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Transcript of SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar...
![Page 1: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/1.jpg)
SEE 1023Circuit Theory
Chapter 4 Second Order Circuit
(11th & 12th week)
Prepared by : jaafar shafie
![Page 2: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/2.jpg)
• In first order circuit, the RC and RL circuits are represented in first order differential equation.
• This is due to the existence of only one storage element at any particular circuit.
• In this chapter, two storage elements will exist in a particular circuit.
• Thus, this circuit are characterized by second order differential equation.
• A circuit with second order differential equation is called SECOND ORDER CIRCUIT.
Second Order Circuit
![Page 3: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/3.jpg)
• Types of second order circuit that may exist:-
1. Series RLC circuit,
2. Parallel RLC circuit,
3. RLL circuit,
4. RCC circuit.
Second Order Circuit
V
R L
C I R LC
VR2
L2L1
R1L1
C2
R2C1I
![Page 4: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/4.jpg)
• As usual, the circuit will be analyzed in two parts:-
1. Source–free Circuit (natural response) Energy is initially stored in the element – thus no effect of current or voltage sources.
2. Circuit with source (forced response) Current or voltage sources is directly connected to the first order circuits.
• Before the circuits are being analyzed, one should find the initial and steady state value of the capacitor voltage and inductor current and it’s derivative; i.e.:-
v(0), i(0), dv(0)/dt, di(0)/dt, v(), i().
Second Order Circuit
![Page 5: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/5.jpg)
• Consider the circuit shown below where the switch has been closed for a long time. Find:-
1. v(0+), i(0+),
2. dv(0+)/dt, di(0+)/dt,
3. v(), i().
Second Order Circuit
24V
4Ω
0.4F
t=0s
4Ω
1H
+v(t)
—
i(t)
![Page 6: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/6.jpg)
Second Order Circuit1. When t=0+s=0–s, the inductor is shorted and the capacitor
is opened. The equivalent circuit is shown below,
2. When the switch is opened, the equivalent circuit is
thus,
24V4Ω
4Ω+
v(0+)-
i(0+)
v(0+)=(4/8)24=12V
i(0+)= iC (0+) =3Ai(0+)
24V4Ω 1H
0.4F
i(0+)= 24/8 =3A
and it is know that
dt
dvCi
)0()0(
V/s5.74.0
3)0()0(
C
i
dt
dv
![Page 7: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/7.jpg)
Second Order CircuitApplying KVL to the circuit when switch is opened,
thus,
i(0+)
24V4Ω 1H
0.4F
0L )0()0()0(424 vvi
dt
div
)0()0(
LL
0L 12)0(3424 v
0L )0(v
0L
L )0()0( v
dt
di
![Page 8: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/8.jpg)
Second Order Circuit3. The steady state value,
0)(i
i()
24V4Ω +
v()-
24V)(v
![Page 9: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/9.jpg)
Natural Response - Series RLC Circuit• Natural response is obtained with Series RLC circuit
without source.
• Energy is initially stored in the L and C, where the initial voltage at capacitor is VO and initial current at inductor is IO.
• Applying KVL to the loop,
IO
R L
C+VO
-
01
tidt
dt
dii
CLR
![Page 10: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/10.jpg)
Natural Response - Series RLC Circuit• To eliminate the integral, differentiate with respect to
t and rearrange the terms such that
• Now, we have second order differential equation.• It is known that in first-order differential equation,
the current is
where A and s are constants.• Substitute Aest to the second order equation.
02
2
LCL
R i
dt
di
dt
id
steAi(t)
![Page 11: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/11.jpg)
Natural Response - Series RLC Circuit• Thus, we may write as
or
• And we should find the value of A, thus Aest must not equal to zero. The only part that should equal to zero is
0LC
As
L
ARAs2
ststst e
ee
01
LCs
L
RsA 2ste
01
LC
sL
Rs2
known as CHARACTERISTIC
EQUATION
![Page 12: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/12.jpg)
Natural Response - Series RLC Circuit• Solve the characteristic equation, one might find the
two roots, which are
and
LC2L
R
2L
Rs1
12
LC2L
R
2L
Rs2
12
![Page 13: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/13.jpg)
Natural Response - Series RLC Circuit• On the other hand, we may represent the two roots
as
and
where
• The two solutions for s (i.e. s1 and s2) shows that there are two values of the current, which are
and• The total response of the current would be
22O 1s
LC2L
R 1, O
22O 2s
tsei 11 1A tsei 2
2 2A
tsts eeiii(t) 2121 21 AA
![Page 14: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/14.jpg)
• Thus, we may found three type of response which are
1. 1st Type : > ω0 ,
the response is called OVERDAMPED
2. 2nd Type : = ω0 ,
the response is called CRITICALLY DAMPED
3. 3rd Type : < ω0 ,
the response is called UNDERDAMPED
Natural Response - Series RLC Circuit
![Page 15: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/15.jpg)
• 1st Type : > ω0 , OVERDAMPED
• In this type, > ω0, or C > 4L/R2. It is found that both roots, (i.e. s1 and s2) are negative and real. Thus, the current response is
which decays to zero when t increased.
