Math240 Elementary Differential Equations Fall 2003 Kansas State University Written Assignment #10: Laplace Transforms (solutions) 1. For this problem you may assume that the integral Γ(p) = Z∞ tp−1 e−t dt converges 0 whenever p > 0. (a) Use integration by parts to show that Γ(p + 1) = pΓ(p) for every p > 0. Solution From the defintion of the Gamma function Zb Zb ¯b ¯ Γ(p + 1) = lim tp e−t dt = lim −tp e−t ¯ + p tp−1 e−t dt . b→∞ b→∞ 0 0 0 Since p > 0, the limit as b → ∞ of the first term is 0. Thus Γ(p + 1) = p Z∞ tp−1 e−t dt = pΓ(p). 0 (b) Compute Γ(6). Solution We could plug 6 into the definition of the Gamma function and integrate by parts 5 times. It is easier, however, to just use the result in (a). Γ(6) = Γ(5+1) = 5Γ(5) = 5Γ(4+1) = 5·4Γ(4) = · · · = 5·4·3·2·1Γ(1). Hence Γ(6) = 120 Z∞ e −t ¤ ¯¯b dt = 120 lim −e ¯ = 120 . b→∞ 0 £ −t 0 (c) Using the definition of the Laplace transform, establish the formula L {ta } = Γ(a + 1) sa+1 for every a > −1. Solution u For this, we will use the substitution u = ts, which implies t = and s 1 a dt = du. Plugging t into the definition of the Laplace transform s yields L {ta } = t=∞ Z ta e−st dt = t=0 = Γ(a + 1) . sa+1 u=∞ Z u=0 ³ u ´a s e−u µ 1 du s ¶ = 1 sa+1 Z∞ 0 u(a+1)−1 e−u du n (d) Find L t − 21 o . Note that Γ( 21 ) = √ π. (e) Apply part(a) to show that Γ(n + 1) = n! whenever n is a nonnegative integer. Solution Note that Γ(1) = 1, so part (a) implies Γ(n + 1) = nΓ(n) = nΓ((n − 1) + 1) = n · (n − 1)Γ(n − 1) = . . . = n(n − 1)(n − 2) · · · 2 · 1 · Γ(1) = n(n − 1)(n − 2) · · · 2 · 1 = n!. 2. Establish the following four transforms. f (t) = L−1 {F (s)} F (s) = L {f (t)} eat cosh(bt) s−a (s − a)2 − b2 eat sinh(bt) b (s − a)2 − b2 tn cosh(bt), n a positive integer n! (s + b)n+1 + (s − b)n+1 · 2 (s2 − b2 )n+1 tn sinh(bt), n a positive integer n! (s + b)n+1 − (s − b)n+1 · 2 (s2 − b2 )n+1 ¡ ¢ ¡ ¢ Recall that cosh(bt) = 12 ebt + e−bt and sinh(bt) = 21 ebt − e−bt . Solution Using the definition of cosh(bt) and the table on page 139 in the text · ¸ © at ª 1 © (a+b)t ª 1 © (a−b)t ª 1 1 1 L e cosh(bt) = L e + L e = + 2 2 2 s − (a + b) s − (a − b) · ¸ 1 s − (a − b) + s − (a + b) s−a = = . 2 ((s − a) − b)((s − a) + b) (s − a)2 − b2 Similarly · ¸ 1 1 © (a+b)t ª 1 © (a−b)t ª 1 1 L e sinh(bt) = L e − L e = − 2 2 2 s − (a + b) s − (a − b) · ¸ 1 s − (a − b) − s + (a + b) b = = . 2 ((s − a) − b)((s − a) + b) (s − a)2 − b2 © at ª Again using the table on page 139, we have · ¸ n! n! 1 © n bt ª 1 © n −bt ª 1 = + L {t cosh(bt)} = L t e + L t e 2 2 2 (s − b)n+1 (s + b)n+1 ¸ · n! (s + b)n+1 + (s − b)n+1 n! (s + b)n+1 + (s − b)n+1 = = · . 2 (s − b)n+1 (s + b)n+1 2 (s2 − b2 )n+1 n Finally, ¸ · n! n! 1 © n bt ª 1 © n −bt ª 1 = − L {t sinh(bt)} = L t e − L t e 2 2 2 (s − b)n+1 (s + b)n+1 · ¸ n! (s + b)n+1 − (s − b)n+1 n! (s + b)n+1 − (s − b)n+1 = = · . 2 (s − b)n+1 (s + b)n+1 2 (s2 − b2 )n+1 n