(s − 1) = . s3 s Then X(s − 1) = 2 . s2 That is, X(s) = 2 . (s + 1)2 By the First Shifting Property, we have x(t) = L−1 [X(s)] = 2e−t t. Therefore, the solution to t2 = Z t eτ x(τ ) dτ is: 0 x(t) = 2e−t t . Convolution 5 6 MINGFENG ZHAO Definition 1. Let f (t) and g(t) be two functions on [0, ∞), the convolution of f and g is defined as: Z t (f ∗ g)(t) = f (τ )g(t − τ ) dτ. 0 Transform of Convolution Proposition 4. There holds that L[(f ∗ g)(t)] = L[f (t)] · L[g(t)]. That is, L−1 [F (s) · G(s)] = L−1 [F (s)] ∗ L−1 [G(s)]. Proof. In fact, we have Z L[f ∗ g] ∞ (f ∗ g)(t)e−st dt = 0 Z ∞ = e −st ∞ 0 Z ∞ e−st f (τ )g(t − τ ) dtdτ τ ∞ = ∞ Z f (τ ) 0 Z ∞ Z 0 f (τ ) g(t )e 0 Z g(t − τ )e−st dt dτ τ ∞ = = dt 0 = Z f (τ )g(t − τ ) dτ 0 Z t Z −s(t0 +τ ) 0 dt dτ Let t0 = t − τ 0 ∞ f (τ )e−sτ Z 0 ∞ 0 g(t0 )e−st dt0 dτ 0 Z = L[g(t)] · ∞ f (τ )e−sτ dτ 0 = L[f (t)] · L[g(t)]. Example 4. Let f (t) = et and g(t) = t for t ≥ 0, find f ∗ g and L[f ∗ g]. Department of Mathematics, The University of British Columbia, Room 121, 1984 Mathematics Road, Vancouver, B.C. Canada V6T 1Z2 E-mail address: mingfeng@math.ubc.ca