• A1 and A2 are determined from the initial inductor current and the rate of change of current.
Natural Response - Series RLC Circuit
tsts eeiii(t) 2121 21 AA
21 AA(0) i
2211L sAsA
(0)
L
dt
div )0(Solve forA1 and A2
![Page 16: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/16.jpg)
Natural Response - Series RLC Circuit• For example
• A series RLC circuit has R=20Ω, L=1mH and C=100F. If i(0+)=1A and vC(0+)=18V, find the current response.
*It is clear that C > 4L/R2, and the response is the 1st type which is ‘overdamped’.
Step1: Find the value of s1 and s2
srad /167.5131
2
LC2L
R
2L
Rs1
sradk /487.191
2
LC2L
R
2L
Rs2
![Page 17: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/17.jpg)
Natural Response - Series RLC CircuitStep2: Find the value of A1 and A2 from the initial
values.
apply KVL to the loop
thus,
21 AA(0) 1i
0L )0()0()0(20 vvi
0L 18)0(20 v
Vv 2)0( L
2211/21
)0()0(sAsAsAk
m
v
dt
di
2
LL
![Page 18: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/18.jpg)
Natural Response - Series RLC CircuitStep3:
It is found that,
A1 = 0.9216, A2 = 78.36m
Aeei(t) tt 8.1948617.513 78.36m0.9216
-2ms 0ms 2ms 4ms 6ms 8ms 10ms 12ms 14ms 16ms 18msI(L1)
0A
0.5A
1.0A
![Page 19: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/19.jpg)
• 2nd Type : = ω0 , CRITICALLY DAMPED
• In this type, = ω0, or C = 4L/R2. It is found that both roots, (i.e. s1 and s2) are equal to – or –R/2L. Thus, the current response is
• It can be seen that solution for A3 could not be obtained with two initial condition [i(0) & di(0)/dt)].
• Thus, there might be another method to find the response of critically damped.
Natural Response - Series RLC Circuit
tttt eeeei(t) 32121 AAAAA )(
![Page 20: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/20.jpg)
• In this type, = ω0 = R/2L = 1/LC. Thus, the second order differential equation become
• Let , thus
• In first order differential equation, it is found that
, thus
, or ,or
Natural Response - Series RLC Circuit
02 22
2
idt
di
dt
id 0
i
dt
dii
dt
di
dt
d
idt
dif 0 ff
dt
d
tef 1A
teidt
di 1A 1A iedt
die tt 1Aie
dt
d t
![Page 21: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/21.jpg)
• By integrating the equation, one will found the response of critically damped response as
• Thus, the derivative of the current is,
when t=0s,
Natural Response - Series RLC Circuit
tetti 21 AA)(
tt etetdt
tdi 21 AA 1)(
21 AA dt
di )0(
![Page 22: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/22.jpg)
Natural Response - Series RLC Circuit• For example
• A series RLC circuit has R=20Ω, L=1mH and C=10F. If i(0+)=1A and vC(0+)=18V, find the current response.
*It is clear that C = 4L/R2, and the response is the 2nd type which is ‘critically damped’.
