ece2031 tutorial 1 solutions
TRANSCRIPT
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ECE2031 Tutorial 1 Solutions
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0),( ttvO
FIND
C
1R
2R
KCLUSE0.tFORMODEL
0)()(0)( 2121
c
CCC vtdt
dvCRR
RR
vt
dt
dvC
sFCRR 6.0)10100)(106()(63
21
STEP 1
)(31)(
422)( tvtvtv CCO
STEP 20,)( 21
teKKtv
t
C 01K
INITIAL CONDITIONS. CIRCUIT IN STEADY STATE t
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0),( ttvO
FIND
0,)( 21
teKKtv
t
o:1STEP
VOLTAGECAPACITORINITIAL:2STEP
)0(Cv
0t
1v
2v
2
12
12)0(
)12(3
1
vv
vv
C
V12
022
8
3
12: 1111
vvvv@KCL 6/*
][60488 11 Vvv
][10)0()0(][22 VvvVv CC
)0( OvDETERMINE:3STEP
0t
)0(Ov
V10
][5)10(22
2)0( VvO
Tute 1 Problem 2
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)(OvDETERMINE:4STEP
)(Ov
][524)12(
52)( Vv
O
CONSTANTTIMEDETERMINE:5STEP
CRTH
:CircuitCapacitive
THR
5
44||1
THR
sFC5
82
21,KKDETERMINE:6STEP
][5
24)(1 VvK O
][5
1][5)0(
221
VKKKVvO
0];[5
1
5
24)( 5
8
tVetv
t
O:ANS
ORIGINAL CIRCUIT
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Tute 1 Problem 3
vs(t)
0 1 2 3 4 5
-1
1
2
t
+
+
R = 2
vc(t)C = 1Fvs(t)
First Approach:
Consider the piecewisecontinuous input waveform shown above. We use the term
piecewise (continuousunderstood) to describe a waveform consisting of continuous
curves jointed together at a finite number of breakpoints. At these breakpoints, thewaveform may or may not be continuous. The waveform shown is a typical piecewise
waveform. A pulse, step, square, and triangular waves (for a finite time interval) can
also be regarded as special cases of piecewise waveforms.
Find the zero-state response vC(t)of the series RC circuit shown below to an
applied voltage vs(t)having the waveform illustrated in the same Figure. Sketch v
c(t)
and note its value at t=0, 4, 5,.
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The peculiarity of the input waveform allows us to solve the problem piece-by-piece,
or from breakpoint to breakpoint. This approach is intuitive, and we shall describe it
by analyzing the above circuit as follows.
First time interval [0,4]
Within this time interval, the problem is obviously that of finding the step response
and the solution is -1 (step response). The circuit is in its zero-state at the beginning
of the interval. The step height is 1, and the natural frequency is1/2. The solution
can be written down by inspection:
At the end of this interval t=4, the capacitor voltage is vc(4)=0.8647.
Tute 1 Problem 3
, 1 2
, 1
, 1 2 2
2
2,
,
( )
( ) 1
(0) 0 1
( ) 1
1
( ) 1
( )
(1 )
t
c ste
t
c ste
p
c step
c step
c
t
p
c step
v t k k e
v k
v k k k
v t
t e
v t
e
v
By linearity property
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Second time interval [4,5]
Within this time interval, the problem is to find the complete response with a step
input. It is expedient to do a time shiftt=(t-4) first. At the beginning of this interval,
the circuit is at a state of vc(t=4)=0.8647, which becomes the initial condition for
this time interval (helping to find the ZIR). The input is 2u(t). The solution can be
written down by inspection:
At the end of this interval t=5 (or t=1), the capacitor voltage is vc(5) = 0.2625.
Third time interval [5, ]
Within this time interval, the problem is to find the zero-input response. It is
expedient to do a time shift t=(t-5) first. At the beginning of this interval, the circuit
is at state vc(t=5) =
vc(t=0) = 0.2625. The solution can be written down byinspection:
The capacitor voltage decays to zero vc() = 0 as expected .
vc(t' ) 2(1 e
t' / 2) 0.8647 e
t' / 2; t' [0,1]
vc
(t") 0.2625e t"/ 2
; t"[0, ]
Tute 1 Problem 3
ZSR ZIR
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0 1 2 3 4 5 6 7 8-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
time t (s)
voltagevc
(t)(V)
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Second Approach:
First we decompose the input waveform in terms of unit step functions as follows.
Immediately we obtain from the LTIV properties of the circuit
Where the step response
and
This completes the derivation. The voltage vC(t) at any time t can be evaluated from
the equations above.
Remark
The step height at the interval [4,5] is 3, while in the First Approach, it was regarded
as 2. Why?
vs(t) u(t)3u(t 4) 2u(t 5)
vc(t) (t)3(t4)2 (t5)
(t)(1et/2)u(t)
-(t- ) /ts(t- ) = (1 - e )u(t- ), = 4,5.
Tute 1 Problem 3
2
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0),( ttiFIND
Once the switch opens the circuit is RLC
series
0)()0()(2)(30
t
C dxxivt
dt
diti
0)(2
1)(
2
3)(
2
2
titdt
dit
dt
id
5.0,1
05.05.12
s
ss
:roots
:Ch.Eq.
0;)( 221
teKeKti
t
t
To find initial conditions use steady state analysis for t
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0),(0 ttvFIND
For t>0 the circuit is RLC series
)(2)(0 titv
)(ti
KVL
0)(2)0()(3/2
1)(
2
1
0
tivdxxitdt
di
C
t
0)(3)(4)(2
2
titdt
dit
dt
id
3,1
0342
s
ss
:roots
:Eq.Ch.
0;)( 321
teKeKti tt
To find initial conditions we use steady
state analysis for t
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0);(),( 00 ttvtiDETERMINE )(12)(18)( 00 Vtitv
KVL
012)(18)(2)0()(36/114
0
titdt
divdxxi
t
C
0)(18)(9)(2
2
titdt
dit
dt
id
6,3
01892
s
ss
:roots
:Eq.Ch.
0;)( 623
10
teKeKti tt
0)0( C
v AiL 5.0)0(
Analysis at t=0+
)(5.0)0()0(0 Aii L
)0()0()0( 0 dt
diL
dt
diLv
L
L )0(Lv
0)0(Cv
012)0(18)0(4 LL iv
210
210
5.0)0(
632/17)0(
KKi
KKdt
di
Steady state t 0
6 6 6
14;
6
1121 KK
Tute 1 Problem 6