Solution to ECE Test #2 Su06 1. 2s ( s + 5) can be expressed in the form s2 + 9 x ( t ) = Aδ ( t ) + B cos ( at ) + C sin ( bt ) u ( t ) . The inverse Laplace transform of X ( s ) = Find numerical values for A, B, C, a and b. A = 2 , B = 10 , C = −0.6 , a = 3 , b = 3 . ) 2 s + 9 2 s + 10 s 2 2 2 s 2 + 18 10 s − 18 ⇒ X(s) = 2 + 10 s − 18 1.8 3 s = 2 + 10 2 − 2 s +9 s +9 3 s2 + 9 x ( t ) = 2δ ( t ) + 10 cos ( 3t ) − 0.6 sin ( 3t ) u ( t ) 2. The inverse Laplace transform of X ( s ) = 3s − 2 can be expressed in the form ( s + 4 )2 x ( t ) = A (1 + Bt ) eat u ( t ) . Find numerical values for A, B and a. A = 3 , B = −14 / 3 , a = −4 . X(s) = −14 (s + 4) 2 + ( ) 3 ⇒ x ( t ) = 3e−4 t − 14 te−4 t u ( t ) = ( 3 − 14 t ) e−4 t u ( t ) s+4 x ( t ) = 3(1 − (14 / 3) t ) e−4 t u ( t ) Alternate Solution: Start with 3 14 3s − 14 L 3 u ( t ) − 14 t u ( t ) ← → − 2 = s s s2 Let s → s + 4 . Then, using the complex-frequency shifting property, L x ( t ) = e−4 t 3 u ( t ) − 14 t u ( t ) = 3(1 − (14 / 3) t ) e− t u ( t ) ← → 3s − 2 ( s + 4 )2 = X(s) Second Alternate Solution: X(s) = ( 3s − 2 (s + 4) 2 = 3s (s + 4) 2 − 2 ( s + 4 )2 ) d 3s 2 L 3te−4 t u ( t ) + 3te−4 t u ( t ) t = 0− − 2te−4 t u ( t ) ← → 2 − dt ( s + 4 ) ( s + 4 )2 ( ) 3s 2 L 3 te−4 tδ ( t ) + u ( t ) −4 te−4 t + e−4 t − 2te−4 t u ( t ) ← → 2 − ( s + 4 ) ( s + 4 )2 L 3(1 − (14 / 3) t ) u ( t ) e−4 t ← → 3s (s + 4) 2 − 2 ( s + 4 )2 3. Given the Laplace-transform pair 3s 2 + 9 s − 14 x ( t ) ←→ s s 2 + 2 s + 10 L ( ) and the fact that x ( t ) is continuous at t = 0 , (a) Find the Laplace transform of d ( x ( t − 2 )) . dt d 3s 2 + 9 s − 14 L − x 0− x ( t )) ←→ s ( 2 dt s s + 2 s + 10 ( ( ) ( ) x 0− = x 0+ ( ) ) (from continuity at t = 0 ) From the initial-value theorem ( ) x 0 + = lim s s →∞ 3s 2 + 9 s − 14 =3 s s 2 + 2 s + 10 ( ) d 3s 2 + 9 s − 14 L ( x (t )) ←→ s 2 + 2 s + 10 − 3 dt 3s 2 + 9 s − 14 d L 2 ← → − 3 e−2 s x t − ( ) ( ) 2 dt s + 2 s + 10 (b) Find the numerical value of lim x ( t ) if it exists. If it does not exist explain t →∞ how you know that. Poles of s X ( s ) are at −1 ± j 3 in the open left half-plane. Therefore the final-value theorem applies. L lim x ( t ) ← → lim s t →∞ s→ 0 3s 2 + 9 s − 14 = −1.4 s s 2 + 2 s + 10 ( ) 4. In the standard feedback configuration (illustrated below), H1 ( s ) = K and s −1 4 . What numerical range of values of K makes the overall feedback s+5 system stable? H2 ( s) = X(s) E(s) H1(s) Y(s) H2(s) K K ( s + 5) s −1 H (s) = = 4K ( s − 1) ( s + 5 ) + 4 K 1+ ( s − 1) ( s + 5 ) For stability the poles must be in the open left half-plane. Poles are at ( s − 1) ( s + 5 ) + 4 K = 0 s2 + 4 s + 4 K − 5 = 0 ⇒ s = −4 ± 16 − 16 K + 20 −4 ± 36 − 16 K = 2 2 If K > 9 / 4 the poles are complex, the real parts are both -2, therefore in the open left half-plane and the system is stable. If K ≤ 9 / 4 the poles are real. If 36 − 16 K ≥ 16 then one real pole will be not be in the open left halfplane. This translates into 16 K ≤ 20 ⇒ K ≤ 5 / 4 . So, overall, for stability, K > 5 / 4 .