Step1: Find the value of s1 and s2
sradk /101
2
LC2L
R
2L
Rs1
sradk /101
2
LC2L
R
2L
Rs2
![Page 23: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/23.jpg)
Natural Response - Series RLC CircuitStep2: Find the value of A1 and A2 from the initial
values.
apply KVL to the loop
thus,
2A(0) 1i
0L )0()0()0(20 vvi
0L 18)0(20 v
Vv 2)0( L
2121
)0()0(AAk
m
v
dt
di
2
LL
![Page 24: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/24.jpg)
Natural Response - Series RLC CircuitStep3:
It is found that,
A1 = 8k, A2 = 1
tetti 10000)( 18000
Time
-0.5ms 0ms 0.5ms 1.0ms 1.5ms 2.0msI(L1)
0A
0.5A
1.0A
![Page 25: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/25.jpg)
• 3rd Type : < ω0 , UNDERDAMPED
• In this type, < ω0, or C < 4L/R2.
• The roots can be written as
where
and
• The response can be further written as
Natural Response - Series RLC Circuit
dO j )( 221s
dO j )( 222s
1j 22 Od
tjtj dd eei(t) )()( 21 AA
![Page 26: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/26.jpg)
Natural Response - Series RLC Circuit• Rearranging the response such that,
• Applying Euler’s identities to the above equation, where
• Thus,
• Let B1=A1+A2 and B2=j(A1–A2), thus
tjtjt dd eeei(t) 21 AA
sincos,sincos jeje jj and
tjtei(t) ddt sincos 2121 AAAA
ttei(t) ddt sincos 21 BB
![Page 27: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/27.jpg)
Natural Response - Series RLC Circuit• Differentiate the i(t), we have
)(sincos
)(cossin)(
tddd
t
tddd
t
ette
ettedt
tdi
2
1
B
B
![Page 28: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/28.jpg)
Natural Response - Series RLC Circuit• For example
• A series RLC circuit has R=20Ω, L=1mH and C=2F. If i(0+)=1A and vC(0+)=18V, find the current response.
*It is clear that C < 4L/R2, and the response is the 3rd type which is ‘underdamped’.
Step1: Find the value of s1 and s2
sradkjk /20101
2
LC2L
R
2L
Rs1
kandk d 2010
![Page 29: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/29.jpg)
Natural Response - Series RLC CircuitStep2: Find the value of A1 and A2 from the initial
values.
apply KVL to the loop
thus,
1B(0) 1i
0L )0()0()0(20 vvi
0L 18)0(20 v
Vv 2)0( L
dsAkm
v
dt
di 21L BB
2
L
/21
)0()0(
![Page 30: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/30.jpg)
Natural Response - Series RLC CircuitStep3:
It is found that,
B1 = 1, B2 = 0.4,
)20000sin()4.0)20000cos(10000 ttei(t) t (
kandk d 2010
Time
-0.4ms -0.2ms 0ms 0.2ms 0.4ms 0.6ms 0.8ms 1.0msI(L1)
-0.5A
0A
0.5A
1.0A
![Page 31: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/31.jpg)
• In summary, the response for series RCL are
1. 1st Type : > ω0 , (OVERDAMPED)
2. 2nd Type : = ω0 , (CRITICALLY DAMPED)
3. 3rd Type : < ω0 , (UNDERDAMPED)
Natural Response - Series RLC Circuit
tsts eei(t) 2121 AA
tetti 21 AA)(
ttei(t) ddt sincos 21 BB
![Page 32: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/32.jpg)
Natural Response - Series RLC Circuit• The comparison of the three responses are
shown below
Time
0s 0.5ms 1.0ms 1.5ms 2.0ms 2.5ms 3.0ms 3.5ms 4.0ms 4.5ms 5.0msI(L1)
-0.5A
0A
0.5A
1.0A
C=2F
C=10FC=100F
![Page 33: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/33.jpg)
• Natural response for Series RLC circuit is obtained without any connection to source.
• Applying KCL, thus we have
• Differentiate with t,
Natural Response - Parallel RLC Circuit
01
dt
dvvdt
v tC
LR
IOR L C+VO
-
+v-
02
2
vdt
dv
dt
vd
LC
1
RC
1
![Page 34: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/34.jpg)
• Replace the first derivative as s and the second derivative as s2. Thus, the characteristic equation is obtained as follows,
• The roots are characterized by these equations
Natural Response - Parallel RLC Circuit
02 LC
1
RC
1ss
LC2RC
1
2RC
1s1
12
LC2RC
1
2RC
1s2
12
![Page 35: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/35.jpg)
Natural Response - Parallel RLC Circuit• On the other hand, we may represent the two roots
as
and
where
22O 1s
LC2RC
1 1, O
22O 2s
![Page 36: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/36.jpg)
• 1st Type : > ω0 , OVERDAMPED
• In this type, > ω0, or L > 4R2C. The roots, (i.e. s1 and s2) are negative and real. Thus, the voltage response is
• A1 and A2 are determined from the initial inductor current and the rate of change of current.
