ch06 - Solutions to Additional Problems 6.26. A signal x(t)...

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Solutions to Additional Problems 6.26. A signal x ( t ) has Laplace transform X ( s ) as given below. Plot the poles and zeros in the s -plane and determine the Fourier transform of x ( t ) without inverting X ( s ). (a) X ( s )= s 2 +1 s 2 +5 s +6 X ( s ( s + j )( s j ) ( s + 3)( s + 2) zeros at: ± j poles at: 3 , 2 X ( X ( s ) | s = = ω 2 +1 ω 2 +5 +6 Pole-Zero Map Real Axis Imag Axis -3.5 -3 -2.5 -2 -1.5 -1 -0.5 0 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Figure P6.26. (a) Pole-Zero Plot of X ( s ) (b) X ( s s 2 1 s 2 + s +1 X ( s ( s + 1)( s 1) ( s +0 . 5 j q 3 4 )( s . 5+ j q 3 4 ) zeros at: ± 1 1
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poles at: 1 ± j 3 2 X ( )= X ( s ) | s = = ω 2 1 ω 2 + +1 Pole-Zero Map Real Axis Imag Axis -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Figure P6.26. (b) Pole-Zero Plot of X ( s ) (c) X ( s 1 s 4 + 2 s 2 X ( s 3( s 10 3 ) ( s 4)( s 2) zero at: 10 3 poles at: 4 , 2 X ( X ( s ) | s = = 1 4 + 2 2 2
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Pole-Zero Map Real Axis Imag Axis 0 0.5 1 1.5 2 2.5 3 3.5 4 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Figure P6.26. (b) Pole-Zero Plot of X ( s ) 6.27. Determine the bilateral Laplace transform and ROC for the following signals: (a) x ( t )= e t u ( t + 2) X ( s Z −∞ x ( t ) e st dt = Z −∞ e t u ( t + 2) e st dt = Z 2 e t (1+ s ) dt = e 2(1+ s ) 1+ s ROC: Re(s) > -1 (b) x ( t u ( t + 3) X ( s Z 3 −∞ e st dt = e 3 s s ROC: Re(s) < 0 3
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(c) x ( t )= δ ( t + 1) X ( s Z −∞ δ ( t + 1) e st dt = e s ROC: all s (d) x ( t ) = sin( t ) u ( t ) X ( s Z 0 1 2 j ( e jt e ) e st dt = Z 0 1 2 j e t ( j s ) dt Z 0 1 2 j e t ( j + s ) dt = 1 2 j µ 1 j s 1 j + s = 1 (1 + s 2 ) ROC: Re(s) > 0 6.28. Determine the unilateral Laplace transform of the following signals using the deFning equation: (a) x ( t u ( t 2) X ( s Z 0 x ( t ) e st dt = Z 0 u ( t 2) e st dt = Z 2 e st dt = e 2 s s (b) x ( t u ( t + 2) X ( s Z 0 u ( t + 2) e st dt = Z 0 e st dt = 1 s (c) x ( t e 2 t u ( t + 1) 4
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X ( s )= Z 0 e 2 t u ( t + 1) e st dt = Z 0 e t ( s +2) dt = 1 s +2 (d) x ( t e 2 t u ( t + 2) X ( s Z 0 e 2 t u ( t + 2) e st dt = Z 2 0 e t (2 s ) dt = e 2(2 s ) 1 2 s (e) x ( t ) = sin( ω o t ) X ( s Z 0 1 2 j ( e o t e o t ) e st dt = 1 2 j · Z 0 e t ( o s ) dt Z 0 e t ( o + s ) dt ¸ = 1 2 j · 1 o s 1 o + s ¸ = ω o s 2 + ω 2 o (f) x ( t u ( t ) u ( t 2) X ( s Z 2 0 e st dt = 1 e 2 s s (g) x ( t ± sin( πt ) , 0 <t< 1 0 , otherwise X ( s Z 1 0 1 2 j ( e jπt e ) e st dt = π (1 + e s ) s 2 + π 2 5
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6.29. Use the basic Laplace transforms and the Laplace transform properties given in Tables D.1 and D.2 to determine the unilateral Laplace transform of the following signals: (a) x ( t )= d dt { te t u ( t ) } a ( t te t u ( t ) L u ←−−−→ A ( s 1 ( s + 1) 2 x ( t d dt a ( t ) L u X ( s s ( s + 1) 2 (b) x ( t tu ( t ) cos(2 πt ) u ( t ) a ( t tu ( t ) L u A ( s 1 s 2 b ( t ) = cos(2 ) u ( t ) L u s s 2 +4 π 2 x ( t a ( t ) b ( t ) L u X ( s A ( s ) B ( s ) X ( s 1 s 2 ( s 2 π 2 ) (c) x ( t t 3 u ( t ) a ( t tu ( t ) L u A ( s 1 s 2 b ( t ta ( t ) L u B ( s d ds A ( s 2 s 3 x ( t tb ( t ) L u X ( s d ds B ( s 6 s 4 (d) x ( t u ( t 1) e 2 t u ( t 1) a ( t u ( t ) L u A ( s 1 s b ( t a ( t 1) L u B ( s e s s c ( t e 2 t u ( t ) L u C ( s 1 s +2 d ( t e 2 c ( t 1) L u D ( s e ( s +2) s x ( t b ( t ) d ( t ) L u X ( s B ( s ) D ( s ) X ( s e 2( s +1) s ( s + 2) 6
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(e)
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This note was uploaded on 04/03/2010 for the course 전자전ê ELEC461-01 taught by Professor 배건성 during the Spring '10 term at 경북대학교.

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ch06 - Solutions to Additional Problems 6.26. A signal x(t)...

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