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Solutions to Sample Exam 2: A Second Order Linear Differential Equation, Exams of Electronic Circuits Analysis

The solutions to problem 2 of a sample exam, which involves finding the particular and homogeneous solutions to a second order linear differential equation, as well as the system response and zero-state response.

Typology: Exams

2012/2013

Uploaded on 04/16/2013

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Sample Exam 2: Solutions
#1) We use the time invariance principle and first find the solution to
0,0)0(),sin()(
)( ==+ tytty
dt
tdy
At the end we will shift the solution obtained by 3 time units. The homogeneous solution is obtained from
t
hh
hCetyty
dt
tdy
==+ )(0)(
)(
The particular solution satisfies
)cos()sin()()sin()(
)( tttytty
dt
tdy
pp
p
βα
+==+
Plugging this solution into the differential equation implies 50.
=
α
and 50.
=
β
so that the particular solution is
given by )cos(5.0)sin(5.0)( tttyp=
The system response is given by
)cos(5.0)sin(5.0)()()( ttCetytyty t
ph +=+=
Its initial condition produces
t
hph etyCCyyy
===+== 5.0)(5.05.0)0()0(0)0(
Hence, the system response due to )sin(t is
)cos(5.0)sin(5.05.0)()()( ttetytyty t
ph +=+=
The system response due to )3sin( t , by the time invariance, is given by
)3())3cos(5.0)3sin(5.05.0()()()( )3( +=+= tuttetytyty t
ph
The system zero-state response satisfies
0,0)0(),3sin()(
)( ==+ tytty
dt
tdy
zszs
zs
Using the previously obtained result, the zero-state response is given by
)3())3cos(5.0)3sin(5.05.0()( )3( += tuttety t
zs
The zero-input response satisfies
0,0)0(,0)(
)( ==+ tyty
dt
tdy
zizi
zi
The zero-input response is given by
00)( == tCety t
zi
The system response in terms of its zero-state and zero-input components, is given by
)3())3cos(5.0)3sin(5.05.0()()()( )3( +=+= tuttetytyty t
zizs
The steady state response is practically obtained for large values of time, that is )3cos(5.0)3sin(5.0)(),()(
= tttylargetfortyty ssss
According to the textbook definition of the transient response, we have
smalltfortyt
tr
y),()( =
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Sample Exam 2: Solutions

#1) We use the time invariance principle and first find the solution to

() sin(), ( 0 ) 0 , 0

  • yt = t y = tdt

dyt

At the end we will shift the solution obtained by 3 time units. The homogeneous solution is obtained from

t h h

h y t y t Ce dt

dy t

  • ()= 0 ⇒ ()=

The particular solution satisfies

() sin() () sin() cos()

y t t y t t t dt

dy t

p p

p

Plugging this solution into the differential equation implies α = 0. 5 and β =− 0. 5 so that the particular solution is

given by

y (^) p ( t )= 0. 5 sin( t )− 0. 5 cos( t )

The system response is given by

y ( t ) y ( t ) y ( t ) Ce 0. 5 sin( t ) 0. 5 cos( t )

t = (^) h + p = + −

Its initial condition produces

t y yh yp C C yht e

− ( 0 )= 0 = ( 0 )+ ( 0 )= − 0. 5 ⇒ = 0. 5 ⇒ ()= 0. 5

Hence, the system response due to sin( t )is

y ( t ) y ( t ) y ( t ) 0. 5 e 0. 5 sin( t ) 0. 5 cos( t )

t = (^) h + p = + −

The system response due to sin( t − 3 ), by the time invariance, is given by

( ) () () ( 0. 5 0. 5 sin( 3 ) 0. 5 cos( 3 )) ( 3 )

( 3 ) = + = + − − − −

− − y t y t y t e t t ut

t h p

The system zero-state response satisfies

() sin( 3 ), ( 0 ) 0 , 0

  • y t = ty = tdt

dy t

zs zs

zs

Using the previously obtained result, the zero-state response is given by

( ) ( 0. 5 0. 5 sin( 3 ) 0. 5 cos( 3 )) ( 3 )

( 3 ) = + − − − −

− − y t e t t ut

t zs

The zero-input response satisfies

  • y t = y = tdt

dy t

zi zi

zi

The zero-input response is given by

y t Ce t

t zi

The system response in terms of its zero-state and zero-input components, is given by

( ) () () ( 0. 5 0. 5 sin( 3 ) 0. 5 cos( 3 )) ( 3 )

( 3 ) = + = + − − − −

− − y t y t y t e t t ut

t zs zi

The steady state response is practically obtained for large values of time, that is

y (^) ss ( t )= y ( t ), for t largeyss ( t )≈ 0. 5 sin( t − 3 )− 0. 5 cos( t − 3 )

According to the textbook definition of the transient response, we have

y (^) tr ( t )= y ( t ), for t small

Using the electrical circuit definition of the transient response we have

( ) 0. 5 (sin( 3 ) 0. 5 cos( 3 )) ( 3 ), () () () 0. 5 ( 3 )

( 3 ) = − − − − ⇒ = − = −

− − y t t t ut y t yt y t e ut

t ss tr ss

#2a)

(i) ( 1 ) ( 1 ) ( 1 1 ) ( 1 ) 0 ( 1 ) 0

2

t − δ t − = − δ t − = δ t − =

(ii) cos( ) ( 1 ) ( 1 ) {cos( )} ( 1 ) sin( ) 0

3 3 3 1

3 ( 3 ) 3 − = − = − = =

+∞

−∞

π δ π π π t

t dt

d t t dt

(iii) The delta impulse signal is located at t = 2 / 3 (within integration limits), hence

sin( 3

{sin( )} 3

sin( ) ( 3 2 ) 2 / 3

2

− = = =

−∞

π π δ π t

t t dt t

(iv) The delta impulse signal is located exactly at the upper integration bound (need a factor of 0.5)

sin( 9 ) 2

1 sin( 3 ) 2

1 sin( 3 ) ( 3 )

15 3

5

3 5 − =

−∞

− − = =

e t t dt e t t e

t t δ

(v) The delta impulse signal is outside of integration limits (at t =− 5 ), hence

4

3

4

3

( 1 )

  • = =

− −

f t δ t dt dt

#2b)

0 , otherwise

0 , otherwise

4 (^25 ) = 2 −

− = p t

t t p t

0 , otherwise

0 , otherwise

− + = u t

t t u t

The direct method for finding the generalized derivative

= p 2 t − − ut + + rt − = t − − t − − − t − + utDt

D

Dt

Dxt δ δ δ

#3a) This is an odd signal so that a n = 0 , n = 0 , 1 , 2 ,.... The coefficient bn is obtained from (using the

formula for integration given on the exam sheet)

π

ω π π n

t n tdt t ntdt t ntdt T

E

T

b

T n

T

n

1 / (^21)

0

1 / 2

1 / 2

0

/ 2

/ 2

sin( ) 2 2 sin( 2 ) 8 sin( 2 )

− −

The Fourier series are given by

sin( 2 )

() sin( )

1

1

0 1

nt n

xt b n t

n

n

n

n^ π

∑ ω^ ∑

=

∞ +

=

#3b)

tan ( ) 2

, arg{ ( )}

1

( )arg{ ( )}, ( ) 1

( )

1

2

ω

π ω

ω

ω ω ω ω ω

ω ω

− = −

= =

= H j H j H j H j j

j H j