Natural Response - Parallel RLC Circuit
tsts eev(t) 2121 AA
21 AA(0) v
2211 sAsA(0)
RC
R
dt
dviv L )0()0( Solve forA1 and A2
![Page 37: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/37.jpg)
Natural Response - Parallel RLC Circuit• For example
• A parallel RLC circuit has R=20Ω, L=10mH and C=1F. If iL(0+)=0.5A and v(0+)=10V, find the current response.
Step1: Find the value of and ω0
*It is clear that > ωO , and the response is the 1st type which is ‘overdamped’.
1000011
25000)1)(20(2
1
)(10m)(1LC
2RC
1
O
![Page 38: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/38.jpg)
Natural Response - Parallel RLC Circuit• Find s1 and s2.
• The initial condition are
kkkkO 087.2)10()25(25 2222 1s
kkkkO 9.47)10()25(25 2222 2s
10 21 AA(0)v
)(A)(AsAsA(0)
)(
)(
RC
R(0)
212211 kkdt
dv
kiv
dt
dv L
9.47087.2
1000)1(20
)5.0(2010)0()0(
![Page 39: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/39.jpg)
Natural Response - Parallel RLC CircuitStep3:
It is found that,
A1 = -18.09, A2 = 28.09
Veev(t) tktk 9.47087.2 21.36711.367-
Time
0s 0.2ms 0.4ms 0.6ms 0.8ms 1.0ms 1.2ms 1.4ms 1.6ms 1.8ms 2.0msV(R5:2)
-10V
-5V
0V
5V
10V
![Page 40: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/40.jpg)
• 2nd Type : = ω0 , CRITICALLY DAMPED
• In this type, = ω0, or L = 4R2C. From the series RLC circuit, the response found in parallel RLC circuit is
• The derivative is represented as
and at t=0s,
Natural Response - Parallel RLC Circuit
tettv 21 AA)(
tt etetdt
tdv 21 AA 1)(
21 AA dt
dv )0(
![Page 41: SEE 1023 Circuit Theory Chapter 4 Second Order Circuit (11 th & 12 th week) Prepared by : jaafar shafie.](https://reader036.fdocuments.us/reader036/viewer/2022062423/56649ee95503460f94bfa7d6/html5/thumbnails/41.jpg)
Natural Response - Parallel RLC Circuit• For example
• A parallel RLC circuit has R=50Ω, L=10mH and C=1F. If iL(0+)=0.5A and v(0+)=10V, find the current response.
Step1: Find the value of and ω0
*It is clear that = ωO , and the response is the 2nd type which is ‘critically damped’.
1000011
10000)1)(50(2
1
)(10m)(1LC
2RC
1
O
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Natural Response - Parallel RLC CircuitStep2: Find the value of A1 and A2 from the initial
values.
apply KCL to the loop
2A(0) 10v
)0(AAAA(0)
)(
)(
RC
R(0)
2121 kdt
dv
kiv
dt
dv L
1
700)1(50
)5.0(5010)0()0(
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Natural Response - Parallel RLC CircuitStep3:
It is found that,
A1 = -600k, A2 = 10
tettv 10000)( 10600k-
Time
0s 0.1ms 0.2ms 0.3ms 0.4ms 0.5ms 0.6ms 0.7ms 0.8ms 0.9ms 1.0msV(R5:2)
-20V
-10V
0V
10V
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• 3rd Type : < ω0 , UNDERDAMPED
• In this type, < ω0, or L < 4R2C.
• The roots can be written as
where
and
• The response can be further written as
Natural Response - Parallel RLC Circuit
dO j )( 221s
dO j )( 222s
1j 22 Od
tjtj dd eev(t) )()( 21 AA
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Natural Response - Parallel RLC Circuit• Applying the same method as in series, the
response of the parallel is
• Let B1=A1+A2 and B2=j(A1–A2), thus
tjtev(t) ddt sincos 2121 AAAA
ttev(t) ddt sincos 21 BB
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Natural Response - Parallel RLC Circuit• Differentiate the v(t), we have
)(sincos
)(cossin)(
tddd
t
tddd
t
ette
ettedt
tdv
2
1
B
B
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Natural Response - Parallel RLC Circuit• For example
• A parallel RLC circuit has R=80Ω, L=10mH and C=1F. If iL(0+)=0.5A and v(0+)=10V, find the current response.
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• In summary, the responses for parallel RCL are
1. 1st Type : > ω0 , (OVERDAMPED)
2. 2nd Type : = ω0 , (CRITICALLY DAMPED)
3. 3rd Type : < ω0 , (UNDERDAMPED)
Natural Response - Parallel RLC Circuit
tsts eev(t) 2121 AA
tettv 21 AA)(
ttev(t) ddt sincos 21 BB
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• Step response is obtained in Series RLC circuit with source.
• Applying KVL to the loop,
,where
• Substitute i to the derivative terms,
Step Response - Series RLC Circuit
SVLR vdt
dii
i
R L
C+v-
CVS
dt
dvi C
LCLCL
R SVv
dt
dv
dt
vd
2
2 2nd order diff. equ for capacitor
voltage
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Step Response - Series RLC Circuit• To obtain the total response, consider the KVL of
the loop
• Differentiate the equation, we get
• It can be seen that the characteristic equation is the same with source-free series RLC.
• Thus, by looking at the roots of the characteristic equation, one may find the type of the response (either overdamped, critically damped or underdamped).
0C
LR i
dt
id
dt
di2
2
SVC
LR
tidt
dt
dii
1
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Step Response - Series RLC Circuit• Furthermore, it can be concluded that the total
response can be represented in terms of ‘transient’ and ‘steady-state’ value,
where vt(t) is the ‘transient response’ and vss(t) is the ‘steady-state’ response.
• The vt(t) is the part which will determine the type of the response, and it reflects to the response for source-free series RLC circuit.
)()()( tvtvtv SSt
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Step Response - Series RLC Circuit• The transient responses are:
• While vss(t) is the final voltage value (i.e. when t=) across the capacitor. Normally, it will equal to Vs.
tstst ee(t)v 21
21 AA
tt ettv 21 AA)(
tte(t)v ddt
t sincos 21 BB
overdamped
critically damped
underdamped
SV )(v(t)vSS
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Step Response - Series RLC Circuit• Thus, the complete responses for series RLC with
source are:
1. 1st Type : > ω0 , (OVERDAMPED)
2. 2nd Type : = ω0 , (CRITICALLY DAMPED)
3. 3rd Type : < ω0 , (UNDERDAMPED)
tsts eev(t) 2121S AAV
tettv 21S AAV)(
tdd ettv(t) sincos 21S BBV
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Step Response - Series RLC CircuitExample• A series RLC circuit is shown below. If i(0+)=1A and
vC(0+)=18V, find i(t) and v(t).
Step 1: Find and ω0. Determine type of response.
It is found that > ω0, type of response overdamped.
i(t)
20Ω 1mH
100F+
v(t)-
20V
sradk /102L
R sradk /162.30 LC
1
sradk /487.19,167.51320
2 1,2s
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Step Response - Series RLC CircuitStep 3: The steady state voltage across capacitor is
Step2: Find the value of A1 and A2 from the initial values.
the derivative of the response at initial is
thus,
2AA
AA2018(0)
21
21
v
2211/10100
1)0()0(sAsAsVk
i
dt
dv
C
0.473A1.527,A 21
Vv(t)vSS 20)( SV
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Step Response - Series RLC CircuitStep3:
It is found that the complete response is
• Next, find the voltage response if R is changed to 6.324Ω and then to 2Ω
Veev(t) tt 8.1948617.513 0.4731.52720
Aee
dt
tdvCi(t)
tt 8.1948617.513
)(
921.68m78.361m
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Step Response - Series RLC Circuit• Comparison of the three responses with different R
value.
Time
0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10msV(L2:2)
18V
19V
20V
21V
22V
20Ω
2Ω
6.324Ω
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• Step response is obtained in Parallel RLC circuit with source.
• Applying KCL to the loop,
,where
• Substitute i to the derivative terms,
Step Response - Parallel RLC Circuit
SCR
I idt
dvvdt
div L
LCLCRC
1 SIi
dt
di
dt
id
2
2 2nd order diff. equ for capacitor
voltage
i
R L+v-
CIS
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Step Response - Parallel RLC Circuit• It has the same characteristic equation to that of
natural response of parallel/series RLC.• Furthermore, it can also be concluded that the total
response can be represented in terms of ‘transient’ and ‘steady-state’ value,
where it(t) is the ‘transient response’ and iss(t) is the ‘steady-state’ response.
• The it(t) is the part which will determine the type of the response, and it reflects to the response for source-free parallel RLC circuit.
)()()( tititi SSt
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Step Response - Parallel RLC Circuit• The transient responses are:
• While iss(t) is the final voltage value (i.e. when t=) across the capacitor. Normally, it will equal to Is.
tstst ee(t)i 21
21 AA
tt etti 21 AA)(
tte(t)i ddt
t sincos 21 BB
overdamped
critically damped
underdamped
SI)( i(t)iSS
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Step Response - Parallel RLC Circuit• Thus, the complete responses for parallel RLC with
source are:
1. 1st Type : > ω0 , (OVERDAMPED)
2. 2nd Type : = ω0 , (CRITICALLY DAMPED)
3. 3rd Type : < ω0 , (UNDERDAMPED)
tsts eei(t) 21I 21S AA
tetti 21S AAI)(
tdd etti(t) sincosI 21S BB
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General Second-Order Circuit• Previously, only the second-order series and
parallel circuits are considered.• If the circuits were neither in series nor in parallel,
what method should be used?• In this topic, we would concentrate to find the
response for a second-order circuit which is neither a series nor parallel circuit.
• The response might be in terms of voltage or current. Thus, generally the response are characterized as x(t).
• In general 2nd-order circuit, the most important part is to find the characteristic equation and find the two roots (s1 and s2). From the two roots, one should know the type of the response.
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General Second-Order Circuit• The type of the response are the same with series
and parallel RLC circuit.• Finally, find the initial and steady state value (x(0),
dx(0)/dt and x()) to determine the constant value; i.e. A1 and A2.
• Generally, the response is the summation of the ‘transient’ and ‘steady-state’ value and can be expressed as
where x is either in voltage or current.
)()()( txtxtx SSt
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General 2nd-Order Circuit – step by step
Turn off the independent source to find the secondorder differential equation using KCL and/or KVL.
Find the roots and determine the type of the response (i.e. O-D, C-D or U-D)
The 2nd order differential equation would determine whether the response is voltage or current!
Find the steady-state and initial valueto determine A1 and A2.
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General Second-Order Circuit - eg• Consider a circuit shown below. Find the complete
response of the voltage v(t)?
Step 1: Turn off the independent source. Find the second order differential equation.
i
4Ω 1H
+v(t)-
0.5F12V2Ω
t >0s
using KCL and KVL to find the 2nd order
differential equations,i
4Ω 1H
+v(t)-
0.5F2Ω
v
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General Second-Order Circuit - egKCL at node ‘v’ KVL at mesh ‘i’
We just concern on ‘v’. Thus, substitute ‘i’ to the right hand side equation
dt
dvvdt
dvvi
iii CR
2
1
4
CR
01
0
vdt
dii
vdt
dii
)(4
LR
02
2
vdt
dv
dt
vd65
Thus, the characteristic equation is,
02 65ss
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General Second-Order Circuit - egStep 2: The two roots are s1 = -2, and s2 = -3
*It is obvious that the two roots are negative and real. Thus, the transient response is the 1st type (OVERDAMPED)
Step 3: The standard response is
The steady state voltage is
The transient voltage is
ttt ee(t)v 32 21 AA
)()()( tvtvtv SSt
VvtvSS 4)0()(
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General Second-Order Circuit - egStep 4: The initial voltage and current is,
At just after the switch is closed, the circuit is shown as
Vvv 12)0()0(
sVdt
dv
dt
dvvi
iii CR
/12)0(
)0()0()0(
)0()0()0(
2
1
2
iC
i
iR
4Ω 1H
+v(t)-
0.5F12V 2Ω
Aii 0)0()0(
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General Second-Order Circuit - egThe overall response is
From the overall response, at initial
It is found that A1 = 12 and A2 = -4.
Thus,
123A2A 21
dt
dv )0(
12AA4 21 )0(v
tt eev(t) 32 21 AA4
tt eev(t) 32 4124